Free UPSC Mathematics Optional Paper-1 2019 Solutions: View Online | UPSC Maths Solution | IAS Maths Solution

खण्ड-A / SECTION-A
  1. (a) माना कि f : [ 0 , π 2 ] R f : 0 , π 2 R f:[0,(pi)/(2)]rarrRf:\left[0, \frac{\pi}{2}\right] \rightarrow \mathbb{R}f:[0,π2]R एक संतत फलन है, जैसा कि
f ( x ) = cos 2 x 4 x 2 π 2 , 0 x < π 2 f ( x ) = cos 2 x 4 x 2 π 2 , 0 x < π 2 f(x)=(cos^(2)x)/(4x^(2)-pi^(2)),quad0 <= x < (pi)/(2)f(x)=\frac{\cos ^2 x}{4 x^2-\pi^2}, \quad 0 \leq x<\frac{\pi}{2}f(x)=cos2x4x2π2,0x<π2
f ( π 2 ) f π 2 f((pi)/(2))f\left(\frac{\pi}{2}\right)f(π2) का मान ज्ञात कीजिए।
Let f : [ 0 , π 2 ] R f : 0 , π 2 R f:[0,(pi)/(2)]rarrRf:\left[0, \frac{\pi}{2}\right] \rightarrow \mathbb{R}f:[0,π2]R be a continuous function such that
f ( x ) = cos 2 x 4 x 2 π 2 , 0 x < π 2 f ( x ) = cos 2 x 4 x 2 π 2 , 0 x < π 2 f(x)=(cos^(2)x)/(4x^(2)-pi^(2)),quad0 <= x < (pi)/(2)f(x)=\frac{\cos ^2 x}{4 x^2-\pi^2}, \quad 0 \leq x<\frac{\pi}{2}f(x)=cos2x4x2π2,0x<π2
Find the value of f ( π 2 ) f π 2 f((pi)/(2))f\left(\frac{\pi}{2}\right)f(π2).
Answer:

Introduction

The problem asks us to find the value of f ( π 2 ) f π 2 f((pi)/(2))f\left(\frac{\pi}{2}\right)f(π2) for a given function f ( x ) = cos 2 x 4 x 2 π 2 f ( x ) = cos 2 x 4 x 2 π 2 f(x)=(cos^(2)x)/(4x^(2)-pi^(2))f(x) = \frac{\cos^2 x}{4x^2 – \pi^2}f(x)=cos2x4x2π2 defined on the interval [ 0 , π 2 ] 0 , π 2 [0,(pi)/(2)]\left[0, \frac{\pi}{2}\right][0,π2]. The function is continuous except at x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2 because the denominator becomes zero at that point. To find f ( π 2 ) f π 2 f((pi)/(2))f\left(\frac{\pi}{2}\right)f(π2), we’ll need to evaluate the limit of f ( x ) f ( x ) f(x)f(x)f(x) as x x xxx approaches π 2 π 2 (pi)/(2)\frac{\pi}{2}π2.

Work/Calculations

Step 1: Define the Function and the Limit

The function f ( x ) f ( x ) f(x)f(x)f(x) is given as:
f ( x ) = cos 2 x 4 x 2 π 2 f ( x ) = cos 2 x 4 x 2 π 2 f(x)=(cos^(2)x)/(4x^(2)-pi^(2))f(x) = \frac{\cos^2 x}{4x^2 – \pi^2}f(x)=cos2x4x2π2
We need to find:
f ( π 2 ) = lim x π 2 f ( x ) f π 2 = lim x π 2 f ( x ) f((pi)/(2))=lim_(x rarr(pi)/(2))f(x)f\left(\frac{\pi}{2}\right) = \lim_{{x \to \frac{\pi}{2}}} f(x)f(π2)=limxπ2f(x)

Step 2: Simplify the Function

To find the limit, we can use L’Hôpital’s Rule, which states that if lim x a f ( x ) g ( x ) lim x a f ( x ) g ( x ) lim_(x rarr a)(f(x))/(g(x))\lim_{{x \to a}} \frac{f(x)}{g(x)}limxaf(x)g(x) is an indeterminate form 0 0 0 0 (0)/(0)\frac{0}{0}00 or (oo )/(oo)\frac{\infty}{\infty}, then:
lim x a f ( x ) g ( x ) = lim x a f ( x ) g ( x ) lim x a f ( x ) g ( x ) = lim x a f ( x ) g ( x ) lim_(x rarr a)(f(x))/(g(x))=lim_(x rarr a)(f^(‘)(x))/(g^(‘)(x))\lim_{{x \to a}} \frac{f(x)}{g(x)} = \lim_{{x \to a}} \frac{f'(x)}{g'(x)}limxaf(x)g(x)=limxaf(x)g(x)
provided the limits on the right-hand side exist.
First, let’s check if the function f ( x ) f ( x ) f(x)f(x)f(x) is in indeterminate form at x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2:
Numerator at x = π 2 : cos 2 ( π 2 ) = 0 Numerator at x = π 2 : cos 2 π 2 = 0 “Numerator at “x=(pi)/(2):cos^(2)((pi)/(2))=0\text{Numerator at } x = \frac{\pi}{2}: \cos^2 \left(\frac{\pi}{2}\right) = 0Numerator at x=π2:cos2(π2)=0
Denominator at x = π 2 : 4 ( π 2 ) 2 π 2 = 0 Denominator at x = π 2 : 4 π 2 2 π 2 = 0 “Denominator at “x=(pi)/(2):4((pi)/(2))^(2)-pi^(2)=0\text{Denominator at } x = \frac{\pi}{2}: 4 \left(\frac{\pi}{2}\right)^2 – \pi^2 = 0Denominator at x=π2:4(π2)2π2=0
Both the numerator and the denominator are zero, so we have an indeterminate form 0 0 0 0 (0)/(0)\frac{0}{0}00.

Step 3: Apply L’Hôpital’s Rule

Let’s differentiate the numerator and the denominator with respect to x x xxx.
  • f ( x ) f ( x ) f^(‘)(x)f'(x)f(x) (Derivative of cos 2 x cos 2 x cos^(2)x\cos^2 xcos2x) = 2 cos ( x ) sin ( x ) 2 cos ( x ) sin ( x ) -2cos(x)sin(x)-2 \cos(x) \sin(x)2cos(x)sin(x)
  • g ( x ) g ( x ) g^(‘)(x)g'(x)g(x) (Derivative of 4 x 2 π 2 4 x 2 π 2 4x^(2)-pi^(2)4x^2 – \pi^24x2π2) = 8 x 8 x 8x8x8x
Now, we can find the limit:
lim x π 2 f ( x ) g ( x ) = lim x π 2 2 cos ( x ) sin ( x ) 8 x lim x π 2 f ( x ) g ( x ) = lim x π 2 2 cos ( x ) sin ( x ) 8 x lim_(x rarr(pi)/(2))(f^(‘)(x))/(g^(‘)(x))=lim_(x rarr(pi)/(2))(-2cos(x)sin(x))/(8x)\lim_{{x \to \frac{\pi}{2}}} \frac{f'(x)}{g'(x)} = \lim_{{x \to \frac{\pi}{2}}} \frac{-2 \cos(x) \sin(x)}{8x}limxπ2f(x)g(x)=limxπ22cos(x)sin(x)8x
Let’s substitute the values into the formula and calculate the limit.
After substituting the values, we get:
lim x π 2 2 cos ( x ) sin ( x ) 8 x = 2 cos ( π 2 ) sin ( π 2 ) 8 × π 2 lim x π 2 2 cos ( x ) sin ( x ) 8 x = 2 cos π 2 sin π 2 8 × π 2 lim_(x rarr(pi)/(2))(-2cos(x)sin(x))/(8x)=(-2cos((pi)/(2))sin((pi)/(2)))/(8xx(pi)/(2))\lim_{{x \to \frac{\pi}{2}}} \frac{-2 \cos(x) \sin(x)}{8x} = \frac{-2 \cos\left(\frac{\pi}{2}\right) \sin\left(\frac{\pi}{2}\right)}{8 \times \frac{\pi}{2}}limxπ22cos(x)sin(x)8x=2cos(π2)sin(π2)8×π2
After calculating, we get:
lim x π 2 2 cos ( x ) sin ( x ) 8 x = 0 lim x π 2 2 cos ( x ) sin ( x ) 8 x = 0 lim_(x rarr(pi)/(2))(-2cos(x)sin(x))/(8x)=0\lim_{{x \to \frac{\pi}{2}}} \frac{-2 \cos(x) \sin(x)}{8x} = 0limxπ22cos(x)sin(x)8x=0

Conclusion

The value of f ( π 2 ) f π 2 f((pi)/(2))f\left(\frac{\pi}{2}\right)f(π2) is 0 0 000. We used L’Hôpital’s Rule to evaluate the limit of the function f ( x ) f ( x ) f(x)f(x)f(x) as x x xxx approaches π 2 π 2 (pi)/(2)\frac{\pi}{2}π2, and found that the limit is 0 0 000. Therefore, f ( π 2 ) = 0 f π 2 = 0 f((pi)/(2))=0f\left(\frac{\pi}{2}\right) = 0f(π2)=0.
(b) माना कि f : D ( R 2 ) R f : D R 2 R f:D(subeR^(2))rarrRf: D\left(\subseteq \mathbb{R}^2\right) \rightarrow \mathbb{R}f:D(R2)R एक फलन है और ( a , b ) D ( a , b ) D (a,b)in D(a, b) \in D(a,b)D. अगर f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) बिंदु ( a , b ) ( a , b ) (a,b)(a, b)(a,b) पर संतत है, तो दर्शाइए कि फलन f ( x , b ) f ( x , b ) f(x,b)f(x, b)f(x,b) और f ( a , y ) f ( a , y ) f(a,y)f(a, y)f(a,y) क्रमशः x = a x = a x=ax=ax=a और y = b y = b y=by=by=b पर संतत हैं।
Let f : D ( R 2 ) R f : D R 2 R f:D(subeR^(2))rarrRf: D\left(\subseteq \mathbb{R}^2\right) \rightarrow \mathbb{R}f:D(R2)R be a function and ( a , b ) D ( a , b ) D (a,b)in D(a, b) \in D(a,b)D. If f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) is continuous at ( a , b ) ( a , b ) (a,b)(a, b)(a,b), then show that the functions f ( x , b ) f ( x , b ) f(x,b)f(x, b)f(x,b) and f ( a , y ) f ( a , y ) f(a,y)f(a, y)f(a,y) are continuous at x = a x = a x=ax=ax=a and at y = b y = b y=by=by=b respectively.
Answer:

Introduction

The problem asks us to prove that if a function f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) is continuous at a point ( a , b ) ( a , b ) (a,b)(a, b)(a,b), then the functions f ( x , b ) f ( x , b ) f(x,b)f(x, b)f(x,b) and f ( a , y ) f ( a , y ) f(a,y)f(a, y)f(a,y) are continuous at x = a x = a x=ax = ax=a and y = b y = b y=by = by=b respectively. To prove this, we will use the definition of continuity and manipulate the mathematical expressions accordingly.

Work/Calculations

Step 1: Definition of Continuity

A function f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) is said to be continuous at ( a , b ) ( a , b ) (a,b)(a, b)(a,b) if for every ϵ > 0 ϵ > 0 epsilon > 0\epsilon > 0ϵ>0, there exists δ > 0 δ > 0 delta > 0\delta > 0δ>0 such that:
( x a ) 2 + ( y b ) 2 < δ | f ( x , y ) f ( a , b ) | < ϵ ( x a ) 2 + ( y b ) 2 < δ | f ( x , y ) f ( a , b ) | < ϵ sqrt((x-a)^(2)+(y-b)^(2)) < deltaLongrightarrow|f(x,y)-f(a,b)| < epsilon\sqrt{(x-a)^2 + (y-b)^2} < \delta \implies |f(x, y) – f(a, b)| < \epsilon(xa)2+(yb)2<δ|f(x,y)f(a,b)|<ϵ

Step 2: Prove Continuity for f ( x , b ) f ( x , b ) f(x,b)f(x, b)f(x,b) at x = a x = a x=ax = ax=a

We need to show that for every ϵ > 0 ϵ > 0 epsilon > 0\epsilon > 0ϵ>0, there exists δ > 0 δ > 0 delta > 0\delta > 0δ>0 such that:
| x a | < δ | f ( x , b ) f ( a , b ) | < ϵ | x a | < δ | f ( x , b ) f ( a , b ) | < ϵ |x-a| < deltaLongrightarrow|f(x,b)-f(a,b)| < epsilon|x – a| < \delta \implies |f(x, b) – f(a, b)| < \epsilon|xa|<δ|f(x,b)f(a,b)|<ϵ
To prove this, let’s consider ϵ > 0 ϵ > 0 epsilon > 0\epsilon > 0ϵ>0. Since f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) is continuous at ( a , b ) ( a , b ) (a,b)(a, b)(a,b), there exists δ > 0 δ > 0 delta > 0\delta > 0δ>0 such that:
( x a ) 2 + ( y b ) 2 < δ | f ( x , y ) f ( a , b ) | < ϵ ( x a ) 2 + ( y b ) 2 < δ | f ( x , y ) f ( a , b ) | < ϵ sqrt((x-a)^(2)+(y-b)^(2)) < deltaLongrightarrow|f(x,y)-f(a,b)| < epsilon\sqrt{(x-a)^2 + (y-b)^2} < \delta \implies |f(x, y) – f(a, b)| < \epsilon(xa)2+(yb)2<δ|f(x,y)f(a,b)|<ϵ
Now, consider | x a | < δ | x a | < δ |x-a| < delta|x – a| < \delta|xa|<δ. We can rewrite this as ( x a ) 2 + ( b b ) 2 < δ ( x a ) 2 + ( b b ) 2 < δ sqrt((x-a)^(2)+(b-b)^(2)) < delta\sqrt{(x-a)^2 + (b-b)^2} < \delta(xa)2+(bb)2<δ.
By the continuity of f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) at ( a , b ) ( a , b ) (a,b)(a, b)(a,b), this implies:
| f ( x , b ) f ( a , b ) | < ϵ | f ( x , b ) f ( a , b ) | < ϵ |f(x,b)-f(a,b)| < epsilon|f(x, b) – f(a, b)| < \epsilon|f(x,b)f(a,b)|<ϵ
Thus, we have shown that f ( x , b ) f ( x , b ) f(x,b)f(x, b)f(x,b) is continuous at x = a x = a x=ax = ax=a.

Step 3: Prove Continuity for f ( a , y ) f ( a , y ) f(a,y)f(a, y)f(a,y) at y = b y = b y=by = by=b

Similarly, we need to show that for every ϵ > 0 ϵ > 0 epsilon > 0\epsilon > 0ϵ>0, there exists δ > 0 δ > 0 delta > 0\delta > 0δ>0 such that:
| y b | < δ | f ( a , y ) f ( a , b ) | < ϵ | y b | < δ | f ( a , y ) f ( a , b ) | < ϵ |y-b| < deltaLongrightarrow|f(a,y)-f(a,b)| < epsilon|y – b| < \delta \implies |f(a, y) – f(a, b)| < \epsilon|yb|<δ|f(a,y)f(a,b)|<ϵ
Again, consider ϵ > 0 ϵ > 0 epsilon > 0\epsilon > 0ϵ>0. By the continuity of f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) at ( a , b ) ( a , b ) (a,b)(a, b)(a,b), there exists δ > 0 δ > 0 delta > 0\delta > 0δ>0 such that:
( x a ) 2 + ( y b ) 2 < δ | f ( x , y ) f ( a , b ) | < ϵ ( x a ) 2 + ( y b ) 2 < δ | f ( x , y ) f ( a , b ) | < ϵ sqrt((x-a)^(2)+(y-b)^(2)) < deltaLongrightarrow|f(x,y)-f(a,b)| < epsilon\sqrt{(x-a)^2 + (y-b)^2} < \delta \implies |f(x, y) – f(a, b)| < \epsilon(xa)2+(yb)2<δ|f(x,y)f(a,b)|<ϵ
Now, consider | y b | < δ | y b | < δ |y-b| < delta|y – b| < \delta|yb|<δ. We can rewrite this as ( a a ) 2 + ( y b ) 2 < δ ( a a ) 2 + ( y b ) 2 < δ sqrt((a-a)^(2)+(y-b)^(2)) < delta\sqrt{(a-a)^2 + (y-b)^2} < \delta(aa)2+(yb)2<δ.
By the continuity of f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) at ( a , b ) ( a , b ) (a,b)(a, b)(a,b), this implies:
| f ( a , y ) f ( a , b ) | < ϵ | f ( a , y ) f ( a , b ) | < ϵ |f(a,y)-f(a,b)| < epsilon|f(a, y) – f(a, b)| < \epsilon|f(a,y)f(a,b)|<ϵ
Thus, we have shown that f ( a , y ) f ( a , y ) f(a,y)f(a, y)f(a,y) is continuous at y = b y = b y=by = by=b.

Conclusion

We have successfully proven that if f ( x , y ) f ( x , y ) f(x,y)f(x, y)f(x,y) is continuous at ( a , b ) ( a , b ) (a,b)(a, b)(a,b), then f ( x , b ) f ( x , b ) f(x,b)f(x, b)f(x,b) is continuous at x = a x = a x=ax = ax=a and f ( a , y ) f ( a , y ) f(a,y)f(a, y)f(a,y) is continuous at y = b y = b y=by = by=b. We used the definition of continuity to establish these results.
(c) माना कि T : R 2 R 2 T : R 2 R 2 T:R^(2)rarrR^(2)T: \mathbb{R}^2 \rightarrow \mathbb{R}^2T:R2R2 एक रैखिक प्रतिचित्र है, जैसा कि T ( 2 , 1 ) = ( 5 , 7 ) T ( 2 , 1 ) = ( 5 , 7 ) T(2,1)=(5,7)T(2,1)=(5,7)T(2,1)=(5,7) एवं T ( 1 , 2 ) = ( 3 , 3 ) T ( 1 , 2 ) = ( 3 , 3 ) T(1,2)=(3,3)T(1,2)=(3,3)T(1,2)=(3,3). अगर A A AAA मानक आधारों e 1 , e 2 e 1 , e 2 e_(1),e_(2)e_1, e_2e1,e2 के सापेक्ष T T TTT के संगत आव्यूह है, तो A A AAA की कोटि ज्ञात कीजिए।
Let T : R 2 R 2 T : R 2 R 2 T:R^(2)rarrR^(2)T: \mathbb{R}^2 \rightarrow \mathbb{R}^2T:R2R2 be a linear map such that T ( 2 , 1 ) = ( 5 , 7 ) T ( 2 , 1 ) = ( 5 , 7 ) T(2,1)=(5,7)T(2,1)=(5,7)T(2,1)=(5,7) and T ( 1 , 2 ) = ( 3 , 3 ) T ( 1 , 2 ) = ( 3 , 3 ) T(1,2)=(3,3)T(1,2)=(3,3)T(1,2)=(3,3).
If A A AAA is the matrix corresponding to T T TTT with respect to the standard bases e 1 , e 2 e 1 , e 2 e_(1),e_(2)e_1, e_2e1,e2, then find Rank ( A ) Rank ( A ) Rank(A)\operatorname{Rank}(A)Rank(A).
Answer:
  1. Expressing ( a , b ) ( a , b ) (a,b)(a, b)(a,b) as a Linear Combination
( a , b ) = α ( 2 , 1 ) + β ( 1 , 2 ) ( a , b ) = α ( 2 , 1 ) + β ( 1 , 2 ) (a,b)=alpha(2,1)+beta(1,2)(a, b) = \alpha(2,1) + \beta(1,2)(a,b)=α(2,1)+β(1,2)
a = 2 α + β (Equation 1) a = 2 α + β (Equation 1) a=2alpha+betaquad(Equation 1)a = 2\alpha + \beta \quad \text{(Equation 1)}a=2α+β(Equation 1)
b = α + 2 β (Equation 2) b = α + 2 β (Equation 2) b=alpha+2betaquad(Equation 2)b = \alpha + 2\beta \quad \text{(Equation 2)}b=α+2β(Equation 2)
  1. Solving for α α alpha\alphaα and β β beta\betaβ
From Equation 2 multiplied by 2 minus Equation 1, we get:
3 β = 2 b a 3 β = 2 b a 3beta=2b-a3\beta = 2b – a3β=2ba
β = 2 b a 3 β = 2 b a 3 beta=(2b-a)/(3)\beta = \frac{2b – a}{3}β=2ba3
α = 2 a b 3 α = 2 a b 3 alpha=(2a-b)/(3)\alpha = \frac{2a – b}{3}α=2ab3
  1. Finding T ( a , b ) T ( a , b ) T(a,b)T(a, b)T(a,b) in terms of T ( 2 , 1 ) T ( 2 , 1 ) T(2,1)T(2,1)T(2,1) and T ( 1 , 2 ) T ( 1 , 2 ) T(1,2)T(1,2)T(1,2)
T ( a , b ) = 2 a b 3 T ( 2 , 1 ) + 2 b a 3 T ( 1 , 2 ) T ( a , b ) = 2 a b 3 T ( 2 , 1 ) + 2 b a 3 T ( 1 , 2 ) T(a,b)=(2a-b)/(3)T(2,1)+(2b-a)/(3)T(1,2)T(a, b) = \frac{2a – b}{3} T(2,1) + \frac{2b – a}{3} T(1,2)T(a,b)=2ab3T(2,1)+2ba3T(1,2)
  1. Finding T ( e 1 ) T ( e 1 ) T(e_(1))T(e_1)T(e1) and T ( e 2 ) T ( e 2 ) T(e_(2))T(e_2)T(e2)
T ( 1 , 0 ) = 2 3 ( 5 , 7 ) 1 3 ( 3 , 3 ) = ( 7 3 , 11 3 ) T ( 1 , 0 ) = 2 3 ( 5 , 7 ) 1 3 ( 3 , 3 ) = 7 3 , 11 3 T(1,0)=(2)/(3)(5,7)-(1)/(3)(3,3)=((7)/(3),(11)/(3))T(1,0) = \frac{2}{3}(5,7) – \frac{1}{3}(3,3) = \left(\frac{7}{3}, \frac{11}{3}\right)T(1,0)=23(5,7)13(3,3)=(73,113)
T ( 0 , 1 ) = 1 3 ( 5 , 7 ) + 2 3 ( 3 , 3 ) = ( 1 3 , 1 3 ) T ( 0 , 1 ) = 1 3 ( 5 , 7 ) + 2 3 ( 3 , 3 ) = 1 3 , 1 3 T(0,1)=-(1)/(3)(5,7)+(2)/(3)(3,3)=((1)/(3),-(1)/(3))T(0,1) = -\frac{1}{3}(5,7) + \frac{2}{3}(3,3) = \left(\frac{1}{3}, -\frac{1}{3}\right)T(0,1)=13(5,7)+23(3,3)=(13,13)
  1. Finding Matrix A A AAA
A = [ 7 3 1 3 11 3 1 3 ] A = 7 3 1 3 11 3 1 3 A=[[(7)/(3),(1)/(3)],[(11)/(3),-(1)/(3)]]A = \left[\begin{array}{cc} \frac{7}{3} & \frac{1}{3} \\ \frac{11}{3} & -\frac{1}{3} \end{array}\right]A=[731311313]
  1. Finding the Rank of A A AAA
The determinant of A A AAA is:
Det ( A ) = 7 × ( 1 / 3 ) 11 × 1 / 3 3 = 18 9 = 2 0 Det ( A ) = 7 × ( 1 / 3 ) 11 × 1 / 3 3 = 18 9 = 2 0 “Det”(A)=(-7xx(-1//3)-11 xx1//3)/(3)=-(18)/(9)=-2!=0\text{Det}(A) = \frac{-7 \times (-1/3) – 11 \times 1/3}{3} = -\frac{18}{9} = -2 \neq 0Det(A)=7×(1/3)11×1/33=189=20
Since the determinant is not zero, the matrix is invertible, and its rank is equal to the dimension of the domain, which is 2.

Conclusion

Rank ( A ) = 2 Rank ( A ) = 2 Rank(A)=2\operatorname{Rank}(A) = 2Rank(A)=2
(d) अगर
A = [ 1 2 1 1 4 1 3 0 3 ] और B = [ 2 1 1 1 1 0 2 1 1 ] A = 1      2      1 1      4      1 3      0      3 और B = 2      1      1 1      1      0 2      1      1 A=[[1,2,1],[1,-4,1],[3,0,-3]]” और “B=[[2,1,1],[1,-1,0],[2,1,-1]]A=\left[\begin{array}{rrr} 1 & 2 & 1 \\ 1 & -4 & 1 \\ 3 & 0 & -3 \end{array}\right] \text { और } B=\left[\begin{array}{rrr} 2 & 1 & 1 \\ 1 & -1 & 0 \\ 2 & 1 & -1 \end{array}\right]A=[121141303] और B=[211110211]
है, तो दर्शाइए कि A B = 6 I 3 A B = 6 I 3 AB=6I_(3)A B=6 I_3AB=6I3. इस परिणाम का उपयोग करते हुए निम्नलिखित समीकरण निकाय को हल कीजिए :
2 x + y + z = 5 x y = 0 2 x + y z = 1 2 x + y + z = 5 x y = 0 2 x + y z = 1 {:[2x+y+z=5],[x-y=0],[2x+y-z=1]:}\begin{array}{r} 2 x+y+z=5 \\ x-y=0 \\ 2 x+y-z=1 \end{array}2x+y+z=5xy=02x+yz=1
If
A = [ 1 2 1 1 4 1 3 0 3 ] and B = [ 2 1 1 1 1 0 2 1 1 ] A = 1      2      1 1      4      1 3      0      3 and B = 2      1      1 1      1      0 2      1      1 A=[[1,2,1],[1,-4,1],[3,0,-3]]quad” and “B=[[2,1,1],[1,-1,0],[2,1,-1]]A=\left[\begin{array}{rrr} 1 & 2 & 1 \\ 1 & -4 & 1 \\ 3 & 0 & -3 \end{array}\right] \quad \text { and } B=\left[\begin{array}{rrr} 2 & 1 & 1 \\ 1 & -1 & 0 \\ 2 & 1 & -1 \end{array}\right]A=[121141303] and B=[211110211]
then show that A B = 6 I 3 A B = 6 I 3 AB=6I_(3)A B=6 I_3AB=6I3. Use this result to solve the following system of equations :
2 x + y + z = 5 x y = 0 2 x + y z = 1 2 x + y + z = 5 x y = 0 2 x + y z = 1 {:[2x+y+z=5],[x-y=0],[2x+y-z=1]:}\begin{array}{r} 2 x+y+z=5 \\ x-y=0 \\ 2 x+y-z=1 \end{array}2x+y+z=5xy=02x+yz=1
Answer:

Introduction

The problem asks us to show that A B = 6 I 3 A B = 6 I 3 AB=6I_(3)AB = 6I_3AB=6I3 for given matrices A A AAA and B B BBB, and then use this result to solve a system of equations. I 3 I 3 I_(3)I_3I3 is the 3 × 3 3 × 3 3xx33 \times 33×3 identity matrix.

Work/Calculations

Step 1: Calculate A B A B ABABAB

The first task is to calculate A B A B ABABAB. The matrices A A AAA and B B BBB are:
A = ( 1 2 1 1 4 1 3 0 3 ) A = 1 2 1 1 4 1 3 0 3 A=([1,2,1],[1,-4,1],[3,0,-3])A = \begin{pmatrix} 1 & 2 & 1 \\ 1 & -4 & 1 \\ 3 & 0 & -3 \end{pmatrix}A=(121141303)
B = ( 2 1 1 1 1 0 2 1 1 ) B = 2 1 1 1 1 0 2 1 1 B=([2,1,1],[1,-1,0],[2,1,-1])B = \begin{pmatrix} 2 & 1 & 1 \\ 1 & -1 & 0 \\ 2 & 1 & -1 \end{pmatrix}B=(211110211)
A × B = [ 1 2 1 1 4 1 3 0 3 ] × [ 2 1 1 1 1 0 2 1 1 ] = [ 1 × 2 + 2 × 1 + 1 × 2 1 × 1 + 2 × 1 + 1 × 1 1 × 1 + 2 × 0 + 1 × 1 1 × 2 4 × 1 + 1 × 2 1 × 1 4 × 1 + 1 × 1 1 × 1 4 × 0 + 1 × 1 3 × 2 + 0 × 1 3 × 2 3 × 1 + 0 × 1 3 × 1 3 × 1 + 0 × 0 3 × 1 ] = [ 2 + 2 + 2 1 2 + 1 1 + 0 1 2 4 + 2 1 + 4 + 1 1 + 0 1 6 + 0 6 3 + 0 3 3 + 0 + 3 ] = [ 6 0 0 0 6 0 0 0 6 ] A × B = 1 2 1 1 4 1 3 0 3 × 2 1 1 1 1 0 2 1 1 = 1 × 2 + 2 × 1 + 1 × 2 1 × 1 + 2 × 1 + 1 × 1 1 × 1 + 2 × 0 + 1 × 1 1 × 2 4 × 1 + 1 × 2 1 × 1 4 × 1 + 1 × 1 1 × 1 4 × 0 + 1 × 1 3 × 2 + 0 × 1 3 × 2 3 × 1 + 0 × 1 3 × 1 3 × 1 + 0 × 0 3 × 1 = 2 + 2 + 2 1 2 + 1 1 + 0 1 2 4 + 2 1 + 4 + 1 1 + 0 1 6 + 0 6 3 + 0 3 3 + 0 + 3 = 6 0 0 0 6 0 0 0 6 {:[A xx B=[[1,2,1],[1,-4,1],[3,0,-3]]xx[[2,1,1],[1,-1,0],[2,1,-1]]],[=[[1xx2+2xx1+1xx2,1xx1+2xx-1+1xx1,1xx1+2xx0+1xx-1],[1xx2-4xx1+1xx2,1xx1-4xx-1+1xx1,1xx1-4xx0+1xx-1],[3xx2+0xx1-3xx2,3xx1+0xx-1-3xx1,3xx1+0xx0-3xx-1]]],[=[[2+2+2,1-2+1,1+0-1],[2-4+2,1+4+1,1+0-1],[6+0-6,3+0-3,3+0+3]]],[=[[6,0,0],[0,6,0],[0,0,6]]],[]:}\begin{aligned} & A \times B=\left[\begin{array}{ccc} 1 & 2 & 1 \\ 1 & -4 & 1 \\ 3 & 0 & -3 \end{array}\right] \times\left[\begin{array}{ccc} 2 & 1 & 1 \\ 1 & -1 & 0 \\ 2 & 1 & -1 \end{array}\right] \\ & =\left[\begin{array}{llll} 1 \times 2+2 \times 1+1 \times 2 & 1 \times 1+2 \times-1+1 \times 1 & 1 \times 1+2 \times 0+1 \times-1 \\ 1 \times 2-4 \times 1+1 \times 2 & 1 \times 1-4 \times-1+1 \times 1 & 1 \times 1-4 \times 0+1 \times-1 \\ 3 \times 2+0 \times 1-3 \times 2 & 3 \times 1+0 \times-1-3 \times 1 & 3 \times 1+0 \times 0-3 \times-1 \end{array}\right] \\ & =\left[\begin{array}{ccc} 2+2+2 & 1-2+1 & 1+0-1 \\ 2-4+2 & 1+4+1 & 1+0-1 \\ 6+0-6 & 3+0-3 & 3+0+3 \end{array}\right] \\ & =\left[\begin{array}{lll} 6 & 0 & 0 \\ 0 & 6 & 0 \\ 0 & 0 & 6 \end{array}\right] \\ & \end{aligned}A×B=[121141303]×[211110211]=[1×2+2×1+1×21×1+2×1+1×11×1+2×0+1×11×24×1+1×21×14×1+1×11×14×0+1×13×2+0×13×23×1+0×13×13×1+0×03×1]=[2+2+212+11+0124+21+4+11+016+063+033+0+3]=[600060006]
After calculating, we find that A B A B ABABAB is:
A B = ( 6 0 0 0 6 0 0 0 6 ) A B = 6 0 0 0 6 0 0 0 6 AB=([6,0,0],[0,6,0],[0,0,6])AB = \begin{pmatrix} 6 & 0 & 0 \\ 0 & 6 & 0 \\ 0 & 0 & 6 \end{pmatrix}AB=(600060006)
This is equivalent to 6 I 3 6 I 3 6I_(3)6I_36I3, where I 3 I 3 I_(3)I_3I3 is the 3 × 3 3 × 3 3xx33 \times 33×3 identity matrix.

Step 2: Solve the System of Equations

The system of equations is:
2 x + y + z = 5 x y = 0 2 x + y z = 1 2 x + y + z = 5 x y = 0 2 x + y z = 1 {:[2x+y+z=5],[x-y=0],[2x+y-z=1]:}\begin{aligned} 2x + y + z &= 5 \\ x – y &= 0 \\ 2x + y – z &= 1 \end{aligned}2x+y+z=5xy=02x+yz=1
We can write this system as A x = b A x = b Ax=bAx = bAx=b, where A A AAA is the matrix from the problem statement, and b = ( 5 0 1 ) b = 5 0 1 b=([5],[0],[1])b = \begin{pmatrix} 5 \\ 0 \\ 1 \end{pmatrix}b=(501).
Since A B = 6 I 3 , we have A 1 = 1 6 B . Since A B = 6 I 3 , we have A 1 = 1 6 B . ” Since “AB=6I_(3)”, we have “A^(-1)=(1)/(6)B”. “\text { Since } A B=6 I_3 \text {, we have } A^{-1}=\frac{1}{6} B \text {. } Since AB=6I3, we have A1=16B.
Here, X = A 1 × b X = A 1 × b X=A^(-1)xx bX=A^{-1} \times bX=A1×b
X = 1 | A | × Adj ( A ) × b X = 1 6 × [ 1 2 1 1 4 1 3 0 3 ] × [ 5 0 1 ] X = 1 6 × [ 1 × 5 + 2 × 0 + 1 × 1 1 × 5 4 × 0 + 1 × 1 3 × 5 + 0 × 0 3 × 1 ] X = 1 6 × [ 6 6 12 ] X = [ 1 1 2 ] X = 1 | A | × Adj ( A ) × b X = 1 6 × 1 2 1 1 4 1 3 0 3 × 5 0 1 X = 1 6 × 1 × 5 + 2 × 0 + 1 × 1 1 × 5 4 × 0 + 1 × 1 3 × 5 + 0 × 0 3 × 1 X = 1 6 × 6 6 12 X = 1 1 2 {:[:.X=(1)/(|A|)xx Adj(A)xx b],[X=(1)/(6)xx[[1,2,1],[1,-4,1],[3,0,-3]]xx[[5],[0],[1]]],[X=(1)/(6)xx[[1xx5+2xx0+1xx1],[1xx5-4xx0+1xx1],[3xx5+0xx0-3xx1]]],[X=(1)/(6)xx[[6],[6],[12]]],[X=[[1],[1],[2]]]:}\begin{aligned} & \therefore X=\frac{1}{|A|} \times \operatorname{Adj}(A) \times b \\ &X =\frac{1}{6} \times\left[\begin{array}{ccc} 1 & 2 & 1 \\ 1 & -4 & 1 \\ 3 & 0 & -3 \end{array}\right] \times\left[\begin{array}{l} 5 \\ 0 \\ 1 \end{array}\right] \\ &X =\frac{1}{6}\times\left[\begin{array}{c} 1 \times 5+2 \times 0+1 \times 1 \\ 1 \times 5-4 \times 0+1 \times 1 \\ 3 \times 5+0 \times 0-3 \times 1 \end{array}\right] \\ &X =\frac{1}{6} \times\left[\begin{array}{c} 6 \\ 6 \\ 12 \end{array}\right] \\ &X =\left[\begin{array}{c} 1 \\ 1 \\ 2 \end{array}\right] \end{aligned}X=1|A|×Adj(A)×bX=16×[121141303]×[501]X=16×[1×5+2×0+1×11×54×0+1×13×5+0×03×1]X=16×[6612]X=[112]
Hence ( x y z ) = ( 1 1 2 ) x y z = 1 1 2 ([x],[y],[z])=([1],[1],[2])\begin{pmatrix}x\\ y\\ z\end{pmatrix}=\begin{pmatrix}1\\ 1\\ 2\end{pmatrix}(xyz)=(112)
(e) दर्शाइए कि
x + 1 3 = y 3 2 = z + 2 1 और x 1 = y 7 3 = z + 7 2 x + 1 3 = y 3 2 = z + 2 1 और x 1 = y 7 3 = z + 7 2 (x+1)/(-3)=(y-3)/(2)=(z+2)/(1)” और “(x)/(1)=(y-7)/(-3)=(z+7)/(2)\frac{x+1}{-3}=\frac{y-3}{2}=\frac{z+2}{1} \text { और } \frac{x}{1}=\frac{y-7}{-3}=\frac{z+7}{2}x+13=y32=z+21 और x1=y73=z+72
प्रतिच्छेदी रेखाएँ हैं। प्रतिच्छेद बिंदु के निर्देशांकों और उस समतल, जिसमें दोनों रेखाएँ हैं, का समीकरण ज्ञात कीजिए।
Show that the lines
x + 1 3 = y 3 2 = z + 2 1 and x 1 = y 7 3 = z + 7 2 x + 1 3 = y 3 2 = z + 2 1 and x 1 = y 7 3 = z + 7 2 (x+1)/(-3)=(y-3)/(2)=(z+2)/(1)” and “(x)/(1)=(y-7)/(-3)=(z+7)/(2)\frac{x+1}{-3}=\frac{y-3}{2}=\frac{z+2}{1} \text { and } \frac{x}{1}=\frac{y-7}{-3}=\frac{z+7}{2}x+13=y32=z+21 and x1=y73=z+72
intersect. Find the coordinates of the point of intersection and the equation of the plane containing them.
Answer:
Proving Intersection of Lines
Given two lines:
Line 1:
x + 1 3 = y 3 2 = z + 2 1 x + 1 3 = y 3 2 = z + 2 1 (x+1)/(-3)=(y-3)/(2)=(z+2)/(1)\frac{x+1}{-3} = \frac{y-3}{2} = \frac{z+2}{1}x+13=y32=z+21
Line 2:
x 1 = y 7 3 = z + 7 2 x 1 = y 7 3 = z + 7 2 (x)/(1)=(y-7)/(-3)=(z+7)/(2)\frac{x}{1} = \frac{y-7}{-3} = \frac{z+7}{2}x1=y73=z+72
Let’s parameterize these lines as follows:
Line 1:
( x , y , z ) = ( 1 3 r , 3 + 2 r , 2 + r ) (1) ( x , y , z ) = ( 1 3 r , 3 + 2 r , 2 + r ) (1) (x,y,z)=(-1-3r,3+2r,-2+r)quad(1)(x, y, z) = (-1-3r, 3+2r, -2+r) \quad \text{(1)}(x,y,z)=(13r,3+2r,2+r)(1)
Line 2:
( x , y , z ) = ( r , 7 3 r , 7 + 2 r ) (2) ( x , y , z ) = ( r , 7 3 r , 7 + 2 r ) (2) (x,y,z)=(r^(‘),7-3r^(‘),-7+2r^(‘))quad(2)(x, y, z) = (r’, 7-3r’, -7+2r’) \quad \text{(2)}(x,y,z)=(r,73r,7+2r)(2)
For the two lines to intersect, there must exist values of r r rrr and r r r^(‘)r’r such that the points on these lines coincide.
Step 1: Setting up Equations
We set up the equations:
1 3 r = r 3 + 2 r = 7 3 r 2 + r = 7 + 2 r 1 3 r = r 3 + 2 r = 7 3 r 2 + r = 7 + 2 r {:[-1-3r=r^(‘)],[3+2r=7-3r^(‘)],[-2+r=-7+2r^(‘)]:}\begin{aligned} & -1-3r = r’ \\ & 3+2r = 7-3r’ \\ & -2+r = -7+2r’ \end{aligned}13r=r3+2r=73r2+r=7+2r
Step 2: Solving Equations
Solving the first two equations:
From the first equation, we get r = 1 r = 1 r=-1r = -1r=1.
Substituting r = 1 r = 1 r=-1r = -1r=1 into the second equation, we find r = 2 r = 2 r^(‘)=2r’ = 2r=2.
Now, we check if these values satisfy the third equation:
2 + ( 1 ) = 7 + 2 ( 2 ) 3 = 3 2 + ( 1 ) = 7 + 2 ( 2 ) 3 = 3 -2+(-1)=-7+2(2)Longrightarrow-3=-3-2 + (-1) = -7 + 2(2) \implies -3 = -32+(1)=7+2(2)3=3
So, the values r = 1 r = 1 r=-1r = -1r=1 and r = 2 r = 2 r^(‘)=2r’ = 2r=2 satisfy all three equations.
Step 3: Finding Intersection Point
Substituting these values of r r rrr and r r r^(‘)r’r into either (1) or (2), we get the coordinates of the point of intersection:
From (1):
( x , y , z ) = ( 2 , 1 , 3 ) ( x , y , z ) = ( 2 , 1 , 3 ) (x,y,z)=(2,1,-3)(x, y, z) = (2, 1, -3)(x,y,z)=(2,1,3)
Step 4: Finding the Equation of the Plane
The equation of the plane containing the given lines can be found using the cross product of the direction ratios of the lines.
Direction ratios of Line 1: ( 3 , 2 , 1 ) ( 3 , 2 , 1 ) (-3,2,1)(-3, 2, 1)(3,2,1)
Direction ratios of Line 2: ( 1 , 3 , 2 ) ( 1 , 3 , 2 ) (1,-3,2)(1, -3, 2)(1,3,2)
Now, we find the cross product of these direction ratios to get the normal vector of the plane:
| i j k 3 2 1 1 3 2 | = i × | 2 1 3 2 | j × | 3 1 1 2 | + k × | 3 2 1 3 | = i × ( 2 × 2 1 × ( 3 ) ) j × ( ( 3 ) × 2 1 × 1 ) + k × ( ( 3 ) × ( 3 ) 2 × 1 ) = i × ( 4 + 3 ) j × ( 6 1 ) + k × ( 9 2 ) = i × ( 7 ) j × ( 7 ) + k × ( 7 ) = 7 i + 7 j + 7 k = 7 i + 7 k + 7 j i j k 3 2 1 1 3 2 = i × 2 1 3 2 j × 3 1 1 2 + k × 3 2 1 3 = i × ( 2 × 2 1 × ( 3 ) ) j × ( ( 3 ) × 2 1 × 1 ) + k × ( ( 3 ) × ( 3 ) 2 × 1 ) = i × ( 4 + 3 ) j × ( 6 1 ) + k × ( 9 2 ) = i × ( 7 ) j × ( 7 ) + k × ( 7 ) = 7 i + 7 j + 7 k = 7 i + 7 k + 7 j {:[|[i,j,k],[-3,2,1],[1,-3,2]|],[=i xx|[2,1],[-3,2]|-j xx|[-3,1],[1,2]|+k xx|[-3,2],[1,-3]|],[=i xx(2xx2-1xx(-3))-j xx((-3)xx2-1xx1)+k xx((-3)xx(-3)-2xx1)],[=i xx(4+3)-j xx(-6-1)+k xx(9-2)],[=i xx(7)-j xx(-7)+k xx(7)],[=7i+7j+7k],[=7i+7k+7j]:}\begin{aligned} &\left|\begin{array}{ccc} i & j & k \\ -3 & 2 & 1 \\ 1 & -3 & 2 \end{array}\right| \\ & =i \times\left|\begin{array}{cc} 2 & 1 \\ -3 & 2 \end{array}\right|-j \times\left|\begin{array}{cc} -3 & 1 \\ 1 & 2 \end{array}\right|+k \times\left|\begin{array}{cc} -3 & 2 \\ 1 & -3 \end{array}\right| \\ & =i \times(2 \times 2-1 \times(-3))-j \times((-3) \times 2-1 \times 1)+k \times((-3) \times(-3)-2 \times 1) \\ & =i \times(4+3)-j \times(-6-1)+k \times(9-2) \\ & =i \times(7)-j \times(-7)+k \times(7) \\ & =7 i+7 j+7 k \\ & =7 i+7 k+7 j \end{aligned}|ijk321132|=i×|2132|j×|3112|+k×|3213|=i×(2×21×(3))j×((3)×21×1)+k×((3)×(3)2×1)=i×(4+3)j×(61)+k×(92)=i×(7)j×(7)+k×(7)=7i+7j+7k=7i+7k+7j
So, the normal vector of the plane is 7 i + 7 j + 7 k 7 i + 7 j + 7 k 7i+7j+7k7 i+7 j+7 k7i+7j+7k.
Now, we can use one of the intersection points, e.g., ( 2 , 1 , 3 ) ( 2 , 1 , 3 ) (2,1,-3)(2, 1, -3)(2,1,3), and the normal vector to find the equation of the plane:
7 ( x 2 ) + 7 ( y 1 ) + 7 ( z + 3 ) = 0 7 ( x 2 ) + 7 ( y 1 ) + 7 ( z + 3 ) = 0 7(x-2)+7(y-1)+7(z+3)=07(x – 2) + 7(y – 1) +7(z + 3) = 07(x2)+7(y1)+7(z+3)=0
Simplifying:
x + y + z = 0 x + y + z = 0 =>x+y+z=0\Rightarrow x+y+z=0x+y+z=0
This is the equation of the plane containing the given lines.
  1. (a) क्या f ( x ) = | cos x | + | sin x | , x = π 2 f ( x ) = | cos x | + | sin x | , x = π 2 f(x)=|cos x|+|sin x|,x=(pi)/(2)f(x)=|\cos x|+|\sin x|, x=\frac{\pi}{2}f(x)=|cosx|+|sinx|,x=π2 पर अवकलनीय है? अगर आपका उत्तर हाँ है, तो f ( x ) f ( x ) f(x)f(x)f(x) का अवकलज x = π 2 x = π 2 x=(pi)/(2)x=\frac{\pi}{2}x=π2 पर ज्ञात कीजिए। अगर आपका उत्तर ना है, तो अपने उत्तर का प्रमाण दीजिए।
Is f ( x ) = | cos x | + | sin x | f ( x ) = | cos x | + | sin x | f(x)=|cos x|+|sin x|f(x)=|\cos x|+|\sin x|f(x)=|cosx|+|sinx| differentiable at x = π 2 x = π 2 x=(pi)/(2)x=\frac{\pi}{2}x=π2 ? If yes, then find its derivative at x = π 2 x = π 2 x=(pi)/(2)x=\frac{\pi}{2}x=π2. If no, then give a proof of it.
Answer:

Introduction

We’re going to look at a pretty cool math problem. We have a function f ( x ) = | cos x | + | sin x | f ( x ) = | cos x | + | sin x | f(x)=|cos x|+|sin x|f(x) = |\cos x| + |\sin x|f(x)=|cosx|+|sinx|, and we want to find out if it’s differentiable at x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2. If it is, we’ll also find its derivative at that point. To make things easier, we’ll break down the function into a piecewise function and then check its differentiability.

Work/Calculations

Step 1: Breaking It Down

First, let’s rewrite f ( x ) f ( x ) f(x)f(x)f(x) as a piecewise function around x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2:
f ( x ) = { cos x + sin x if x < π 2 cos x + sin x if x > π 2 1 if x = π 2 f ( x ) = cos x + sin x      if x < π 2 cos x + sin x      if x > π 2 1      if x = π 2 f(x)={[-cos x+sin x,”if “x < (pi)/(2)],[cos x+sin x,”if “x > (pi)/(2)],[1,”if “x=(pi)/(2)]:}f(x) = \begin{cases} -\cos x + \sin x & \text{if } x < \frac{\pi}{2} \\ \cos x + \sin x & \text{if } x > \frac{\pi}{2} \\ 1 & \text{if } x = \frac{\pi}{2} \end{cases}f(x)={cosx+sinxif x<π2cosx+sinxif x>π21if x=π2

Step 2: Checking the Derivative

To see if f ( x ) f ( x ) f(x)f(x)f(x) is differentiable at x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2, we need to find the derivative from both sides of that point and see if they match.
  • Left-hand derivative: The derivative of cos x + sin x cos x + sin x -cos x+sin x-\cos x + \sin xcosx+sinx is sin x + cos x sin x + cos x sin x+cos x\sin x + \cos xsinx+cosx.
  • Right-hand derivative: The derivative of cos x + sin x cos x + sin x cos x+sin x\cos x + \sin xcosx+sinx is sin x + cos x sin x + cos x -sin x+cos x-\sin x + \cos xsinx+cosx.
Now, let’s plug x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2 into both of these derivatives and see what we get.
After calculating, we find that both the left-hand and right-hand derivatives at x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2 are 1 1 111. That’s awesome because it means the function is differentiable at x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2

Conclusion

So, there we have it! The function f ( x ) = | cos x | + | sin x | f ( x ) = | cos x | + | sin x | f(x)=|cos x|+|sin x|f(x) = |\cos x| + |\sin x|f(x)=|cosx|+|sinx| is differentiable at x = π 2 x = π 2 x=(pi)/(2)x = \frac{\pi}{2}x=π2, and its derivative at that point is 1 1 111.
(b) माना कि A A AAA और B B BBB समान कोटि के दो लांबिक आव्यूह हैं तथा det A + det B = 0 det A + det B = 0 det A+det B=0\operatorname{det} A+\operatorname{det} B=0detA+detB=0. दर्शाइए कि A + B A + B A+BA+BA+B एक अव्युत्क्रमणीय (सिंगुलर) आव्यूह है।
Let A A AAA and B B BBB be two orthogonal matrices of same order and det A + det B = 0 det A + det B = 0 det A+det B=0\operatorname{det} A+\operatorname{det} B=0detA+detB=0. Show that A + B A + B A+BA+BA+B is a singular matrix.
Answer:
Proving that A + B is Singular
Given:
  • A A AAA and B B BBB are two orthogonal matrices of the same order.
  • det A + det B = 0 det A + det B = 0 det A+det B=0\det A + \det B = 0detA+detB=0
We want to show that A + B A + B A+BA + BA+B is a singular matrix.
Step 1: Given Orthogonal Matrices
Given that A A T = B B T = I A A T = B B T = I AA^(T)=BB^(T)=IAA^T = BB^T = IAAT=BBT=I, where I I III is the identity matrix.
Also, det A = det B = 1 det A = det B = 1 det A=det B=1\det A = \det B = 1detA=detB=1 because orthogonal matrices have a determinant of 1 1 111 or 1 1 -1-11, and we’re given that det A + det B = 0 det A + det B = 0 det A+det B=0\det A + \det B = 0detA+detB=0, which implies det A = det B det A = det B det A=-det B\det A = -\det BdetA=detB.
Step 2: Determinant of AB
We know that det A det B = 1 det A det B = 1 det A*det B=-1\det A \cdot \det B = -1detAdetB=1. This implies that det ( A B ) = 1 det ( A B ) = 1 det(AB)=-1\det(AB) = -1det(AB)=1. (This is due to the property of determinants that det ( A B ) = det ( A ) det ( B ) det ( A B ) = det ( A ) det ( B ) det(AB)=det(A)*det(B)\det(AB) = \det(A) \cdot \det(B)det(AB)=det(A)det(B).)
Step 3: Expressing A + B
Now, let’s express A + B A + B A+BA + BA+B in terms of A A AAA and B B BBB:
A + B = A I + B I = A ( B T + A T ) B A + B = A I + B I = A ( B T + A T ) B A+B=AI+BI=A(B^(T)+A^(T))BA + B = AI + BI = A(B^T + A^T)BA+B=AI+BI=A(BT+AT)B
Step 4: Determinant of A + B
We want to find the determinant of A + B A + B A+BA + BA+B:
det ( A + B ) = det ( A ) det ( B T + A T ) det ( B ) = det ( A B ) det ( B T + A T ) = ( 1 ) det ( B T + A T ) (From Step 2) = det ( B T + A T ) det ( A + B ) = det ( A ) det ( B T + A T ) det ( B ) = det ( A B ) det ( B T + A T ) = ( 1 ) det ( B T + A T ) (From Step 2) = det ( B T + A T ) {:[det(A+B)=det(A)*det(B^(T)+A^(T))*det(B)],[=det(AB)*det(B^(T)+A^(T))],[=(-1)*det(B^(T)+A^(T))quad(From Step 2)],[=-det(B^(T)+A^(T))]:}\begin{aligned} \det(A + B) &= \det(A) \cdot \det(B^T + A^T) \cdot \det(B) \\ &= \det(AB) \cdot \det(B^T + A^T) \\ &= (-1) \cdot \det(B^T + A^T) \quad \text{(From Step 2)} \\ &= -\det(B^T + A^T) \end{aligned}det(A+B)=det(A)det(BT+AT)det(B)=det(AB)det(BT+AT)=(1)det(BT+AT)(From Step 2)=det(BT+AT)
Step 5: Determinant of Transpose Sum
Now, let’s focus on the determinant of the transpose sum:
det ( B T + A T ) = det ( ( B + A ) T ) (Transpose of a sum) = det ( B + A ) det ( B T + A T ) = det ( ( B + A ) T ) (Transpose of a sum) = det ( B + A ) {:[det(B^(T)+A^(T))=det((B+A)^(T))quad(Transpose of a sum)],[=det(B+A)]:}\begin{aligned} \det(B^T + A^T) &= \det((B + A)^T) \quad \text{(Transpose of a sum)} \\ &= \det(B + A) \end{aligned}det(BT+AT)=det((B+A)T)(Transpose of a sum)=det(B+A)
Step 6: Putting It All Together
Now, we can express det ( A + B ) det ( A + B ) det(A+B)\det(A + B)det(A+B) as:
det ( A + B ) = det ( B + A ) det ( A + B ) = det ( B + A ) det(A+B)=-det(B+A)\det(A + B) = -\det(B + A)det(A+B)=det(B+A)
But A + B = B + A A + B = B + A A+B=B+AA + B = B + AA+B=B+A because matrix addition is commutative.
So, we have:
det ( A + B ) = det ( B + A ) = det ( A + B ) det ( A + B ) = det ( B + A ) = det ( A + B ) det(A+B)=-det(B+A)=-det(A+B)\det(A + B) = -\det(B + A) = -\det(A + B)det(A+B)=det(B+A)=det(A+B)
This implies that 2 det ( A + B ) = 0 2 det ( A + B ) = 0 2det(A+B)=02\det(A + B) = 02det(A+B)=0.
Step 7: Conclusion
From the equation 2 det ( A + B ) = 0 2 det ( A + B ) = 0 2det(A+B)=02\det(A + B) = 02det(A+B)=0, we can conclude that det ( A + B ) = 0 det ( A + B ) = 0 det(A+B)=0\det(A + B) = 0det(A+B)=0.
A matrix is considered singular if its determinant is zero. Therefore, we have shown that A + B A + B A+BA + BA+B is a singular matrix.
(c) (i) समतल x + 2 y + 3 z = 12 x + 2 y + 3 z = 12 x+2y+3z=12x+2 y+3 z=12x+2y+3z=12 निर्देशांक अक्षों को A , B , C A , B , C A,B,CA, B, CA,B,C पर प्रतिच्छेद करता है। त्रिभुज A B C A B C ABCA B CABC के परिवृत्त का समीकरण ज्ञात कीजिए।
(ii) सिद्ध कीजिए कि समतल z = 0 z = 0 z=0z=0z=0 गोलक x 2 + y 2 + z 2 = 11 x 2 + y 2 + z 2 = 11 x^(2)+y^(2)+z^(2)=11x^2+y^2+z^2=11x2+y2+z2=11 के अन्वालोपी शंकु, जिसका शीर्ष ( 2 , 4 , 1 ) ( 2 , 4 , 1 ) (2,4,1)(2,4,1)(2,4,1) पर है, को एक समकोणीय अतिपरवलय पर प्रतिच्छेद करता है।
(i) The plane x + 2 y + 3 z = 12 x + 2 y + 3 z = 12 x+2y+3z=12x+2 y+3 z=12x+2y+3z=12 cuts the axes of coordinates in A , B , C A , B , C A,B,CA, B, CA,B,C. Find the equations of the circle circumscribing the triangle A B C A B C ABCA B CABC.
Answer:
To find the equation of the circle circumscribing the triangle ABC, we start with the given plane equation:
x + 2 y + 3 z = 12 x + 2 y + 3 z = 12 x+2y+3z=12x + 2y + 3z = 12x+2y+3z=12
This plane intersects the x-axis, y-axis, and z-axis at points A, B, and C, respectively. We’ve already found the coordinates of these points:
A(12, 0, 0)
B(0, 6, 0)
C(0, 0, 4)
Now, let’s assume the equation of the circumscribing circle is:
x 2 + y 2 + z 2 + 2 u x + 2 v y + 2 w z + d = 0 x 2 + y 2 + z 2 + 2 u x + 2 v y + 2 w z + d = 0 x^(2)+y^(2)+z^(2)+2ux+2vy+2wz+d=0x^2 + y^2 + z^2 + 2ux + 2vy + 2wz + d = 0x2+y2+z2+2ux+2vy+2wz+d=0
We need to find the values of u, v, w, and d.
  1. Using point A(12, 0, 0):
( 12 ) 2 + 2 u ( 12 ) + d = 0 ( 12 ) 2 + 2 u ( 12 ) + d = 0 (12)^(2)+2u(12)+d=0(12)^2 + 2u(12) + d = 0(12)2+2u(12)+d=0
144 + 24 u + d = 0 144 + 24 u + d = 0 144+24 u+d=0144 + 24u + d = 0144+24u+d=0
24 u + d = 144 ( 1 ) 24 u + d = 144 ( 1 ) 24 u+d=-144—-(1)24u + d = -144—- (1)24u+d=144(1)
  1. Using point B(0, 6, 0):
( 6 ) 2 + 2 v ( 6 ) + d = 0 ( 6 ) 2 + 2 v ( 6 ) + d = 0 (6)^(2)+2v(6)+d=0(6)^2 + 2v(6) + d = 0(6)2+2v(6)+d=0
36 + 12 v + d = 0 36 + 12 v + d = 0 36+12 v+d=036 + 12v + d = 036+12v+d=0
12 v + d = 36 ( 2 ) 12 v + d = 36 ( 2 ) 12 v+d=-36—-(2)12v + d = -36—- (2)12v+d=36(2)
  1. Using point C(0, 0, 4):
( 4 ) 2 + 2 w ( 4 ) + d = 0 ( 4 ) 2 + 2 w ( 4 ) + d = 0 (4)^(2)+2w(4)+d=0(4)^2 + 2w(4) + d = 0(4)2+2w(4)+d=0
16 + 8 w + d = 0 16 + 8 w + d = 0 16+8w+d=016 + 8w + d = 016+8w+d=0
8 w + d = 16 ( 3 ) 8 w + d = 16 ( 3 ) 8w+d=-16—-(3)8w + d = -16—- (3)8w+d=16(3)
Now, we can solve equations (1), (2), and (3) for u, v, and w:
  1. 24 u + d = 144 24 u + d = 144 24 u+d=-14424u + d = -14424u+d=144 implies 24 u = 144 d 24 u = 144 d 24 u=-144-d24u = -144 – d24u=144d
  2. 12 v + d = 36 12 v + d = 36 12 v+d=-3612v + d = -3612v+d=36 implies 12 v = 36 d 12 v = 36 d 12 v=-36-d12v = -36 – d12v=36d
  3. 8 w + d = 16 8 w + d = 16 8w+d=-168w + d = -168w+d=16 implies 8 w = 16 d 8 w = 16 d 8w=-16-d8w = -16 – d8w=16d
Now, we can substitute these expressions for 2u, 2v, and 2w back into the equation of the circle:
x 2 + y 2 + z 2 ( 12 d / 12 ) x ( 6 d / 6 ) y ( 4 d / 4 ) z + d = 0 x 2 + y 2 + z 2 ( 12 d / 12 ) x ( 6 d / 6 ) y ( 4 d / 4 ) z + d = 0 x^(2)+y^(2)+z^(2)-(12-d//12)x-(6-d//6)y-(4-d//4)z+d=0x^2 + y^2 + z^2 – (12 – d/12)x – (6 – d/6)y – (4 – d/4)z + d = 0x2+y2+z2(12d/12)x(6d/6)y(4d/4)z+d=0
Simplify further:
x 2 + y 2 + z 2 ( 12 d / 12 ) x ( 6 d / 6 ) y ( 4 d / 4 ) z + d = 0 x 2 + y 2 + z 2 ( 12 d / 12 ) x ( 6 d / 6 ) y ( 4 d / 4 ) z + d = 0 x^(2)+y^(2)+z^(2)-(12-d//12)x-(6-d//6)y-(4-d//4)z+d=0x^2 + y^2 + z^2 – (12 – d/12)x – (6 – d/6)y – (4 – d/4)z + d = 0x2+y2+z2(12d/12)x(6d/6)y(4d/4)z+d=0
Now, the equation of the circle is in the form:
x 2 + y 2 + z 2 + A x + B y + C z + D = 0 x 2 + y 2 + z 2 + A x + B y + C z + D = 0 x^(2)+y^(2)+z^(2)+Ax+By+Cz+D=0x^2 + y^2 + z^2 + Ax + By + Cz + D = 0x2+y2+z2+Ax+By+Cz+D=0
Where:
A = ( 12 d / 12 ) A = ( 12 d / 12 ) A=-(12-d//12)A = -(12 – d/12)A=(12d/12)
B = ( 6 d / 6 ) B = ( 6 d / 6 ) B=-(6-d//6)B = -(6 – d/6)B=(6d/6)
C = ( 4 d / 4 ) C = ( 4 d / 4 ) C=-(4-d//4)C = -(4 – d/4)C=(4d/4)
D = d D = d D=dD = dD=d
The values of A, B, C, and D can vary as d takes any real value. So, the equation of the circle circumscribing the triangle ABC is:
x 2 + y 2 + z 2 ( 12 d / 12 ) x ( 6 d / 6 ) y ( 4 d / 4 ) z + d = 0 x 2 + y 2 + z 2 ( 12 d / 12 ) x ( 6 d / 6 ) y ( 4 d / 4 ) z + d = 0 x^(2)+y^(2)+z^(2)-(12-d//12)x-(6-d//6)y-(4-d//4)z+d=0x^2 + y^2 + z^2 – (12 – d/12)x – (6 – d/6)y – (4 – d/4)z + d = 0x2+y2+z2(12d/12)x(6d/6)y(4d/4)z+d=0
Where d can be any real number.
(ii) Prove that the plane z = 0 z = 0 z=0z=0z=0 cuts the enveloping cone of the sphere x 2 + y 2 + z 2 = 11 x 2 + y 2 + z 2 = 11 x^(2)+y^(2)+z^(2)=11x^2+y^2+z^2=11x2+y2+z2=11 which has the vertex at ( 2 , 4 , 1 ) ( 2 , 4 , 1 ) (2,4,1)(2,4,1)(2,4,1) in a rectangular hyperbola.
Answer:
Given the equation of the sphere S = x 2 + y 2 + z 2 11 S = x 2 + y 2 + z 2 11 S=x^(2)+y^(2)+z^(2)-11\mathrm{S}=\mathrm{x}^2+\mathrm{y}^2+\mathrm{z}^2-11S=x2+y2+z211 and the coordinates of its vertex ( α , β , γ ) = ( 2 , 4 , 1 ) ( α , β , γ ) = ( 2 , 4 , 1 ) (alpha,beta,gamma)=(2,4,1)(\alpha, \beta, \gamma)=(2,4,1)(α,β,γ)=(2,4,1).
  1. Calculate S 1 S 1 S_(1)S_1S1 and the equation of the plane T T TTT:
    S 1 = α 2 + β 2 + γ 2 11 = 2 2 + 4 2 + 1 2 11 = 10 T = 2 x + 4 y + z 11 S 1 = α 2 + β 2 + γ 2 11 = 2 2 + 4 2 + 1 2 11 = 10 T = 2 x + 4 y + z 11 {:[S_(1)=alpha^(2)+beta^(2)+gamma^(2)-11=2^(2)+4^(2)+1^(2)-11=10],[T=2x+4y+z-11]:}\begin{aligned} \mathrm{S}_1 & = \alpha^2+\beta^2+\gamma^2-11 = 2^2+4^2+1^2-11 = 10 \\ \mathrm{T} & = 2\mathrm{x}+4\mathrm{y}+\mathrm{z}-11 \end{aligned}S1=α2+β2+γ211=22+42+1211=10T=2x+4y+z11
  2. Write the equation of the enveloping cone of the sphere:
    The equation of the enveloping cone can be written as T 2 = S S 1 T 2 = S S 1 T^(2)=SS_(1)\mathbf{T}^2 = \mathbf{S}\mathbf{S}_1T2=SS1, where T T T\mathbf{T}T is the equation of the plane and S S S\mathbf{S}S is the equation of the sphere.
    ( 2 x + 4 y + z 11 ) 2 = ( x 2 + y 2 + z 2 11 ) ( 10 ) ( 2 x + 4 y + z 11 ) 2 = ( x 2 + y 2 + z 2 11 ) ( 10 ) (2x+4y+z-11)^(2)=(x^(2)+y^(2)+z^(2)-11)(10)(2\mathrm{x}+4\mathrm{y}+\mathrm{z}-11)^2 = (\mathrm{x}^2+\mathrm{y}^2+\mathrm{z}^2-11)(10)(2x+4y+z11)2=(x2+y2+z211)(10)
  3. Substitute z = 0 z = 0 z=0z=0z=0 into the equation:
    To check if the plane z = 0 z = 0 z=0z=0z=0 cuts the cone, put z = 0 z = 0 z=0z=0z=0 in the above equation:
    10 ( x 2 + y 2 11 ) = ( 2 x + 4 y 11 ) 2 10 ( x 2 + y 2 11 ) = ( 2 x + 4 y 11 ) 2 10(x^(2)+y^(2)-11)=(2x+4y-11)^(2)10(\mathrm{x}^2+\mathrm{y}^2-11) = (2\mathrm{x}+4\mathrm{y}-11)^210(x2+y211)=(2x+4y11)2
  4. Simplify the equation:
    Further simplify the equation:
    6 x 2 + 6 y 2 16 xy + 44 x 88 y 231 = 0 6 x 2 + 6 y 2 16 xy + 44 x 88 y 231 = 0 6x^(2)+6y^(2)-16xy+44x-88y-231=06\mathrm{x}^2+6\mathrm{y}^2-16\mathrm{xy}+44\mathrm{x}-88\mathrm{y}-231 = 06x2+6y216xy+44x88y231=0
The resulting equation is a rectangular hyperbola, which proves that the plane z = 0 z = 0 z=0z=0z=0 cuts the enveloping cone of the sphere in a rectangular hyperbola.
  1. (a) फलन f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f(x)=2x^(3)-9x^(2)+12 x+6f(x)=2 x^3-9 x^2+12 x+6f(x)=2x39x2+12x+6 का अंतराल [ 2 , 3 ] [ 2 , 3 ] [2,3][2,3][2,3] पर अधिकतम और न्यूनतम मान ज्ञात कीजिए।
Find the maximum and the minimum value of the function f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f(x)=2x^(3)-9x^(2)+12 x+6f(x)=2 x^3-9 x^2+12 x+6f(x)=2x39x2+12x+6 on the interval [ 2 , 3 ] [ 2 , 3 ] [2,3][2,3][2,3].
Answer:

Introduction

The problem asks us to find the maximum and minimum values of the function f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f(x)=2x^(3)-9x^(2)+12 x+6f(x) = 2x^3 – 9x^2 + 12x + 6f(x)=2x39x2+12x+6 on the interval [ 2 , 3 ] [ 2 , 3 ] [2,3][2, 3][2,3]. To find these extremum points, we’ll use calculus methods, specifically by finding the derivative of the function and setting it equal to zero to find critical points. We’ll then evaluate the function at these critical points and the endpoints of the interval to determine the maximum and minimum values.

Work/Calculations

Step 1: Find the Derivative of f ( x ) f ( x ) f(x)f(x)f(x)

The first derivative of f ( x ) f ( x ) f(x)f(x)f(x) will give us the rate of change of the function at any given point x x xxx.
f ( x ) = d d x ( 2 x 3 9 x 2 + 12 x + 6 ) f ( x ) = d d x ( 2 x 3 9 x 2 + 12 x + 6 ) f^(‘)(x)=(d)/(dx)(2x^(3)-9x^(2)+12 x+6)f'(x) = \frac{d}{dx}(2x^3 – 9x^2 + 12x + 6)f(x)=ddx(2x39x2+12x+6)
After calculating, we find that the derivative of f ( x ) f ( x ) f(x)f(x)f(x) is:
f ( x ) = 6 x 2 18 x + 12 f ( x ) = 6 x 2 18 x + 12 f^(‘)(x)=6x^(2)-18 x+12f'(x) = 6x^2 – 18x + 12f(x)=6x218x+12

Step 2: Find the Critical Points

To find the critical points, we set f ( x ) = 0 f ( x ) = 0 f^(‘)(x)=0f'(x) = 0f(x)=0 and solve for x x xxx.
6 x 2 18 x + 12 = 0 6 x 2 18 x + 12 = 0 6x^(2)-18 x+12=06x^2 – 18x + 12 = 06x218x+12=0
After solving, we find that the critical points are x = 1 x = 1 x=1x = 1x=1 and x = 2 x = 2 x=2x = 2x=2.

Step 3: Evaluate f ( x ) f ( x ) f(x)f(x)f(x) at Critical Points and Endpoints

To find the maximum and minimum values of f ( x ) f ( x ) f(x)f(x)f(x) on the interval [ 2 , 3 ] [ 2 , 3 ] [2,3][2, 3][2,3], we need to evaluate f ( x ) f ( x ) f(x)f(x)f(x) at the critical points and the endpoints of the interval. The critical points within the interval are x = 2 x = 2 x=2x = 2x=2 and the endpoints are x = 2 x = 2 x=2x = 2x=2 and x = 3 x = 3 x=3x = 3x=3.
Let’s substitute the values into f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f ( x ) = 2 x 3 9 x 2 + 12 x + 6 f(x)=2x^(3)-9x^(2)+12 x+6f(x) = 2x^3 – 9x^2 + 12x + 6f(x)=2x39x2+12x+6 and calculate:
  1. f ( 2 ) f ( 2 ) f(2)f(2)f(2)
  2. f ( 3 ) f ( 3 ) f(3)f(3)f(3)
Let’s start by calculating f ( 2 ) f ( 2 ) f(2)f(2)f(2).
After substituting the values, we get:
f ( 2 ) = 2 × 2 3 9 × 2 2 + 12 × 2 + 6 = 10 f ( 2 ) = 2 × 2 3 9 × 2 2 + 12 × 2 + 6 = 10 f(2)=2xx2^(3)-9xx2^(2)+12 xx2+6=10f(2) = 2 \times 2^3 – 9 \times 2^2 + 12 \times 2 + 6 = 10f(2)=2×239×22+12×2+6=10
Next, let’s calculate f ( 3 ) f ( 3 ) f(3)f(3)f(3).
After substituting the values, we get:
f ( 3 ) = 2 × 3 3 9 × 3 2 + 12 × 3 + 6 = 15 f ( 3 ) = 2 × 3 3 9 × 3 2 + 12 × 3 + 6 = 15 f(3)=2xx3^(3)-9xx3^(2)+12 xx3+6=15f(3) = 2 \times 3^3 – 9 \times 3^2 + 12 \times 3 + 6 = 15f(3)=2×339×32+12×3+6=15

Conclusion

We evaluated f ( x ) f ( x ) f(x)f(x)f(x) at the critical point x = 2 x = 2 x=2x = 2x=2 and the endpoint x = 3 x = 3 x=3x = 3x=3 within the interval [ 2 , 3 ] [ 2 , 3 ] [2,3][2, 3][2,3]:
  • f ( 2 ) = 10 f ( 2 ) = 10 f(2)=10f(2) = 10f(2)=10
  • f ( 3 ) = 15 f ( 3 ) = 15 f(3)=15f(3) = 15f(3)=15
Therefore, the maximum value of f ( x ) f ( x ) f(x)f(x)f(x) on the interval [ 2 , 3 ] [ 2 , 3 ] [2,3][2, 3][2,3] is 15 15 151515 at x = 3 x = 3 x=3x = 3x=3, and the minimum value is 10 10 101010 at x = 2 x = 2 x=2x = 2x=2.
(b) सिद्ध कीजिए कि साधारणतः किसी एक बिंदु से परवलयज x 2 + y 2 = 2 a z x 2 + y 2 = 2 a z x^(2)+y^(2)=2azx^2+y^2=2 a zx2+y2=2az पर तीन अभिलंब बनाए जा सकते हैं, लेकिन अगर बिंदु सतह 27 a ( x 2 + y 2 ) + 8 ( a z ) 3 = 0 27 a x 2 + y 2 + 8 ( a z ) 3 = 0 27 a(x^(2)+y^(2))+8(a-z)^(3)=027 a\left(x^2+y^2\right)+8(a-z)^3=027a(x2+y2)+8(az)3=0 पर स्थित है, तो इन तीन अभिलंबों में से दो अभिलंब एक ही हैं।
Prove that, in general, three normals can be drawn from a given point to the paraboloid x 2 + y 2 = 2 a z x 2 + y 2 = 2 a z x^(2)+y^(2)=2azx^2+y^2=2 a zx2+y2=2az, but if the point lies on the surface
27 a ( x 2 + y 2 ) + 8 ( a z ) 3 = 0 27 a x 2 + y 2 + 8 ( a z ) 3 = 0 27 a(x^(2)+y^(2))+8(a-z)^(3)=027 a\left(x^2+y^2\right)+8(a-z)^3=027a(x2+y2)+8(az)3=0
then two of the three normals coincide.
Answer:
Introduction:
We are tasked with proving that, in general, three normals can be drawn from a given point to the paraboloid x 2 + y 2 = 2 a z x 2 + y 2 = 2 a z x^(2)+y^(2)=2azx^2+y^2=2azx2+y2=2az. However, if the point lies on the surface 27 a ( x 2 + y 2 ) + 8 ( a z ) 3 = 0 27 a ( x 2 + y 2 ) + 8 ( a z ) 3 = 0 27 a(x^(2)+y^(2))+8(a-z)^(3)=027a(x^2+y^2)+8(a-z)^3=027a(x2+y2)+8(az)3=0, then two of the three normals coincide.
Work/Calculations:
  1. The equation of the normal at ( x 1 , y 1 , z 1 ) ( x 1 , y 1 , z 1 ) (x_(1),y_(1),z_(1))(x_1, y_1, z_1)(x1,y1,z1) to the paraboloid is given by:
x x 1 x 1 = y y 1 y 1 = z z 1 a x x 1 x 1 = y y 1 y 1 = z z 1 a (x-x_(1))/(x_(1))=(y-y_(1))/(y_(1))=(z-z_(1))/(-a)\frac{x-x_1}{x_1}=\frac{y-y_1}{y_1}=\frac{z-z_1}{-a}xx1x1=yy1y1=zz1a
  1. This passes through a given point ( α , β , γ ) ( α , β , γ ) (alpha,beta,gamma)(\alpha, \beta, \gamma)(α,β,γ) if:
α x 1 x 1 = β y 1 y 1 = γ z 1 a = λ α x 1 x 1 = β y 1 y 1 = γ z 1 a = λ (alpha-x_(1))/(x_(1))=(beta-y_(1))/(y_(1))=(gamma-z_(1))/(-a)=lambda\frac{\alpha-x_1}{x_1}=\frac{\beta-y_1}{y_1}=\frac{\gamma-z_1}{-a}=\lambdaαx1x1=βy1y1=γz1a=λ
  1. Solving for x 1 x 1 x_(1)x_1x1, y 1 y 1 y_(1)y_1y1, and z 1 z 1 z_(1)z_1z1 in terms of α α alpha\alphaα, β β beta\betaβ, γ γ gamma\gammaγ, and λ λ lambda\lambdaλ using the above equations:
x 1 = α 1 + λ ; y 1 = β 1 + λ ; z 1 = γ + a λ (from (1)) x 1 = α 1 + λ ; y 1 = β 1 + λ ; z 1 = γ + a λ (from (1)) x_(1)=(alpha)/(1+lambda);quady_(1)=(beta)/(1+lambda);quadz_(1)=gamma+a lambdaquad(from (1))x_1=\frac{\alpha}{1+\lambda}; \quad y_1=\frac{\beta}{1+\lambda}; \quad z_1=\gamma+a\lambda \quad \text{(from (1))}x1=α1+λ;y1=β1+λ;z1=γ+aλ(from (1))
  1. Also, ( x 1 , y 1 , z 1 ) ( x 1 , y 1 , z 1 ) (x_(1),y_(1),z_(1))(x_1, y_1, z_1)(x1,y1,z1) lies on the given paraboloid, so:
x 1 2 + y 1 2 = 2 a z 1 (from the equation of the paraboloid) x 1 2 + y 1 2 = 2 a z 1 (from the equation of the paraboloid) x_(1)^(2)+y_(1)^(2)=2az_(1)quad(from the equation of the paraboloid)x_1^2+y_1^2=2az_1 \quad \text{(from the equation of the paraboloid)}x12+y12=2az1(from the equation of the paraboloid)
  1. Substituting the expressions for x 1 x 1 x_(1)x_1x1, y 1 y 1 y_(1)y_1y1, and z 1 z 1 z_(1)z_1z1 from step 3 into the equation above:
( α 1 + λ ) 2 + ( β 1 + λ ) 2 = 2 a ( γ + a λ ) (from (1)) α 1 + λ 2 + β 1 + λ 2 = 2 a ( γ + a λ ) (from (1)) ((alpha)/(1+lambda))^(2)+((beta)/(1+lambda))^(2)=2a(gamma+a lambda)quad(from (1))\left(\frac{\alpha}{1+\lambda}\right)^2+\left(\frac{\beta}{1+\lambda}\right)^2=2a(\gamma+a\lambda) \quad \text{(from (1))}(α1+λ)2+(β1+λ)2=2a(γ+aλ)(from (1))
  1. This equation can be simplified to:
α 2 + β 2 = 2 a ( γ + a λ ) ( 1 + λ ) 2 (from (2)) α 2 + β 2 = 2 a ( γ + a λ ) ( 1 + λ ) 2 (from (2)) alpha^(2)+beta^(2)=2a(gamma+a lambda)(1+lambda)^(2)quad(from (2))\alpha^2+\beta^2=2a(\gamma+a\lambda)(1+\lambda)^2 \quad \text{(from (2))}α2+β2=2a(γ+aλ)(1+λ)2(from (2))
  1. Equation (2) is a cubic in λ λ lambda\lambdaλ and has three values of λ λ lambda\lambdaλ that satisfy it, leading to three points on the paraboloid normal at which pass through ( α , β , γ ) ( α , β , γ ) (alpha,beta,gamma)(\alpha, \beta, \gamma)(α,β,γ).
  2. Rewriting equation (2) as a function f ( λ ) f ( λ ) f(lambda)f(\lambda)f(λ):
f ( λ ) + 2 a ( 1 + λ ) 2 ( γ + a λ ) ( α 2 β 2 ) = 0 (from (3)) f ( λ ) + 2 a ( 1 + λ ) 2 ( γ + a λ ) ( α 2 β 2 ) = 0 (from (3)) f(lambda)+2a(1+lambda)^(2)(gamma+a lambda)-(alpha^(2)-beta^(2))=0quad(from (3))f(\lambda)+2a(1+\lambda)^2(\gamma+a\lambda)-(\alpha^2-\beta^2)=0 \quad \text{(from (3))}f(λ)+2a(1+λ)2(γ+aλ)(α2β2)=0(from (3))
  1. To find the condition that equation (3) has two equal roots, we need to solve for λ λ lambda\lambdaλ where both f ( λ ) = 0 f ( λ ) = 0 f(lambda)=0f(\lambda)=0f(λ)=0 and f ( λ ) = 0 f ( λ ) = 0 f^(‘)(lambda)=0f'(\lambda)=0f(λ)=0.
  2. Differentiating f ( λ ) f ( λ ) f(lambda)f(\lambda)f(λ) with respect to λ λ lambda\lambdaλ to find f ( λ ) f ( λ ) f^(‘)(lambda)f'(\lambda)f(λ):
f ( λ ) = 2 a ( 1 + λ ) 2 ( a ) + 4 a ( 1 + λ ) ( γ + a λ ) = 0 f ( λ ) = 2 a ( 1 + λ ) 2 ( a ) + 4 a ( 1 + λ ) ( γ + a λ ) = 0 f^(‘)(lambda)=2a(1+lambda)^(2)(a)+4a(1+lambda)(gamma+a lambda)=0f'(\lambda)=2a(1+\lambda)^2(a)+4a(1+\lambda)(\gamma+a\lambda)=0f(λ)=2a(1+λ)2(a)+4a(1+λ)(γ+aλ)=0
  1. Solving for λ λ lambda\lambdaλ in f ( λ ) = 0 f ( λ ) = 0 f^(‘)(lambda)=0f'(\lambda)=0f(λ)=0:
a ( 1 + λ ) + 2 ( γ + a λ ) = 0 (since 1 + λ 0 ) a ( 1 + λ ) + 2 ( γ + a λ ) = 0 (since 1 + λ 0 ) a(1+lambda)+2(gamma+a lambda)=0quad(since 1+lambda!=0″)”a(1+\lambda)+2(\gamma+a\lambda)=0 \quad \text{(since } 1+\lambda \neq 0\text{)}a(1+λ)+2(γ+aλ)=0(since 1+λ0)
  1. Simplifying and solving for λ λ lambda\lambdaλ:
( a + 2 γ ) + λ ( 3 a ) = 0 λ = a + 2 γ 3 a ( a + 2 γ ) + λ ( 3 a ) = 0 λ = a + 2 γ 3 a (a+2gamma)+lambda(3a)=0=>lambda=-(a+2gamma)/(3a)(a+2\gamma)+\lambda(3a)=0 \Rightarrow \lambda=-\frac{a+2\gamma}{3a}(a+2γ)+λ(3a)=0λ=a+2γ3a
  1. Substituting this value of λ λ lambda\lambdaλ into equation (3):
2 a [ 1 a + 2 γ 3 a ] 2 [ γ a ( a + 2 γ ) 3 a ] = α 2 + β 2 2 a 1 a + 2 γ 3 a 2 γ a ( a + 2 γ ) 3 a = α 2 + β 2 2a[1-(a+2gamma)/(3a)]^(2)[gamma-(a(a+2gamma))/(3a)]=alpha^(2)+beta^(2)2a\left[1-\frac{a+2\gamma}{3a}\right]^2\left[\gamma-\frac{a(a+2\gamma)}{3a}\right]=\alpha^2+\beta^22a[1a+2γ3a]2[γa(a+2γ)3a]=α2+β2
  1. Further simplifying this equation:
2 a [ 2 ( a γ ) ] 2 [ a ( γ a ) ] = 27 a 3 ( α 2 + β 2 ) 2 a [ 2 ( a γ ) ] 2 [ a ( γ a ) ] = 27 a 3 ( α 2 + β 2 ) 2a[2(a-gamma)]^(2)[a(gamma-a)]=27a^(3)(alpha^(2)+beta^(2))2a[2(a-\gamma)]^2[a(\gamma-a)]=27a^3(\alpha^2+\beta^2)2a[2(aγ)]2[a(γa)]=27a3(α2+β2)
  1. Finally, the equation simplifies to:
27 a ( α 2 + β 2 ) + 8 ( a γ ) 3 = 0 27 a ( α 2 + β 2 ) + 8 ( a γ ) 3 = 0 27 a(alpha^(2)+beta^(2))+8(a-gamma)^(3)=027a(\alpha^2+\beta^2)+8(a-\gamma)^3=027a(α2+β2)+8(aγ)3=0
Conclusion:
We have successfully shown that the locus of the point ( α , β , γ ) ( α , β , γ ) (alpha,beta,gamma)(\alpha, \beta, \gamma)(α,β,γ) is 27 a ( x 2 + y 2 ) + 8 ( a z ) 3 = 0 27 a ( x 2 + y 2 ) + 8 ( a z ) 3 = 0 27 a(x^(2)+y^(2))+8(a-z)^(3)=027a(x^2+y^2)+8(a-z)^3=027a(x2+y2)+8(az)3=0. This proves the given statement.
(c) माना कि
A = ( 5 7 2 1 1 1 8 1 2 3 5 0 3 4 3 1 ) A = 5      7      2      1 1      1      8      1 2      3      5      0 3      4      3      1 A=([5,7,2,1],[1,1,-8,1],[2,3,5,0],[3,4,-3,1])A=\left(\begin{array}{rrrr} 5 & 7 & 2 & 1 \\ 1 & 1 & -8 & 1 \\ 2 & 3 & 5 & 0 \\ 3 & 4 & -3 & 1 \end{array}\right)A=(5721118123503431)
(i) आव्यूह A A AAA की कोटि ज्ञात कीजिए।
(ii) उपसमष्टि
V = { ( x 1 , x 2 , x 3 , x 4 ) R 4 A ( x 1 x 2 x 3 x 4 ) = 0 } V = x 1 , x 2 , x 3 , x 4 R 4 A x 1 x 2 x 3 x 4 = 0 V={(x_(1),x_(2),x_(3),x_(4))inR^(4)∣A([x_(1)],[x_(2)],[x_(3)],[x_(4)])=0}V=\left\{\left(x_1, x_2, x_3, x_4\right) \in \mathbb{R}^4 \mid A\left(\begin{array}{l} x_1 \\ x_2 \\ x_3 \\ x_4 \end{array}\right)=0\right\}V={(x1,x2,x3,x4)R4A(x1x2x3x4)=0}
की विमा ज्ञात कीजिए।
Let
A = ( 5 7 2 1 1 1 8 1 2 3 5 0 3 4 3 1 ) A = 5      7      2      1 1      1      8      1 2      3      5      0 3      4      3      1 A=([5,7,2,1],[1,1,-8,1],[2,3,5,0],[3,4,-3,1])A=\left(\begin{array}{rrrr} 5 & 7 & 2 & 1 \\ 1 & 1 & -8 & 1 \\ 2 & 3 & 5 & 0 \\ 3 & 4 & -3 & 1 \end{array}\right)A=(5721118123503431)
(i) Find the rank of matrix A A AAA.
(ii) Find the dimension of the subspace
V = { ( x 1 , x 2 , x 3 , x 4 ) R 4 A ( x 1 x 2 x 3 x 4 ) = 0 } V = x 1 , x 2 , x 3 , x 4 R 4 A x 1 x 2 x 3 x 4 = 0 V={(x_(1),x_(2),x_(3),x_(4))inR^(4)∣A([x_(1)],[x_(2)],[x_(3)],[x_(4)])=0}V=\left\{\left(x_1, x_2, x_3, x_4\right) \in \mathbb{R}^4 \mid A\left(\begin{array}{l} x_1 \\ x_2 \\ x_3 \\ x_4 \end{array}\right)=0\right\}V={(x1,x2,x3,x4)R4A(x1x2x3x4)=0}
Answer:
Rank [ 5 7 2 1 1 1 8 1 2 3 5 0 3 4 3 1 ] Rank 5 7 2 1 1 1 8 1 2 3 5 0 3 4 3 1 Rank[[5,7,2,1],[1,1,-8,1],[2,3,5,0],[3,4,-3,1]]\operatorname{Rank}\left[\begin{array}{cccc} 5 & 7 & 2 & 1 \\ 1 & 1 & -8 & 1 \\ 2 & 3 & 5 & 0 \\ 3 & 4 & -3 & 1 \end{array}\right]Rank[5721118123503431]
Now, reduce this matrix
R 1 R 1 ÷ 5 = [ 1 7 5 2 5 1 5 1 1 8 1 2 3 5 0 3 4 3 1 ] R 1 R 1 ÷ 5 = 1 7 5 2 5 1 5 1 1 8 1 2 3 5 0 3 4 3 1 {:[R_(1)larrR_(1)-:5],[=[[1,(7)/(5),(2)/(5),(1)/(5)],[1,1,-8,1],[2,3,5,0],[3,4,-3,1]]]:}\begin{aligned} & R_1 \leftarrow R_1 \div 5 \\ & =\left[\begin{array}{cccc} 1 & \frac{7}{5} & \frac{2}{5} & \frac{1}{5} \\ 1 & 1 & -8 & 1 \\ 2 & 3 & 5 & 0 \\ 3 & 4 & -3 & 1 \end{array}\right] \end{aligned}R1R1÷5=[1752515118123503431]
R 2 R 2 R 1 = [ 1 7 5 2 5 1 5 0 2 5 42 5 4 5 2 3 5 0 3 4 3 1 ] R 3 R 3 2 × R 1 = [ 1 7 5 2 5 1 5 0 2 5 42 5 4 5 0 1 5 21 5 2 5 3 4 3 1 ] R 2 R 2 R 1 = 1 7 5 2 5 1 5 0 2 5 42 5 4 5 2 3 5 0 3 4 3 1 R 3 R 3 2 × R 1 = 1 7 5 2 5 1 5 0 2 5 42 5 4 5 0 1 5 21 5 2 5 3 4 3 1 {:[{:[R_(2)larrR_(2)-R_(1)],[=[[1,(7)/(5),(2)/(5),(1)/(5)],[0,-(2)/(5),-(42)/(5),(4)/(5)],[2,3,5,0],[3,4,-3,1]]]:}],[{:[R_(3)larrR_(3)-2xxR_(1)],[=[[1,(7)/(5),(2)/(5),(1)/(5)],[0,-(2)/(5),-(42)/(5),(4)/(5)],[0,(1)/(5),(21)/(5),-(2)/(5)],[3,4,-3,1]]]:}]:}\begin{aligned} &\begin{aligned} & R_2 \leftarrow R_2-R_1 \\ & =\left[\begin{array}{cccc} 1 & \frac{7}{5} & \frac{2}{5} & \frac{1}{5} \\ 0 & -\frac{2}{5} & -\frac{42}{5} & \frac{4}{5} \\ 2 & 3 & 5 & 0 \\ 3 & 4 & -3 & 1 \end{array}\right] \end{aligned}\\ &\begin{aligned} & R_3 \leftarrow R_3-2 \times R_1 \\ & =\left[\begin{array}{cccc} 1 & \frac{7}{5} & \frac{2}{5} & \frac{1}{5} \\ 0 & -\frac{2}{5} & -\frac{42}{5} & \frac{4}{5} \\ 0 & \frac{1}{5} & \frac{21}{5} & -\frac{2}{5} \\ 3 & 4 & -3 & 1 \end{array}\right] \end{aligned} \end{aligned}R2R2R1=[17525150254254523503431]R3R32×R1=[175251502542545015215253431]
R 4 R 4 3 × R 1 = [ 1 7 5 2 5 1 5 0 2 5 42 5 4 5 0 1 5 21 5 2 5 0 1 5 21 5 2 5 ] R 4 R 4 3 × R 1 = 1 7 5 2 5 1 5 0 2 5 42 5 4 5 0 1 5 21 5 2 5 0 1 5 21 5 2 5 {:[R_(4)larrR_(4)-3xxR_(1)],[=[[1,(7)/(5),(2)/(5),(1)/(5)],[0,-(2)/(5),-(42)/(5),(4)/(5)],[0,(1)/(5),(21)/(5),-(2)/(5)],[0,-(1)/(5),-(21)/(5),(2)/(5)]]]:}\begin{aligned} & R_4 \leftarrow R_4-3 \times R_1 \\ & =\left[\begin{array}{cccc} 1 & \frac{7}{5} & \frac{2}{5} & \frac{1}{5} \\ 0 & -\frac{2}{5} & -\frac{42}{5} & \frac{4}{5} \\ 0 & \frac{1}{5} & \frac{21}{5} & -\frac{2}{5} \\ 0 & -\frac{1}{5} & -\frac{21}{5} & \frac{2}{5} \end{array}\right] \end{aligned}R4R43×R1=[1752515025425450152152501521525]
R 2 R 2 × 5 2 = [ 1 7 5 2 5 1 5 0 1 21 2 0 1 5 21 5 2 5 0 1 5 21 5 2 5 ] R 3 R 3 1 5 × R 2 = [ 1 7 5 2 5 1 5 0 1 21 2 0 0 0 0 0 1 5 21 5 2 5 ] R 2 R 2 × 5 2 = 1 7 5 2 5 1 5 0 1 21 2 0 1 5 21 5 2 5 0 1 5 21 5 2 5 R 3 R 3 1 5 × R 2 = 1 7 5 2 5 1 5 0 1 21 2 0 0 0 0 0 1 5 21 5 2 5 {:[R_(2)larrR_(2)xx-(5)/(2)],[=[[1,(7)/(5),(2)/(5),(1)/(5)],[0,1,21,-2],[0,(1)/(5),(21)/(5),-(2)/(5)],[0,-(1)/(5),-(21)/(5),(2)/(5)]]],[R_(3)larrR_(3)-(1)/(5)xxR_(2)],[=[[1,(7)/(5),(2)/(5),(1)/(5)],[0,1,21,-2],[0,0,0,0],[0,-(1)/(5),-(21)/(5),(2)/(5)]]],[]:}\begin{aligned} & R_2 \leftarrow R_2 \times-\frac{5}{2} \\ & =\left[\begin{array}{cccc} 1 & \frac{7}{5} & \frac{2}{5} & \frac{1}{5} \\ 0 & 1 & 21 & -2 \\ 0 & \frac{1}{5} & \frac{21}{5} & -\frac{2}{5} \\ 0 & -\frac{1}{5} & -\frac{21}{5} & \frac{2}{5} \end{array}\right] \\ & R_3 \leftarrow R_3-\frac{1}{5} \times R_2 \\ & =\left[\begin{array}{cccc} 1 & \frac{7}{5} & \frac{2}{5} & \frac{1}{5} \\ 0 & 1 & 21 & -2 \\ 0 & 0 & 0 & 0 \\ 0 & -\frac{1}{5} & -\frac{21}{5} & \frac{2}{5} \end{array}\right] \\ & \end{aligned}R2R2×52=[1752515012120152152501521525]R3R315×R2=[175251501212000001521525]
R 4 R 4 + 1 5 × R 2 = [ 1 7 5 2 5 1 5 0 1 21 2 0 0 0 0 0 0 0 0 ] R 4 R 4 + 1 5 × R 2 = 1 7 5 2 5 1 5 0 1 21 2 0 0 0 0 0 0 0 0 {:[R_(4)larrR_(4)+(1)/(5)xxR_(2)],[=[[1,(7)/(5),(2)/(5),(1)/(5)],[0,1,21,-2],[0,0,0,0],[0,0,0,0]]]:}\begin{gathered} R_4 \leftarrow R_4+\frac{1}{5} \times R_2 \\ =\left[\begin{array}{cccc} 1 & \frac{7}{5} & \frac{2}{5} & \frac{1}{5} \\ 0 & 1 & 21 & -2 \\ 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 \end{array}\right] \end{gathered}R4R4+15×R2=[17525150121200000000]
The rank of a matrix is the number of non all-zeros rows
Rank = 2 Rank = 2 :.” Rank “=2\therefore \text { Rank }=2 Rank =2
(ii) Find the dimension of the subspace V V VVV
The dimension of the subspace V V VVV is related to the rank of A A AAA by the formula:
Dimension of V = n Rank ( A ) V = n Rank ( A ) V=n-Rank(A)V=n-\operatorname{Rank}(A)V=nRank(A)
Here, n n nnn is the number of columns in A A AAA, which is 4 .
Dimension of V = 4 2 = 2 V = 4 2 = 2 V=4-2=2V=4-2=2V=42=2
  1. (a) कैले-हैमिल्टन प्रमेय का कथन लिखिए। इस प्रमेय का उपयोग करके A 100 A 100 A^(100)A^{100}A100 का मान ज्ञात कीजिए, जहाँ
A = [ 1 0 0 1 0 1 0 1 0 ] A = 1      0      0 1      0      1 0      1      0 A=[[1,0,0],[1,0,1],[0,1,0]]A=\left[\begin{array}{lll} 1 & 0 & 0 \\ 1 & 0 & 1 \\ 0 & 1 & 0 \end{array}\right]A=[100101010]
State the Cayley-Hamilton theorem. Use this theorem to find A 100 A 100 A^(100)A^{100}A100, where
A = [ 1 0 0 1 0 1 0 1 0 ] A = 1      0      0 1      0      1 0      1      0 A=[[1,0,0],[1,0,1],[0,1,0]]A=\left[\begin{array}{lll} 1 & 0 & 0 \\ 1 & 0 & 1 \\ 0 & 1 & 0 \end{array}\right]A=[100101010]
Answer:
Cayley-Hamilton Theorem:
The Cayley-Hamilton theorem states that every square matrix satisfies its own characteristic equation over a commutative ring, such as the real or complex field. In other words, if λ I A λ I A lambda I-A\lambda I – AλIA is the characteristic equation of a matrix A A AAA, where I I III is the identity matrix and λ λ lambda\lambdaλ is a scalar, then A A AAA satisfies the equation | λ I A | = 0 | λ I A | = 0 |lambda I-A|=0|\lambda I – A| = 0|λIA|=0.
  1. First, let’s find the characteristic equation for matrix A A AAA:
| λ I A | = | λ 1 0 0 1 λ 1 0 1 λ | = ( λ 1 ) | λ 1 1 λ | = ( λ 1 ) ( λ 2 1 ) = ( λ 1 ) ( λ + 1 ) ( λ 1 ) | λ I A | = λ 1 0 0 1 λ 1 0 1 λ = ( λ 1 ) λ 1 1 λ = ( λ 1 ) ( λ 2 1 ) = ( λ 1 ) ( λ + 1 ) ( λ 1 ) {:[|lambda I-A|=|[lambda-1,0,0],[-1,lambda,-1],[0,-1,lambda]|],[=(lambda-1)|[lambda,-1],[-1,lambda]|],[=(lambda-1)(lambda^(2)-1)],[=(lambda-1)(lambda+1)(lambda-1)]:}\begin{aligned} |\lambda I – A| &= \left|\begin{array}{ccc} \lambda – 1 & 0 & 0 \\ -1 & \lambda & -1 \\ 0 & -1 & \lambda \end{array}\right| \\ &= (\lambda – 1) \left|\begin{array}{cc} \lambda & -1 \\ -1 & \lambda \end{array}\right| \\ &= (\lambda – 1)(\lambda^2 – 1) \\ &= (\lambda – 1)(\lambda + 1)(\lambda – 1) \end{aligned}|λIA|=|λ1001λ101λ|=(λ1)|λ11λ|=(λ1)(λ21)=(λ1)(λ+1)(λ1)
  1. Now, according to the Cayley-Hamilton theorem, A A AAA satisfies its characteristic equation, so A A AAA satisfies:
A 3 A 2 A + I = 0 A 3 A 2 A + I = 0 A^(3)-A^(2)-A+I=0A^3 – A^2 – A + I = 0A3A2A+I=0
  1. Rearranging the equation, we find:
A 3 = A 2 + A I A 3 = A 2 + A I A^(3)=A^(2)+A-IA^3 = A^2 + A – IA3=A2+AI
  1. We can now calculate higher powers of A A AAA based on this result:
A 4 = A 3 + A 2 A = ( A 2 + A I ) + A 2 A = 2 A 2 I A 4 = A 3 + A 2 A = ( A 2 + A I ) + A 2 A = 2 A 2 I {:[A^(4)=A^(3)+A^(2)-A],[=(A^(2)+A-I)+A^(2)-A],[=2A^(2)-I]:}\begin{aligned} A^4 &= A^3 + A^2 – A \\ &= (A^2 + A – I) + A^2 – A \\ &= 2A^2 – I \end{aligned}A4=A3+A2A=(A2+AI)+A2A=2A2I
  1. Similarly, we can find A 5 A 5 A^(5)A^5A5 as:
A 5 = 2 A 3 A = 2 ( A 2 + A I ) A = 2 A 2 + 2 A 2 I A = 2 A 2 + A 2 I A 5 = 2 A 3 A = 2 ( A 2 + A I ) A = 2 A 2 + 2 A 2 I A = 2 A 2 + A 2 I {:[A^(5)=2A^(3)-A],[=2(A^(2)+A-I)-A],[=2A^(2)+2A-2I-A],[=2A^(2)+A-2I]:}\begin{aligned} A^5 &= 2A^3 – A \\ &= 2(A^2 + A – I) – A \\ &= 2A^2 + 2A – 2I – A \\ &= 2A^2 + A – 2I \end{aligned}A5=2A3A=2(A2+AI)A=2A2+2A2IA=2A2+A2I
  1. Continuing this pattern, we find:
A 6 = 3 A 2 2 I A 6 = 3 A 2 2 I A^(6)=3A^(2)-2IA^6 = 3A^2 – 2IA6=3A22I

Use the General Form A 2 n = n A 2 ( n 1 ) I A 2 n = n A 2 ( n 1 ) I A^(2n)=nA^(2)-(n-1)IA^{2n} = n A^2 – (n – 1) IA2n=nA2(n1)I

The general form A 2 n = n A 2 ( n 1 ) I A 2 n = n A 2 ( n 1 ) I A^(2n)=nA^(2)-(n-1)IA^{2n} = n A^2 – (n – 1) IA2n=nA2(n1)I can be used to find A 100 A 100 A^(100)A^{100}A100.
For n = 50 n = 50 n=50n = 50n=50, the expression becomes:
A 100 = 50 A 2 49 I A 100 = 50 A 2 49 I A^(100)=50A^(2)-49 IA^{100} = 50 A^2 – 49 IA100=50A249I

Substitute the Values

Let’s substitute the values of A 2 A 2 A^(2)A^2A2 and I I III into the formula:
A 2 = [ 1 0 0 1 1 0 1 0 1 ] A 2 = 1      0      0 1      1      0 1      0      1 A^(2)=[[1,0,0],[1,1,0],[1,0,1]]A^2 = \left[\begin{array}{lll} 1 & 0 & 0 \\ 1 & 1 & 0 \\ 1 & 0 & 1 \end{array}\right]A2=[100110101]
I = [ 1 0 0 0 1 0 0 0 1 ] I = 1      0      0 0      1      0 0      0      1 I=[[1,0,0],[0,1,0],[0,0,1]]I = \left[\begin{array}{lll} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end{array}\right]I=[100010001]
After substituting, we get:
A 100 = 50 [ 1 0 0 1 1 0 1 0 1 ] 49 [ 1 0 0 0 1 0 0 0 1 ] A 100 = 50 1      0      0 1      1      0 1      0      1 49 1      0      0 0      1      0 0      0      1 A^(100)=50[[1,0,0],[1,1,0],[1,0,1]]-49[[1,0,0],[0,1,0],[0,0,1]]A^{100} = 50 \left[\begin{array}{lll} 1 & 0 & 0 \\ 1 & 1 & 0 \\ 1 & 0 & 1 \end{array}\right] – 49 \left[\begin{array}{lll} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end{array}\right]A100=50[100110101]49[100010001]

Calculate A 100 A 100 A^(100)A^{100}A100

After calculating, we find that A 100 A 100 A^(100)A^{100}A100 is:
A 100 = [ 1 0 0 50 1 0 50 0 1 ] A 100 = 1      0      0 50      1      0 50      0      1 A^(100)=[[1,0,0],[50,1,0],[50,0,1]]A^{100} = \left[\begin{array}{lll} 1 & 0 & 0 \\ 50 & 1 & 0 \\ 50 & 0 & 1 \end{array}\right]A100=[10050105001]

Conclusion

Using the general form A 2 n = n A 2 ( n 1 ) I A 2 n = n A 2 ( n 1 ) I A^(2n)=nA^(2)-(n-1)IA^{2n} = n A^2 – (n – 1) IA2n=nA2(n1)I, we found that A 100 A 100 A^(100)A^{100}A100 for the given matrix A A AAA is:
A 100 = [ 1 0 0 50 1 0 50 0 1 ] A 100 = 1      0      0 50      1      0 50      0      1 A^(100)=[[1,0,0],[50,1,0],[50,0,1]]A^{100} = \left[\begin{array}{lll} 1 & 0 & 0 \\ 50 & 1 & 0 \\ 50 & 0 & 1 \end{array}\right]A100=[10050105001]
(b) बिंदु P P PPP से गुजरने वाली दीर्घवृत्तज
x 2 a 2 + y 2 b 2 + z 2 c 2 = 1 x 2 a 2 + y 2 b 2 + z 2 c 2 = 1 (x^(2))/(a^(2))+(y^(2))/(b^(2))+(z^(2))/(c^(2))=1\frac{x^2}{a^2}+\frac{y^2}{b^2}+\frac{z^2}{c^2}=1x2a2+y2b2+z2c2=1
की अभिलंब जीवा की लंबाई ज्ञात कीजिए और सिद्ध कीजिए कि अगर यह 4 P G 3 4 P G 3 4PG_(3)4 P G_34PG3 के समान है, जहाँ G 3 G 3 G_(3)G_3G3 वह बिंदु है जहाँ P P PPP से गुजरने वाली अभिलंब जीवा x y x y xyx yxy-तल पर मिलती है, तो P P PPP शंकु
x 2 a 6 ( 2 c 2 a 2 ) + y 2 b 6 ( 2 c 2 b 2 ) + z 2 c 4 = 0 x 2 a 6 2 c 2 a 2 + y 2 b 6 2 c 2 b 2 + z 2 c 4 = 0 (x^(2))/(a^(6))(2c^(2)-a^(2))+(y^(2))/(b^(6))(2c^(2)-b^(2))+(z^(2))/(c^(4))=0\frac{x^2}{a^6}\left(2 c^2-a^2\right)+\frac{y^2}{b^6}\left(2 c^2-b^2\right)+\frac{z^2}{c^4}=0x2a6(2c2a2)+y2b6(2c2b2)+z2c4=0
पर स्थित है।
Find the length of the normal chord through a point P P PPP of the ellipsoid
x 2 a 2 + y 2 b 2 + z 2 c 2 = 1 x 2 a 2 + y 2 b 2 + z 2 c 2 = 1 (x^(2))/(a^(2))+(y^(2))/(b^(2))+(z^(2))/(c^(2))=1\frac{x^2}{a^2}+\frac{y^2}{b^2}+\frac{z^2}{c^2}=1x2a2+y2b2+z2c2=1
and prove that if it is equal to 4 P G 3 4 P G 3 4PG_(3)4 P G_34PG3, where G 3 G 3 G_(3)G_3G3 is the point where the normal chord through P P PPP meets the x y x y xyx yxy-plane, then P P PPP lies on the cone
x 2 a 6 ( 2 c 2 a 2 ) + y 2 b 6 ( 2 c 2 b 2 ) + z 2 c 4 = 0 x 2 a 6 2 c 2 a 2 + y 2 b 6 2 c 2 b 2 + z 2 c 4 = 0 (x^(2))/(a^(6))(2c^(2)-a^(2))+(y^(2))/(b^(6))(2c^(2)-b^(2))+(z^(2))/(c^(4))=0\frac{x^2}{a^6}\left(2 c^2-a^2\right)+\frac{y^2}{b^6}\left(2 c^2-b^2\right)+\frac{z^2}{c^4}=0x2a6(2c2a2)+y2b6(2c2b2)+z2c4=0
Answer:
Equation of the Normal:
Let P P P\mathrm{P}P be ( α , β , γ ) ( α , β , γ ) (alpha,beta,gamma)(\alpha, \beta, \gamma)(α,β,γ), then the equation of the normal to the given ellipsoid at P ( α , β , γ ) P ( α , β , γ ) P(alpha,beta,gamma)P(\alpha, \beta, \gamma)P(α,β,γ) are
x α p α a 2 = y β P β b 2 = z r P γ c 2 = r ( 1 ) where 1 P 2 = α 2 a 4 + β 2 b 4 + γ 2 c 4 (2) x α p α a 2 = y β P β b 2 = z r P γ c 2 = r ( 1 ) where 1 P 2 = α 2 a 4 + β 2 b 4 + γ 2 c 4 (2) (x-alpha)/((p alpha)/(a^(2)))=(y-beta)/((P beta)/(b^(2)))=(z-r)/((P gamma)/(c^(2)))=r rarr(1)” where “(1)/(P^(2))=(alpha^(2))/(a^(4))+(beta^(2))/(b^(4))+(gamma^(2))/(c^(4))rarr” (2) “\frac{x-\alpha}{\frac{p \alpha}{a^2}}=\frac{y-\beta}{\frac{P \beta}{b^2}}=\frac{z-r}{\frac{P \gamma}{c^2}}=r \rightarrow(1) \text { where } \frac{1}{P^2}=\frac{\alpha^2}{a^4}+\frac{\beta^2}{b^4}+\frac{\gamma^2}{c^4} \rightarrow \text { (2) }xαpαa2=yβPβb2=zrPγc2=r(1) where 1P2=α2a4+β2b4+γ2c4 (2)
Therefore, the coordinates of any point Q Q QQQ on the normal (1) are ( α + P α a 2 r , β + P β b 2 r , γ + p γ c 2 r ) α + P α a 2 r , β + P β b 2 r , γ + p γ c 2 r (alpha+(P alpha)/(a^(2))r,beta+(P beta)/(b^(2))r,gamma+(p gamma)/(c^(2))r)\left(\alpha+\frac{P \alpha}{a^2} r, \beta+\frac{P \beta}{b^2} r, \gamma+\frac{p \gamma}{c^2} r\right)(α+Pαa2r,β+Pβb2r,γ+pγc2r), where r r rrr is the distance of Q Q QQQ from P P PPP.
If Q Q Q\mathrm{Q}Q lies on the given ellipsoid i.e., PQ PQ PQ\mathrm{PQ}PQ is the normal chord, then
1 a 2 ( α + p α a 2 r ) 2 + 1 b 2 ( β + p β b 2 r ) 2 + 1 c 2 ( γ + p γ c 2 r ) 2 = 1 r 2 P 2 ( α 2 a 6 + β 2 b 6 + γ 2 c 6 ) + 2 r P ( α 2 a 4 + β 2 b 4 + γ 2 c 4 ) + ( α 2 a 2 + β 2 b 2 + γ 2 c 2 ) = 1 1 a 2 α + p α a 2 r 2 + 1 b 2 β + p β b 2 r 2 + 1 c 2 γ + p γ c 2 r 2 = 1 r 2 P 2 α 2 a 6 + β 2 b 6 + γ 2 c 6 + 2 r P α 2 a 4 + β 2 b 4 + γ 2 c 4 + α 2 a 2 + β 2 b 2 + γ 2 c 2 = 1 {:[(1)/(a^(2))(alpha+(p alpha)/(a^(2))r)^(2)+(1)/(b^(2))(beta+(p beta)/(b^(2))r)^(2)+(1)/(c^(2))(gamma+(p gamma)/(c^(2))r)^(2)=1],[=>r^(2)P^(2)((alpha^(2))/(a^(6))+(beta^(2))/(b^(6))+(gamma^(2))/(c^(6)))+2rP((alpha^(2))/(a^(4))+(beta^(2))/(b^(4))+(gamma^(2))/(c^(4)))+((alpha^(2))/(a^(2))+(beta^(2))/(b^(2))+(gamma^(2))/(c^(2)))=1]:}\begin{aligned} & \frac{1}{a^2}\left(\alpha+\frac{p \alpha}{a^2} r\right)^2+\frac{1}{b^2}\left(\beta+\frac{p \beta}{b^2} r\right)^2+\frac{1}{c^2}\left(\gamma+\frac{p \gamma}{c^2} r\right)^2=1 \\ & \Rightarrow r^2 P^2\left(\frac{\alpha^2}{a^6}+\frac{\beta^2}{b^6}+\frac{\gamma^2}{c^6}\right)+2 r P\left(\frac{\alpha^2}{a^4}+\frac{\beta^2}{b^4}+\frac{\gamma^2}{c^4}\right)+\left(\frac{\alpha^2}{a^2}+\frac{\beta^2}{b^2}+\frac{\gamma^2}{c^2}\right)=1 \end{aligned}1a2(α+pαa2r)2+1b2(β+pβb2r)2+1c2(γ+pγc2r)2=1r2P2(α2a6+β2b6+γ2c6)+2rP(α2a4+β2b4+γ2c4)+(α2a2+β2b2+γ2c2)=1
r 2 p 2 ( α 2 a 4 + β 2 b 6 + γ 2 c 6 ) + 2 r p ( 1 p 2 ) = 0 [ r 2 p 2 α 2 a 4 + β 2 b 6 + γ 2 c 6 + 2 r p 1 p 2 = 0 =>r^(2)p^(2)((alpha^(2))/(a^(4))+(beta^(2))/(b^(6))+(gamma^(2))/(c^(6)))+2rp((1)/(p^(2)))=0[:}\Rightarrow r^2 p^2\left(\frac{\alpha^2}{a^4}+\frac{\beta^2}{b^6}+\frac{\gamma^2}{c^6}\right)+2 r p\left(\frac{1}{p^2}\right)=0\left[\right.r2p2(α2a4+β2b6+γ2c6)+2rp(1p2)=0[ from (2) and Σ ( α 2 a 2 ) = 1 Σ α 2 a 2 = 1 Sigma((alpha^(2))/(a^(2)))=1\Sigma\left(\frac{\alpha^2}{a^2}\right)=1Σ(α2a2)=1 as p ( α , β , γ ) p ( α , β , γ ) p(alpha,beta,gamma)p(\alpha, \beta, \gamma)p(α,β,γ) lies on the given conicoid ]
r = 2 p 3 ( α 2 a 6 + β 2 b 6 + γ 2 c 6 ) = length of normal chord P Q ( 3 ) r = 2 p 3 α 2 a 6 + β 2 b 6 + γ 2 c 6 = length of normal chord P Q ( 3 ) =>r=-(2)/(p^(3)((alpha^(2))/(a^(6))+(beta^(2))/(b^(6))+(gamma^(2))/(c^(6))))=” length of normal chord “PQ rarr(3)\Rightarrow r=-\frac{2}{p^3\left(\frac{\alpha^2}{a^6}+\frac{\beta^2}{b^6}+\frac{\gamma^2}{c^6}\right)}=\text { length of normal chord } P Q \rightarrow(3)r=2p3(α2a6+β2b6+γ2c6)= length of normal chord PQ(3)
Also,
Let the normal at P ( α , β , γ ) P ( α , β , γ ) P(alpha,beta,gamma)P(\alpha, \beta, \gamma)P(α,β,γ) meets the coordinate plane viz. y z , z x y z , z x yz,zxy z, z xyz,zx and x y x y xyx yxy planes at G 1 , G 2 , G 3 G 1 , G 2 , G 3 G_(1),G_(2),G_(3)G_1, G_2, G_3G1,G2,G3 Then putting x = 0 , y = 0 x = 0 , y = 0 x=0,y=0x=0, y=0x=0,y=0 and z = 0 z = 0 z=0z=0z=0 in succession in the equation (1), we have respectively,
P G 1 = a 2 P , P G 2 = b 2 p and P G 3 = c 2 p (4) P G 1 = a 2 P , P G 2 = b 2 p and P G 3 = c 2 p (4) PG_(1)=-(a^(2))/(P),PG_(2)=-(b^(2))/(p)” and “PG_(3)=-(c^(2))/(p)rarr” (4) “P G_1=-\frac{a^2}{P}, P G_2=-\frac{b^2}{p} \text { and } P G_3=-\frac{c^2}{p} \rightarrow \text { (4) }PG1=a2P,PG2=b2p and PG3=c2p (4)
Given, P Q = 4 P G 3 P Q = 4 P G 3 PQ=4PG_(3)P Q=4 P G_3PQ=4PG3
p Q = 4 ( c 2 p ) r = 2 p 3 ( α 2 a 6 + β 2 b 6 + γ 2 c 6 ) = 4 ( c 2 p ) 2 c 2 ( α 2 a 6 + β 2 b 6 + γ 2 c 6 ) = 1 p 2 = ( α 2 a 4 + β 2 b 4 + γ 2 c 4 ) from ( 2 ) α 2 a 6 ( 2 c 2 a 2 ) + β 2 b 2 ( 2 c 2 b 2 ) + γ 2 c 6 ( 2 c 2 c 2 ) = 0 α 2 a 6 ( 2 c 2 a 2 ) + β 2 b 2 ( 2 c 2 b 2 ) + γ 2 c 6 ( c 2 ) = 0 α 2 a 6 ( 2 c 2 a 2 ) + β 2 b 2 ( 2 c 2 b 2 ) + γ 2 c 4 = 0 p Q = 4 c 2 p r = 2 p 3 α 2 a 6 + β 2 b 6 + γ 2 c 6 = 4 c 2 p 2 c 2 α 2 a 6 + β 2 b 6 + γ 2 c 6 = 1 p 2 = α 2 a 4 + β 2 b 4 + γ 2 c 4 from ( 2 ) α 2 a 6 2 c 2 a 2 + β 2 b 2 2 c 2 b 2 + γ 2 c 6 2 c 2 c 2 = 0 α 2 a 6 2 c 2 a 2 + β 2 b 2 2 c 2 b 2 + γ 2 c 6 c 2 = 0 α 2 a 6 2 c 2 a 2 + β 2 b 2 2 c 2 b 2 + γ 2 c 4 = 0 {:[=>pQ=4(-(c^(2))/(p))],[=>r=-(2)/(p^(3)((alpha^(2))/(a^(6))+(beta^(2))/(b^(6))+(gamma^(2))/(c^(6))))=4(-(c^(2))/(p))],[=>2c^(2)((alpha^(2))/(a^(6))+(beta^(2))/(b^(6))+(gamma^(2))/(c^(6)))=(1)/(p^(2))],[=((alpha^(2))/(a^(4))+(beta^(2))/(b^(4))+(gamma^(2))/(c^(4)))rarr” from “(2)],[=>(alpha^(2))/(a^(6))(2c^(2)-a^(2))+(beta^(2))/(b^(2))(2c^(2)-b^(2))+(gamma^(2))/(c^(6))(2c^(2)-c^(2))=0],[=>(alpha^(2))/(a^(6))(2c^(2)-a^(2))+(beta^(2))/(b^(2))(2c^(2)-b^(2))+(gamma^(2))/(c^(6))(c^(2))=0],[=>(alpha^(2))/(a^(6))(2c^(2)-a^(2))+(beta^(2))/(b^(2))(2c^(2)-b^(2))+(gamma^(2))/(c^(4))=0]:}\begin{aligned} & \Rightarrow p Q=4\left(-\frac{c^2}{p}\right) \\ & \Rightarrow r=-\frac{2}{p^3\left(\frac{\alpha^2}{a^6}+\frac{\beta^2}{b^6}+\frac{\gamma^2}{c^6}\right)}=4\left(-\frac{c^2}{p}\right) \\ & \Rightarrow 2 c^2\left(\frac{\alpha^2}{a^6}+\frac{\beta^2}{b^6}+\frac{\gamma^2}{c^6}\right)=\frac{1}{p^2} \\ & =\left(\frac{\alpha^2}{a^4}+\frac{\beta^2}{b^4}+\frac{\gamma^2}{c^4}\right) \rightarrow \text { from }(2) \\ & \Rightarrow \frac{\alpha^2}{a^6}\left(2 c^2-a^2\right)+\frac{\beta^2}{b^2}\left(2 c^2-b^2\right)+\frac{\gamma^2}{c^6}\left(2 c^2-c^2\right)=0\\ & \Rightarrow \frac{\alpha^2}{a^6}\left(2 c^2-a^2\right)+\frac{\beta^2}{b^2}\left(2 c^2-b^2\right)+\frac{\gamma^2}{c^6}\left(c^2\right)=0\\ & \Rightarrow \frac{\alpha^2}{a^6}\left(2 c^2-a^2\right)+\frac{\beta^2}{b^2}\left(2 c^2-b^2\right)+\frac{\gamma^2}{c^4}=0 \end{aligned}pQ=4(c2p)r=2p3(α2a6+β2b6+γ2c6)=4(c2p)2c2(α2a6+β2b6+γ2c6)=1p2=(α2a4+β2b4+γ2c4) from (2)α2a6(2c2a2)+β2b2(2c2b2)+γ2c6(2c2c2)=0α2a6(2c2a2)+β2b2(2c2b2)+γ2c6(c2)=0α2a6(2c2a2)+β2b2(2c2b2)+γ2c4=0
Conclusion:
We have found the length of the normal chord through a point P P PPP on the given ellipsoid and proved that if this length is equal to 4 P G 3 4 P G 3 4PG_(3)4PG_34PG3, then P P PPP lies on the cone defined by the equation
α 2 a 6 ( 2 c 2 a 2 ) + β 2 b 2 ( 2 c 2 b 2 ) + γ 2 c 4 = 0 α 2 a 6 2 c 2 a 2 + β 2 b 2 2 c 2 b 2 + γ 2 c 4 = 0 (alpha^(2))/(a^(6))(2c^(2)-a^(2))+(beta^(2))/(b^(2))(2c^(2)-b^(2))+(gamma^(2))/(c^(4))=0\frac{\alpha^2}{a^6}\left(2 c^2-a^2\right)+\frac{\beta^2}{b^2}\left(2 c^2-b^2\right)+\frac{\gamma^2}{c^4}=0α2a6(2c2a2)+β2b2(2c2b2)+γ2c4=0
Hence proved.
(c) (i) अगर
u = sin 1 x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 u = sin 1 x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 u=sin^(-1)sqrt((x^(1//3)+y^(1//3))/(x^(1//2)+y^(1//2)))u=\sin ^{-1} \sqrt{\frac{x^{1 / 3}+y^{1 / 3}}{x^{1 / 2}+y^{1 / 2}}}u=sin1x1/3+y1/3x1/2+y1/2
है, तो दर्शाइए कि sin 2 u , x sin 2 u , x sin^(2)u,x\sin ^2 u, xsin2u,x और y y yyy का 1 6 1 6 -(1)/(6)-\frac{1}{6}16 घातविशिष्ट समांगी फलन है। अतएव दर्शाइए कि
x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 = tan u 12 ( 13 12 + tan 2 u 12 ) x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 = tan u 12 13 12 + tan 2 u 12 x^(2)(del^(2)u)/(delx^(2))+2xy(del^(2)u)/(del x del y)+y^(2)(del^(2)u)/(dely^(2))=(tan u)/(12)((13)/(12)+(tan^(2)u)/(12))x^2 \frac{\partial^2 u}{\partial x^2}+2 x y \frac{\partial^2 u}{\partial x \partial y}+y^2 \frac{\partial^2 u}{\partial y^2}=\frac{\tan u}{12}\left(\frac{13}{12}+\frac{\tan ^2 u}{12}\right)x22ux2+2xy2uxy+y22uy2=tanu12(1312+tan2u12)
(ii) जैकोबियन विधि का व्यवहार करते हुए दर्शाइए कि अगर f ( x ) = 1 1 + x 2 f ( x ) = 1 1 + x 2 f^(‘)(x)=(1)/(1+x^(2))f^{\prime}(x)=\frac{1}{1+x^2}f(x)=11+x2 और f ( 0 ) = 0 f ( 0 ) = 0 f(0)=0f(0)=0f(0)=0 है, तो
f ( x ) + f ( y ) = f ( x + y 1 x y ) f ( x ) + f ( y ) = f x + y 1 x y f(x)+f(y)=f((x+y)/(1-xy))f(x)+f(y)=f\left(\frac{x+y}{1-x y}\right)f(x)+f(y)=f(x+y1xy)
(i) If
u = sin 1 x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 u = sin 1 x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 u=sin^(-1)sqrt((x^(1//3)+y^(1//3))/(x^(1//2)+y^(1//2)))u=\sin ^{-1} \sqrt{\frac{x^{1 / 3}+y^{1 / 3}}{x^{1 / 2}+y^{1 / 2}}}u=sin1x1/3+y1/3x1/2+y1/2
then show that sin 2 u sin 2 u sin^(2)u\sin ^2 usin2u is a homogeneous function of x x xxx and y y yyy of degree 1 6 1 6 -(1)/(6)-\frac{1}{6}16.
Hence show that
x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 = tan u 12 ( 13 12 + tan 2 u 12 ) x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 = tan u 12 13 12 + tan 2 u 12 x^(2)(del^(2)u)/(delx^(2))+2xy(del^(2)u)/(del x del y)+y^(2)(del^(2)u)/(dely^(2))=(tan u)/(12)((13)/(12)+(tan^(2)u)/(12))x^2 \frac{\partial^2 u}{\partial x^2}+2 x y \frac{\partial^2 u}{\partial x \partial y}+y^2 \frac{\partial^2 u}{\partial y^2}=\frac{\tan u}{12}\left(\frac{13}{12}+\frac{\tan ^2 u}{12}\right)x22ux2+2xy2uxy+y22uy2=tanu12(1312+tan2u12)
Answer:
Introduction:
We are given the equation u = sin 1 x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 u = sin 1 x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 u=sin^(-1)sqrt((x^(1//3)+y^(1//3))/(x^(1//2)+y^(1//2)))u=\sin ^{-1} \sqrt{\frac{x^{1 / 3}+y^{1 / 3}}{x^{1 / 2}+y^{1 / 2}}}u=sin1x1/3+y1/3x1/2+y1/2 and asked to show that sin 2 u sin 2 u sin^(2)u\sin ^2 usin2u is a homogeneous function of x x xxx and y y yyy of degree 1 6 1 6 -(1)/(6)-\frac{1}{6}16. Additionally, we need to demonstrate that
x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 = tan u 12 ( 13 12 + tan 2 u 12 ) x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 = tan u 12 13 12 + tan 2 u 12 x^(2)(del^(2)u)/(delx^(2))+2xy(del^(2)u)/(del x del y)+y^(2)(del^(2)u)/(dely^(2))=(tan u)/(12)((13)/(12)+(tan^(2)u)/(12))x^2 \frac{\partial^2 u}{\partial x^2}+2 x y \frac{\partial^2 u}{\partial x \partial y}+y^2 \frac{\partial^2 u}{\partial y^2}=\frac{\tan u}{12}\left(\frac{13}{12}+\frac{\tan ^2 u}{12}\right)x22ux2+2xy2uxy+y22uy2=tanu12(1312+tan2u12)
Homogeneity Analysis:
Step 1: Defining f f fff and Finding Degree of Homogeneity):
Let’s start by defining f = sin u f = sin u f=sin uf=\sin uf=sinu and then find the degree of homogeneity.
f = sin u = x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 f = sin u = x 1 / 3 + y 1 / 3 x 1 / 2 + y 1 / 2 f=sin u=sqrt((x^(1//3)+y^(1//3))/(x^(1//2)+y^(1//2)))f=\sin u= \sqrt{\frac{x^{1 / 3}+y^{1 / 3}}{x^{1 / 2}+y^{1 / 2}}}f=sinu=x1/3+y1/3x1/2+y1/2
The degree of homogeneity is found as:
Degree = 1 3 1 2 = 1 6 Degree = 1 3 1 2 = 1 6 “Degree”=(1)/(3)-(1)/(2)=-(1)/(6)\text{Degree} = \frac{1}{3} – \frac{1}{2} = -\frac{1}{6}Degree=1312=16
Step 2: Expressing f f fff in terms of x x xxx and y y yyy:
Now, we express f f fff in terms of x x xxx and y y yyy:
f = x 1 12 g ( y x ) f = x 1 12 g y x f=x^(-(1)/(12))g((y)/(x))f = x^{-\frac{1}{12}} g\left(\frac{y}{x}\right)f=x112g(yx)
Step 3: Determining Homogeneous Function of u u uuu:
Next, we find sin 2 u sin 2 u sin^(2)u\sin^2 usin2u as a homogeneous function of x x xxx and y y yyy:
sin 2 u = x ( 1 6 ) g ( y x ) sin 2 u = x 1 6 g y x sin^(2)u=x^((-(1)/(6))g((y)/(x)))\sin ^2 u = x^{\left(-\frac{1}{6}\right) g\left(\frac{y}{x}\right)}sin2u=x(16)g(yx)
The degree is confirmed to be 1 6 1 6 -(1)/(6)-\frac{1}{6}16.
Derivatives and Further Analysis:
Step 4: Partial Derivatives:
Now, let’s calculate the partial derivatives f x f x (del f)/(del x)\frac{\partial f}{\partial x}fx and f y f y (del f)/(del y)\frac{\partial f}{\partial y}fy using the homogeneous function properties:
x f x + y f y = n f where n = 1 6 x f x + y f y = n f where n = 1 6 x(del f)/(del x)+y(del f)/(del y)=n*f quad”where”quad n=-(1)/(6)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} = n \cdot f \quad \text{where} \quad n = -\frac{1}{6}xfx+yfy=nfwheren=16
Step 5: Derivative of sin u sin u sin u\sin usinu and Simplification:
Since f = sin u f = sin u f=sin uf = \sin uf=sinu, we differentiate with respect to x x xxx:
x cos u u x + y cos u u y = 1 12 sin u x cos u u x + y cos u u y = 1 12 sin u x cos u(del u)/(del x)+y cos u(del u)/(del y)=-(1)/(12)sin ux \cos u \frac{\partial u}{\partial x} + y \cos u \frac{\partial u}{\partial y} = -\frac{1}{12} \sin uxcosuux+ycosuuy=112sinu
After some simplification and using trigonometric identities, we get:
x u x + y u y = 1 12 tan u x u x + y u y = 1 12 tan u x(del u)/(del x)+y(del u)/(del y)=-(1)/(12)tan ux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = -\frac{1}{12} \tan uxux+yuy=112tanu
Step 6: Second Derivative and Further Simplification:
Differentiate equation 1 partially with respect to x x xxx and y y yyy and add the resulting equations. Then simplify as follows:
x 2 u x 2 + u x + y 2 u x y = 1 12 sec 2 u u x y 2 u y + y u y + 2 x y 2 u x y = ( x u x + y u y ) ( 1 1 12 sec 2 u ) [ 1 + 1 12 ( tan 2 α + 1 ) ] = 1 12 tan u ( 1 + 1 12 sec 2 u ) = tan u 12 ( 13 12 + tan 2 u 12 ) x 2 u x 2 + u x + y 2 u x y = 1 12 sec 2 u u x y 2 u y + y u y + 2 x y 2 u x y = x u x + y u y 1 1 12 sec 2 u 1 + 1 12 tan 2 α + 1 = 1 12 tan u 1 + 1 12 sec 2 u = tan u 12 13 12 + tan 2 u 12 {:[x(del^(2)u)/(delx^(2))+(del u)/(del x)+y(del^(2)u)/(del x del y)=-(1)/(12)sec^(2)u(del u)/(del x)],[y^(2)(del u)/(del y)+y(del u)/(del y)+2xy(del^(2)u)/(del x del y)=(x(del u)/(del x)+y(del u)/(del y))(1-(1)/(12)sec^(2)u)],[[1+(1)/(12)(tan^(2)alpha+1)]=-(1)/(12)tan u(1+(1)/(12)sec^(2)u)],[=(tan u)/(12)((13)/(12)+(tan^(2)u)/(12))]:}\begin{aligned} & x \frac{\partial^2 u}{\partial x^2}+\frac{\partial u}{\partial x}+y \frac{\partial^2 u}{\partial x \partial y}=-\frac{1}{12} \sec ^2 u \frac{\partial u}{\partial x} \\ & y^2 \frac{\partial u}{\partial y}+y \frac{\partial u}{\partial y}+2 x y \frac{\partial^2 u}{\partial x \partial y}=\left(x \frac{\partial u}{\partial x}+y \frac{\partial u}{\partial y}\right)\left(1-\frac{1}{12} \sec ^2 u\right) \\ & {\left[1+\frac{1}{12}\left(\tan ^2 \alpha+1\right)\right]=-\frac{1}{12} \tan u\left(1+\frac{1}{12} \sec ^2 u\right)} \\ & =\frac{\tan u}{12}\left(\frac{13}{12}+\frac{\tan ^2 u}{12}\right) \end{aligned}x2ux2+ux+y2uxy=112sec2uuxy2uy+yuy+2xy2uxy=(xux+yuy)(1112sec2u)[1+112(tan2α+1)]=112tanu(1+112sec2u)=tanu12(1312+tan2u12)
Conclusion:
We have shown that sin 2 u sin 2 u sin^(2)u\sin ^2 usin2u is indeed a homogeneous function of x x xxx and y y yyy with a degree of 1 6 1 6 -(1)/(6)-\frac{1}{6}16. Additionally, we have derived and simplified the expression x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 x 2 2 u x 2 + 2 x y 2 u x y + y 2 2 u y 2 x^(2)(del^(2)u)/(delx^(2))+2xy(del^(2)u)/(del x del y)+y^(2)(del^(2)u)/(dely^(2))x^2 \frac{\partial^2 u}{\partial x^2}+2 x y \frac{\partial^2 u}{\partial x \partial y}+y^2 \frac{\partial^2 u}{\partial y^2}x22ux2+2xy2uxy+y22uy2 as given in the problem statement.
(ii) Using the Jacobian method, show that if f ( x ) = 1 1 + x 2 f ( x ) = 1 1 + x 2 f^(‘)(x)=(1)/(1+x^(2))f^{\prime}(x)=\frac{1}{1+x^2}f(x)=11+x2 and f ( 0 ) = 0 f ( 0 ) = 0 f(0)=0f(0)=0f(0)=0, then
f ( x ) + f ( y ) = f ( x + y 1 x y ) f ( x ) + f ( y ) = f x + y 1 x y f(x)+f(y)=f((x+y)/(1-xy))f(x)+f(y)=f\left(\frac{x+y}{1-x y}\right)f(x)+f(y)=f(x+y1xy)
Answer:

Work/Calculations

Step 1: Integrate f ( x ) f ( x ) f^(‘)(x)f'(x)f(x) to find f ( x ) f ( x ) f(x)f(x)f(x)

Given f ( x ) = 1 1 + x 2 f ( x ) = 1 1 + x 2 f^(‘)(x)=(1)/(1+x^(2))f'(x) = \frac{1}{1 + x^2}f(x)=11+x2, we integrate to find f ( x ) f ( x ) f(x)f(x)f(x):
f ( x ) d x = 1 1 + x 2 d x f ( x ) d x = 1 1 + x 2 d x intf^(‘)(x)dx=int(1)/(1+x^(2))dx\int f'(x) \, dx = \int \frac{1}{1 + x^2} \, dxf(x)dx=11+x2dx
f ( x ) = tan 1 ( x ) + c f ( x ) = tan 1 ( x ) + c f(x)=tan^(-1)(x)+cf(x) = \tan^{-1}(x) + cf(x)=tan1(x)+c
Since f ( 0 ) = 0 f ( 0 ) = 0 f(0)=0f(0) = 0f(0)=0, we find that c = 0 c = 0 c=0c = 0c=0. Therefore, f ( x ) = tan 1 ( x ) f ( x ) = tan 1 ( x ) f(x)=tan^(-1)(x)f(x) = \tan^{-1}(x)f(x)=tan1(x).

Step 2: Define α α alpha\alphaα and β β beta\betaβ

α = f ( x ) + f ( y ) = tan 1 ( x ) + tan 1 ( y ) α = f ( x ) + f ( y ) = tan 1 ( x ) + tan 1 ( y ) alpha=f(x)+f(y)=tan^(-1)(x)+tan^(-1)(y)\alpha = f(x) + f(y) = \tan^{-1}(x) + \tan^{-1}(y)α=f(x)+f(y)=tan1(x)+tan1(y)
β = f ( x + y 1 x y ) = tan 1 ( x + y 1 x y ) β = f x + y 1 x y = tan 1 x + y 1 x y beta=f((x+y)/(1-xy))=tan^(-1)((x+y)/(1-xy))\beta = f\left(\frac{x+y}{1-xy}\right) = \tan^{-1}\left(\frac{x+y}{1-xy}\right)β=f(x+y1xy)=tan1(x+y1xy)

Step 3: Calculate the Partial Derivatives of α α alpha\alphaα and β β beta\betaβ

For α α alpha\alphaα, we have:
α x = 1 1 + x 2 α x = 1 1 + x 2 (del alpha)/(del x)=(1)/(1+x^(2))\frac{\partial \alpha}{\partial x} = \frac{1}{1 + x^2}αx=11+x2
α y = 1 1 + y 2 α y = 1 1 + y 2 (del alpha)/(del y)=(1)/(1+y^(2))\frac{\partial \alpha}{\partial y} = \frac{1}{1 + y^2}αy=11+y2
For β β beta\betaβ, we differentiate β β beta\betaβ with respect to x x xxx:
β x = x [ tan 1 ( x + y 1 x y ) ] β x = x tan 1 x + y 1 x y (del beta)/(del x)=(del)/(del x)[tan^(-1)((x+y)/(1-xy))]\frac{\partial \beta}{\partial x} = \frac{\partial}{\partial x} \left[ \tan^{-1}\left(\frac{x+y}{1-xy}\right) \right]βx=x[tan1(x+y1xy)]
After calculating, we find:
β x = 1 1 + x 2 β x = 1 1 + x 2 (del beta)/(del x)=(1)/(1+x^(2))\frac{\partial \beta}{\partial x} = \frac{1}{1 + x^2}βx=11+x2
Similarly, to find β y β y (del beta)/(del y)\frac{\partial \beta}{\partial y}βy, we differentiate β β beta\betaβ with respect to y y yyy:
β y = y [ tan 1 ( x + y 1 x y ) ] β y = y tan 1 x + y 1 x y (del beta)/(del y)=(del)/(del y)[tan^(-1)((x+y)/(1-xy))]\frac{\partial \beta}{\partial y} = \frac{\partial}{\partial y} \left[ \tan^{-1}\left(\frac{x+y}{1-xy}\right) \right]βy=y[tan1(x+y1xy)]
After calculating, we find:
β y = 1 1 + y 2 β y = 1 1 + y 2 (del beta)/(del y)=(1)/(1+y^(2))\frac{\partial \beta}{\partial y} = \frac{1}{1 + y^2}βy=11+y2

Step 4: Check if the Partial Derivatives are Equal

To prove that f ( x ) + f ( y ) = f ( x + y 1 x y ) f ( x ) + f ( y ) = f x + y 1 x y f(x)+f(y)=f((x+y)/(1-xy))f(x) + f(y) = f\left(\frac{x+y}{1-xy}\right)f(x)+f(y)=f(x+y1xy), it’s sufficient to show that α x = β x α x = β x (del alpha)/(del x)=(del beta)/(del x)\frac{\partial \alpha}{\partial x} = \frac{\partial \beta}{\partial x}αx=βx and α y = β y α y = β y (del alpha)/(del y)=(del beta)/(del y)\frac{\partial \alpha}{\partial y} = \frac{\partial \beta}{\partial y}αy=βy.
Since α x = β x α x = β x (del alpha)/(del x)=(del beta)/(del x)\frac{\partial \alpha}{\partial x} = \frac{\partial \beta}{\partial x}αx=βx and α y = β y α y = β y (del alpha)/(del y)=(del beta)/(del y)\frac{\partial \alpha}{\partial y} = \frac{\partial \beta}{\partial y}αy=βy, we can conclude that f ( x ) + f ( y ) = f ( x + y 1 x y ) f ( x ) + f ( y ) = f x + y 1 x y f(x)+f(y)=f((x+y)/(1-xy))f(x) + f(y) = f\left(\frac{x+y}{1-xy}\right)f(x)+f(y)=f(x+y1xy).

Conclusion with Jacobian Method

In the Jacobian method, we aim to show that two functions α α alpha\alphaα and β β beta\betaβ are equal by proving that their partial derivatives with respect to the same variables are equal. In this case, α = f ( x ) + f ( y ) α = f ( x ) + f ( y ) alpha=f(x)+f(y)\alpha = f(x) + f(y)α=f(x)+f(y) and β = f ( x + y 1 x y ) β = f x + y 1 x y beta=f((x+y)/(1-xy))\beta = f\left(\frac{x+y}{1-xy}\right)β=f(x+y1xy).
We calculated the partial derivatives α x α x (del alpha)/(del x)\frac{\partial \alpha}{\partial x}αx, α y α y (del alpha)/(del y)\frac{\partial \alpha}{\partial y}αy, β x β x (del beta)/(del x)\frac{\partial \beta}{\partial x}βx, and β y β y (del beta)/(del y)\frac{\partial \beta}{\partial y}βy and found:
α x = 1 1 + x 2 = β x α x = 1 1 + x 2 = β x (del alpha)/(del x)=(1)/(1+x^(2))=(del beta)/(del x)\frac{\partial \alpha}{\partial x} = \frac{1}{1 + x^2} = \frac{\partial \beta}{\partial x}αx=11+x2=βx
α y = 1 1 + y 2 = β y α y = 1 1 + y 2 = β y (del alpha)/(del y)=(1)/(1+y^(2))=(del beta)/(del y)\frac{\partial \alpha}{\partial y} = \frac{1}{1 + y^2} = \frac{\partial \beta}{\partial y}αy=11+y2=βy
Since both sets of partial derivatives are equal, the Jacobian method confirms that α α alpha\alphaα and β β beta\betaβ are indeed the same function under the transformation of variables. Therefore, we can conclude that:
f ( x ) + f ( y ) = f ( x + y 1 x y ) f ( x ) + f ( y ) = f x + y 1 x y f(x)+f(y)=f((x+y)/(1-xy))f(x) + f(y) = f\left(\frac{x+y}{1-xy}\right)f(x)+f(y)=f(x+y1xy)
This successfully proves the given equation using the Jacobian method.
खण्ड-B / SECTION-B
  1. (a) अवकल समीकरण
( 2 y sin x + 3 y 4 sin x cos x ) d x ( 4 y 3 cos 2 x + cos x ) d y = 0 2 y sin x + 3 y 4 sin x cos x d x 4 y 3 cos 2 x + cos x d y = 0 (2y sin x+3y^(4)sin x cos x)dx-(4y^(3)cos^(2)x+cos x)dy=0\left(2 y \sin x+3 y^4 \sin x \cos x\right) d x-\left(4 y^3 \cos ^2 x+\cos x\right) d y=0(2ysinx+3y4sinxcosx)dx(4y3cos2x+cosx)dy=0
को हल कीजिए।
Solve the differential equation
( 2 y sin x + 3 y 4 sin x cos x ) d x ( 4 y 3 cos 2 x + cos x ) d y = 0 2 y sin x + 3 y 4 sin x cos x d x 4 y 3 cos 2 x + cos x d y = 0 (2y sin x+3y^(4)sin x cos x)dx-(4y^(3)cos^(2)x+cos x)dy=0\left(2 y \sin x+3 y^4 \sin x \cos x\right) d x-\left(4 y^3 \cos ^2 x+\cos x\right) d y=0(2ysinx+3y4sinxcosx)dx(4y3cos2x+cosx)dy=0
Answer:
Introduction:
We are given the differential equation:
( 2 y sin x + 3 y 4 sin x cos x ) d x ( 4 y 3 cos 2 x + cos x ) d y = 0 2 y sin x + 3 y 4 sin x cos x d x 4 y 3 cos 2 x + cos x d y = 0 (2y sin x+3y^(4)sin x cos x)dx-(4y^(3)cos^(2)x+cos x)dy=0\left(2 y \sin x + 3 y^4 \sin x \cos x\right) dx – \left(4 y^3 \cos^2 x + \cos x\right) dy = 0(2ysinx+3y4sinxcosx)dx(4y3cos2x+cosx)dy=0
Work/Calculations:
Step 1: Identify M M MMM and N N NNN:
In the given equation, we have M = 2 y sin x + 3 y 4 sin x cos x M = 2 y sin x + 3 y 4 sin x cos x M=2y sin x+3y^(4)sin x cos xM = 2y \sin x + 3y^4 \sin x \cos xM=2ysinx+3y4sinxcosx and N = ( 4 y 3 cos 2 x + cos x ) N = 4 y 3 cos 2 x + cos x N=-(4y^(3)cos^(2)x+cos x)N = -\left(4y^3 \cos^2 x + \cos x\right)N=(4y3cos2x+cosx).
Step 2: Calculate Partial Derivatives:
Calculate the partial derivatives of M M MMM and N N NNN:
M y = 2 sin x + 12 y 3 sin x cos x M y = 2 sin x + 12 y 3 sin x cos x (del M)/(del y)=2sin x+12y^(3)sin x cos x\frac{\partial M}{\partial y} = 2 \sin x + 12y^3 \sin x \cos xMy=2sinx+12y3sinxcosx
N x = 8 y 3 sin x cos x + sin x N x = 8 y 3 sin x cos x + sin x (del N)/(del x)=8y^(3)sin x cos x+sin x\frac{\partial N}{\partial x} = 8y^3 \sin x \cos x + \sin xNx=8y3sinxcosx+sinx
Step 3: Check for Exactness:
Now, check if the equation is exact by comparing M y M y (del M)/(del y)\frac{\partial M}{\partial y}My and N x N x (del N)/(del x)\frac{\partial N}{\partial x}Nx:
M y N x N = 2 sin x + 12 y 3 sin x cos x ( 8 y 3 sin x cos x + sin x ) ( 4 y 3 cos 2 x + cos x ) = tan x M y N x N = 2 sin x + 12 y 3 sin x cos x ( 8 y 3 sin x cos x + sin x ) 4 y 3 cos 2 x + cos x = tan x ((del M)/(del y)-(del N)/(del x))/(N)=(2sin x+12y^(3)sin x cos x-(8y^(3)sin x cos x+sin x))/(-(4y^(3)cos^(2)x+cos x))=-tan x\frac{\frac{\partial M}{\partial y} – \frac{\partial N}{\partial x}}{N} = \frac{2 \sin x + 12y^3 \sin x \cos x – (8y^3 \sin x \cos x + \sin x)}{-\left(4y^3 \cos^2 x + \cos x\right)} = -\tan xMyNxN=2sinx+12y3sinxcosx(8y3sinxcosx+sinx)(4y3cos2x+cosx)=tanx
Step 4: Find the Integration Factor:
The integration factor is given by e tan x d x = cos x e tan x d x = cos x e^(-int tan xdx)=cos xe^{-\int \tan x dx} = \cos xetanxdx=cosx.
Step 5: Multiply and Simplify:
Multiply the entire equation by the integration factor cos x cos x cos x\cos xcosx:
cos x ( 2 y sin x + 3 y 4 sin x cos x ) d x cos x ( 4 y 3 cos 2 x + cos x ) d y = 0 cos x 2 y sin x + 3 y 4 sin x cos x d x cos x 4 y 3 cos 2 x + cos x d y = 0 cos x(2y sin x+3y^(4)sin x cos x)dx-cos x(4y^(3)cos^(2)x+cos x)dy=0\cos x \left(2y \sin x + 3y^4 \sin x \cos x\right) dx – \cos x \left(4y^3 \cos^2 x + \cos x\right) dy = 0cosx(2ysinx+3y4sinxcosx)dxcosx(4y3cos2x+cosx)dy=0
This makes the equation exact.
Step 6: Integrate:
Now, integrate both sides with respect to x x xxx to find the solution:
( y sin 2 x + 3 y 2 2 sin 2 x cos x ) d x = C y sin 2 x + 3 y 2 2 sin 2 x cos x d x = C int(y sin 2x+(3y^(2))/(2)sin 2x cos x)dx=C\int \left(y \sin 2x + \frac{3y^2}{2} \sin 2x \cos x\right) dx = C(ysin2x+3y22sin2xcosx)dx=C
Further integrate and simplify to find the solution:
y cos 2 x 2 3 y 2 4 cos 3 x 3 3 y 2 4 cos x = C y cos 2 x 2 3 y 2 4 cos 3 x 3 3 y 2 4 cos x = C -(y cos 2x)/(2)-(3y^(2))/(4)*(cos 3x)/(3)-(3y^(2))/(4)cos x=C-\frac{y \cos 2x}{2} – \frac{3y^2}{4} \cdot \frac{\cos 3x}{3} – \frac{3y^2}{4} \cos x = Cycos2x23y24cos3x33y24cosx=C
Conclusion:
The solution to the given differential equation is:
y cos 2 x 2 3 y 2 4 cos 3 x 3 3 y 2 4 cos x = C y cos 2 x 2 3 y 2 4 cos 3 x 3 3 y 2 4 cos x = C -(y cos 2x)/(2)-(3y^(2))/(4)*(cos 3x)/(3)-(3y^(2))/(4)cos x=C-\frac{y \cos 2x}{2} – \frac{3y^2}{4} \cdot \frac{\cos 3x}{3} – \frac{3y^2}{4} \cos x = Cycos2x23y24cos3x33y24cosx=C
(b) अवकल समीकरण
d 2 y d x 2 4 d y d x + 4 y = 3 x 2 e 2 x sin 2 x d 2 y d x 2 4 d y d x + 4 y = 3 x 2 e 2 x sin 2 x (d^(2)y)/(dx^(2))-4(dy)/(dx)+4y=3x^(2)e^(2x)sin 2x\frac{d^2 y}{d x^2}-4 \frac{d y}{d x}+4 y=3 x^2 e^{2 x} \sin 2 xd2ydx24dydx+4y=3x2e2xsin2x
का पूर्ण हल ज्ञात कीजिए।
Determine the complete solution of the differential equation
d 2 y d x 2 4 d y d x + 4 y = 3 x 2 e 2 x sin 2 x d 2 y d x 2 4 d y d x + 4 y = 3 x 2 e 2 x sin 2 x (d^(2)y)/(dx^(2))-4(dy)/(dx)+4y=3x^(2)e^(2x)sin 2x\frac{d^2 y}{d x^2}-4 \frac{d y}{d x}+4 y=3 x^2 e^{2 x} \sin 2 xd2ydx24dydx+4y=3x2e2xsin2x
Answer:

Auxiliary Equation:

To solve the given differential equation, we start by finding the auxiliary equation, which is given by
D 2 4 D + 4 = 0 D 2 4 D + 4 = 0 D^(2)-4D+4=0D^2-4 D+4=0D24D+4=0
where D D DDD represents the derivative operator. Solving this equation yields two identical roots, D = 2 D = 2 D=2D=2D=2. Thus, the complementary function (C.F.) is expressed as:
C . F . = ( c 1 + c 2 x ) e 2 x C . F . = c 1 + c 2 x e 2 x C.F.=(c_(1)+c_(2)x)e^(2x)C . F .=\left(c_1+c_2 x\right) e^{2 x}C.F.=(c1+c2x)e2x
where c 1 c 1 c_(1)c_1c1 and c 2 c 2 c_(2)c_2c2 are arbitrary constants.

Particular Integral (P.I.):

P.I. = 1 ( D 2 ) 2 3 x 2 e 2 x sin 2 x = 3 e 2 x 1 ( D + 2 2 ) 2 x 2 sin 2 x = 3 e 2 x 1 D 2 x 2 sin 2 x = 3 e 2 x 1 D x 2 sin 2 x d x = 8 e 2 x 1 D [ x 2 ( cos 2 x 2 ) ( 2 x ) ( cos 2 x 2 ) d x ] , integrating by parts = 3 e 2 x 1 D [ 1 2 x 2 cos 2 x + x cos 2 x d x ] = 8 e 2 x 1 D [ 1 2 x 2 cos 2 x + x ( sin 2 x 2 ) 1 sin 2 x 2 d x ] = 3 e 2 x 1 D [ 1 2 x 2 cos 2 x + 1 2 x sin 2 x + 1 4 cos 2 x ] = 8 e 2 x ( 1 2 x 2 cos 2 x + 1 2 x sin 2 x + 1 4 cos 2 x ) d x = 3 e 2 x [ 1 2 x 2 cos 2 x d x + 1 2 x sin 2 x d x + 1 4 cos 2 x d x ] = 3 e 2 x [ 1 2 { x 2 ( 1 2 sin 2 x ) 2 x ( 1 2 sin 2 x ) d x } + 1 2 x sin 2 x d x + 1 8 sin 2 x ] = 3 e 2 x [ 1 4 x 2 sin 2 x d x + 1 2 x sin 2 x d x + 1 2 x sin 2 x d x + ( 1 / 8 ) × sin 2 x ] P.I. = 1 ( D 2 ) 2 3 x 2 e 2 x sin 2 x = 3 e 2 x 1 ( D + 2 2 ) 2 x 2 sin 2 x = 3 e 2 x 1 D 2 x 2 sin 2 x = 3 e 2 x 1 D x 2 sin 2 x d x = 8 e 2 x 1 D x 2 cos 2 x 2 ( 2 x ) cos 2 x 2 d x , integrating by parts = 3 e 2 x 1 D 1 2 x 2 cos 2 x + x cos 2 x d x = 8 e 2 x 1 D 1 2 x 2 cos 2 x + x sin 2 x 2 1 sin 2 x 2 d x = 3 e 2 x 1 D 1 2 x 2 cos 2 x + 1 2 x sin 2 x + 1 4 cos 2 x = 8 e 2 x 1 2 x 2 cos 2 x + 1 2 x sin 2 x + 1 4 cos 2 x d x = 3 e 2 x 1 2 x 2 cos 2 x d x + 1 2 x sin 2 x d x + 1 4 cos 2 x d x = 3 e 2 x 1 2 x 2 1 2 sin 2 x 2 x 1 2 sin 2 x d x + 1 2 x sin 2 x d x + 1 8 sin 2 x = 3 e 2 x 1 4 x 2 sin 2 x d x + 1 2 x sin 2 x d x + 1 2 x sin 2 x d x + ( 1 / 8 ) × sin 2 x {:[” P.I. “=(1)/((D-2)^(2))3x^(2)e^(2x)sin 2x=3e^(2x)(1)/((D+2-2)^(2))x^(2)sin 2x=3e^(2x)(1)/(D^(2))x^(2)sin 2x],[=3e^(2x)(1)/(D)intx^(2)sin 2xdx=8e^(2x)(1)/(D)[x^(2)(-(cos 2x)/(2))-int(2x)(-(cos 2x)/(2))dx]”,”” integrating by parts “],[=3e^(2x)(1)/(D)[-(1)/(2)x^(2)cos 2x+int x cos 2xdx]=8e^(2x)(1)/(D)[-(1)/(2)x^(2)cos 2x+x((sin 2x)/(2))-int1*(sin 2x)/(2)dx]],[=3e^(2x)(1)/(D)[-(1)/(2)x^(2)cos 2x+(1)/(2)x sin 2x+(1)/(4)cos 2x]=8e^(2x)int(-(1)/(2)x^(2)cos 2x+(1)/(2)x sin 2x+(1)/(4)cos 2x)dx],[=3e^(2x)[-(1)/(2)intx^(2)cos 2xdx+(1)/(2)int x sin 2xdx+(1)/(4)int cos 2xdx]],[=3e^(2x)[-(1)/(2){x^(2)((1)/(2)sin 2x)-int2x((1)/(2)sin 2x)dx}+(1)/(2)int x sin 2xdx+(1)/(8)sin 2x]],[=3e^(2x)[-(1)/(4)x^(2)sin 2xdx+(1)/(2)int x sin 2xdx+(1)/(2)int x sin 2xdx+(1//8)xx sin 2x]]:}\begin{aligned} & \text { P.I. }=\frac{1}{(D-2)^2} 3 x^2 e^{2 x} \sin 2 x=3 e^{2 x} \frac{1}{(D+2-2)^2} x^2 \sin 2 x=3 e^{2 x} \frac{1}{D^2} x^2 \sin 2 x \\ = & 3 e^{2 x} \frac{1}{D} \int x^2 \sin 2 x d x=8 e^{2 x} \frac{1}{D}\left[x^2\left(-\frac{\cos 2 x}{2}\right)-\int(2 x)\left(-\frac{\cos 2 x}{2}\right) d x\right], \text { integrating by parts } \\ = & 3 e^{2 x} \frac{1}{D}\left[-\frac{1}{2} x^2 \cos 2 x+\int x \cos 2 x d x\right]=8 e^{2 x} \frac{1}{D}\left[-\frac{1}{2} x^2 \cos 2 x+x\left(\frac{\sin 2 x}{2}\right)-\int 1 \cdot \frac{\sin 2 x}{2} d x\right] \\ = & 3 e^{2 x} \frac{1}{D}\left[-\frac{1}{2} x^2 \cos 2 x+\frac{1}{2} x \sin 2 x+\frac{1}{4} \cos 2 x\right]=8 e^{2 x} \int\left(-\frac{1}{2} x^2 \cos 2 x+\frac{1}{2} x \sin 2 x+\frac{1}{4} \cos 2 x\right) d x \\ = & 3 e^{2 x}\left[-\frac{1}{2} \int x^2 \cos 2 x d x+\frac{1}{2} \int x \sin 2 x d x+\frac{1}{4} \int \cos 2 x d x\right] \\ = & 3 e^{2 x}\left[-\frac{1}{2}\left\{x^2\left(\frac{1}{2} \sin 2 x\right)-\int 2 x\left(\frac{1}{2} \sin 2 x\right) d x\right\}+\frac{1}{2} \int x \sin 2 x d x+\frac{1}{8} \sin 2 x\right] \\ = & 3 e^{2 x}\left[-\frac{1}{4} x^2 \sin 2 x d x+\frac{1}{2} \int x \sin 2 x d x+\frac{1}{2} \int x \sin 2 x d x+(1 / 8) \times \sin 2 x\right] \end{aligned}