(a) (i) Define chemical thermodynamics and outline its significance.
(ii) Explain the concept of thermodynamic reversibility with the help of a suitable example.
(b) (i) 223 J of heat was supplied to a thermodynamic system and its internal energy was found to decrease by 92 J . Calculate the amount of associated work and state whether the work was done by the system or done on the system?
(ii) Derive the relationship between the temperature and pressure for a reversible adiabatic process.
(a) (i) 0.5 mole of an ideal gas is taken in a container at 298 K . Calculate the values of its heat capacities at constant pressure and at constant volume conditions.
(ii) 1 mole of an ideal gas is allowed to undergo isothermal reversible expansion at 25^(@)C25^{\circ} \mathrm{C} from a volume of 10dm^(3)10 \mathrm{dm}^3 to 20dm^(3)20 \mathrm{dm}^3. Calculate the maximum amount of work done by the gas on the surroundings.
(b) (i) Derive the relationship between Delta _(r)U\Delta_r U and Delta _(s)H\Delta_s H.
(ii) Describe the method for experimental determination of energy changes accompanying chemical reactions under constant volume conditions.
(a) (i) State Hess’ law of constant heat summation and give its significance
(ii) Using the bond enthalpy datafrom Table 3.2 of (Unit 3; p, 76), calculate the enthalpy of hydrogenation of 1-propene.
(b) (i) Give the mathematical expressions for the thermodynamic and statistical definitions of entropy.
(ii) Explain the effect of temperature on the enthalpy of a reaction and derive the Kirchhoff’s equation.
(a) (i) What is residual entropy? What kind of systems show residual entropy?
(ii) Explain the difference between enthalpy driven and entropy driven reactions.
(b) (i) Define equilibrium constant and write the expressions for concentration equilibrium constant for the following reaction
2SO_(2)(g)+O_(2)(g)⇌2SO_(3)(g)K_(c)=245(” at “100K)2 \mathrm{SO}_2(\mathrm{~g})+\mathrm{O}_2(\mathrm{~g}) \rightleftharpoons 2 \mathrm{SO}_3(\mathrm{~g}) K_{\mathrm{c}}=245(\text { at } 100 \mathrm{~K})
the equilibrium concentrations are [SO_(2)]=0.204,[O_(2)]=0.0264\left[\mathrm{SO}_2\right]=0.204,\left[\mathrm{O}_2\right]=0.0264 and [SO_(3)]=0.368\left[\mathrm{SO}_3\right]=0.368. Show that the equilibrium will shift towards the reactants side if the concentration of SO_(2)\mathrm{SO}_2 is suddenly doubled.
(a) (i) Define degree of hydrolysis and derive its relationship with hydrolysis constant
(ii) Explain the effect of addition of inert gas to a gaseous equilibrium reaction under the conditions of i) constant volume and ii) constant pressure.
(b) (i) Calculate the pH of 0.1 M aqueous solution of sodium formate at 298 K . [Given: Ka(HCOOH)=1.7 xx10^(-4)\mathrm{Ka}(\mathrm{HCOOH})=1.7 \times 10^{-4} at 298 K
(ii) Define solubility product constant and derive an expression for the solubility product constant for a sparingly soluble salt of M_(2)A_(3)\mathrm{M}_2 \mathrm{~A}_3 type having a solubility of S moldm^(-3)\mathrm{mol} \mathrm{dm}{ }^{-3}.
PART B: FUNCTIONAL GROUP ORGANIC CHEMISTRY-I
(a) Both 1,3,5-cycloheptatrienyl cation and 1,3,5-cycloheptatriene have 6pi6 \pi elections, comments on the aromaticity of these compounds.
(b) Discuss the role of Lewis acids in halogenations and alkylation reactions of benzene. Write the limitations of Freidel Crafts alkylation reaction.
(a) Nitro group is meta directing, explain.
(b) What would be the final products of the reaction of HI with diethyl ether and anisol? Write the mechanism of both the reactions.
(a) What is aldol condensation? Write its mechanism.
(b) Arrange the following in order of their increasing reactivity towards S_(N)2\mathrm{S}_{\mathrm{N}} 2 substitution reactions: bromomethane, 1-bromo-propane, 2-bromopropane, 2 -bormo-2-methyl propane. Justify your answer.
(a) Write their representative reaction for the following reactions.
(b) Sandmeyer reaction
(c) Reimer-Tiemann reaction
(d) Mannich reaction
(e) Willgerodt reaction
(f) Knoevenagel reaction
10 (a) Write the mechanism of Pinacol-pinacolone reaction.
(b) How you will introduce a formyl group into phenol ring.
Answer:
Question:-1
1. (a) (i) Define chemical thermodynamics and outline its significance.
Answer:
Chemical Thermodynamics is the branch of physical chemistry that deals with the relationships between heat, work, energy, and the properties of matter during chemical reactions. It focuses on understanding how energy is transferred and transformed in chemical processes and helps in predicting the direction and extent of reactions.
Significance of Chemical Thermodynamics:
Predicting Reaction Feasibility: It helps in determining whether a chemical reaction will occur spontaneously under specific conditions.
Understanding Energy Transfer: It provides insights into how energy is absorbed or released during chemical reactions, essential for designing efficient processes in industries.
Equilibrium Analysis: Chemical thermodynamics aids in understanding the conditions under which a chemical equilibrium is reached, guiding the optimization of industrial reactions.
Calculating Work and Heat: It enables the calculation of work done by or on a system and the heat exchanged, crucial for processes like engines, refrigeration, and chemical manufacturing.
Design of Chemical Processes: The principles of thermodynamics are key in designing processes like distillation, refrigeration, and power plants, ensuring they are energy-efficient and cost-effective.
Enzyme and Biological Reactions: It helps explain biochemical processes in living organisms, from metabolic pathways to the functioning of enzymes.
1. (a) (ii) Explain the concept of thermodynamic reversibility with the help of a suitable example.
Answer:
Thermodynamic Reversibility refers to a process that can be reversed without any net change in both the system and its surroundings. In a reversible process, the system is in equilibrium at every stage, meaning it can be returned to its original state by infinitesimally small changes in external conditions, without dissipation of energy.
For a process to be truly reversible, it must be carried out infinitely slowly, so the system remains in thermodynamic equilibrium throughout. In real-life situations, some degree of irreversibility always occurs due to friction, heat loss, or other factors.
Example: Reversible Isothermal Expansion of an Ideal Gas
Imagine an ideal gas confined in a piston at a certain temperature and pressure. If the gas expands isothermally (at a constant temperature) in a perfectly reversible manner, it does so in such a way that the temperature of the gas remains constant throughout the expansion. The gas does work on the piston, but the heat energy required for the expansion is supplied from the surroundings, maintaining the temperature.
Process description:
The gas is allowed to expand slowly by pushing the piston up.
At every point during the expansion, the gas is in thermal equilibrium with its surroundings (since heat is exchanged to maintain temperature).
The system’s pressure and volume change continuously and uniformly, ensuring no entropy is generated.
Reversibility:
If you reverse the process, you can compress the gas back to its original volume and pressure by lowering the piston very slowly, again ensuring equilibrium at every stage.
No energy is lost in the process, and both the system and surroundings are returned to their original states with no net change in entropy.
In contrast, an irreversible process (like the rapid expansion of the gas into a vacuum, also known as free expansion) involves a sudden change, causing a large increase in entropy and heat dissipation to the surroundings, making it impossible to reverse the process without additional work.
Thus, thermodynamic reversibility ensures the maximum possible efficiency and no energy loss, a concept critical to understanding idealized processes in thermodynamics.
1. (b) (i) 223 J of heat was supplied to a thermodynamic system and its internal energy was found to decrease by 92 J. Calculate the amount of associated work and state whether the work was done by the system or done on the system?
Answer:
To solve this problem, we can use the First Law of Thermodynamics, which states:
Delta U=Q-W\Delta U = Q – W
Where:
Delta U\Delta U is the change in internal energy of the system.
QQ is the heat supplied to the system.
WW is the work done by the system.
Given:
Heat supplied, Q=223″J”Q = 223 \, \text{J}
Change in internal energy, Delta U=-92″J”\Delta U = -92 \, \text{J} (The internal energy decreases, so it’s negative.)
Now, substitute the values into the equation:
-92=223-W-92 = 223 – W
Rearranging to solve for WW:
W=223+92=315″J”W = 223 + 92 = 315 \, \text{J}
Interpretation:
The positive value of W=315″J”W = 315 \, \text{J} means that 315 J of work was done by the system on its surroundings.
Thus, the system did work as it lost some of the supplied heat to do work while its internal energy decreased.
1. (b) (ii) Derive the relationship between the temperature and pressure for a reversible adiabatic process.
Answer:
Deriving the Relationship between Temperature and Pressure for a Reversible Adiabatic Process
We aim to find the relationship between temperature and pressure for a reversible adiabatic process.
Step 1: Start with the First Law of Thermodynamics
For an adiabatic process, there is no heat exchange, so the change in internal energy is equal to the work done by or on the gas:
dU=-pdV\mathrm{d}U = -p \, \mathrm{d}V
Since internal energy change for an ideal gas is given by dU=C_(V)dT\mathrm{d}U = C_V \, \mathrm{d}T, where C_(V)C_V is the heat capacity at constant volume, we can equate the two expressions:
This equation shows how temperature and pressure are related during an adiabatic expansion or compression.
Question:-2
2. (a) (i) 0.5 mole of an ideal gas is taken in a container at 298 K. Calculate the values of its heat capacities at constant pressure and at constant volume conditions.
Answer:
To calculate the heat capacities of an ideal gas at constant pressure (C_(P)C_P) and constant volume (C_(V)C_V), we will use the general relationships for ideal gases and the values of the specific heat capacities in terms of the gas constant.
Step 1: Understanding the given information
Number of moles of the gas, n=0.5″mol”n = 0.5 \, \text{mol}
Temperature, T=298″K”T = 298 \, \text{K}
We’ll assume the gas behaves ideally and that we are working with a diatomic ideal gas (which is typical unless otherwise specified).
Step 2: Use of heat capacities for ideal gases
For an ideal gas, the heat capacities at constant volume and constant pressure are related to the molar specific heats:
C_(V)=(f)/(2)RC_V = \frac{f}{2} R, where ff is the number of degrees of freedom of the gas molecules.
C_(P)=C_(V)+RC_P = C_V + R, where RR is the universal gas constant (R=8.314″J/mol·K”R = 8.314 \, \text{J/mol·K}).
Step 3: Assumption about the type of gas
If the gas is diatomic (e.g., oxygen or nitrogen), then the number of degrees of freedom ff is typically 5 (3 translational and 2 rotational degrees of freedom, assuming we are neglecting vibrational modes at this temperature).
For a diatomic gas:
C_(V)=(5)/(2)RC_V = \frac{5}{2} R
C_(P)=C_(V)+R=(5)/(2)R+R=(7)/(2)RC_P = C_V + R = \frac{5}{2} R + R = \frac{7}{2} R
Step 4: Calculate the heat capacities
Using R=8.314″J/mol·K”R = 8.314 \, \text{J/mol·K}:
The heat capacity at constant volume (C_(V)C_V) is 10.39″J/K”\boxed{10.39 \, \text{J/K}}.
The heat capacity at constant pressure (C_(P)C_P) is 14.55″J/K”\boxed{14.55 \, \text{J/K}}.
2. (a) (ii) 1 mole of an ideal gas is allowed to undergo isothermal reversible expansion at 25^(@)C25^{\circ} \mathrm{C} from a volume of 10dm^(3)10 \mathrm{dm}^3 to 20dm^(3)20 \mathrm{dm}^3. Calculate the maximum amount of work done by the gas on the surroundings.
Answer:
To calculate the maximum work done by the gas on the surroundings during an isothermal reversible expansion, we can use the formula for work in an isothermal process for an ideal gas:
The maximum work done by the gas on the surroundings during the isothermal reversible expansion is approximately 1722.2″J”\boxed{1722.2 \, \text{J}}.
2. (b) (i) Derive the relationship between Delta _(r)U\Delta_r U and Delta _(s)H\Delta_s H.
Answer:
To derive the relationship between the change in internal energy (Delta _(r)U\Delta_r U) and the change in enthalpy (Delta _(r)H\Delta_r H) for a reversible reaction, we need to start with the fundamental thermodynamic definitions and use the first law of thermodynamics.
Step 1: Recall the first law of thermodynamics
The first law of thermodynamics states that the change in internal energy (Delta U\Delta U) for a system is related to the heat (QQ) and the work (WW) done by or on the system:
Delta U=Q-W\Delta U = Q – W
For a reversible process, the work done by an ideal gas is W=P Delta VW = P \Delta V, where PP is the pressure and Delta V\Delta V is the change in volume.
Step 2: Define Enthalpy
Enthalpy HH is defined as:
H=U+PVH = U + PV
The change in enthalpy (Delta H\Delta H) is therefore:
Delta H=Delta U+Delta(PV)\Delta H = \Delta U + \Delta (PV)
Now, if the pressure is constant during the process (which is often assumed in many reactions), the term Delta(PV)\Delta(PV) can be written as P Delta VP \Delta V. So, we get:
Delta H=Delta U+P Delta V\Delta H = \Delta U + P \Delta V
Step 3: Relating Delta _(r)U\Delta_r U and Delta _(r)H\Delta_r H for a Reversible Process
Now, let’s relate this to a reversible reaction. For a reversible reaction, we can write the change in internal energy (Delta _(r)U\Delta_r U) and change in enthalpy (Delta _(r)H\Delta_r H) for the reaction as:
Delta _(r)H=Delta _(r)U+P Delta V\Delta_r H = \Delta_r U + P \Delta V
This equation relates the change in enthalpy to the change in internal energy and the work done during the process.
Step 4: Generalize for Reactions Involving Heat Transfer
In many cases, heat is transferred during a reaction, and this heat is related to the enthalpy change. For an isothermal process (constant temperature) or a process where the heat exchanged is not a function of the change in volume alone, the relationship will take the form:
Delta _(r)U=Delta _(r)H-P Delta V\Delta_r U = \Delta_r H – P \Delta V
This equation shows how the change in internal energy for a reversible reaction (Delta _(r)U\Delta_r U) is related to the change in enthalpy (Delta _(r)H\Delta_r H) and the work done by the system.
Step 5: Special Case for Ideal Gases
For ideal gases, where P Delta V=nR Delta TP \Delta V = n R \Delta T (and assuming temperature is constant or known), the above equation simplifies further, but this equation gives the general relationship between Delta _(r)U\Delta_r U and Delta _(r)H\Delta_r H in terms of the pressure-volume work.
Final Answer:
Thus, the relationship between the change in internal energy and the change in enthalpy is:
Delta _(r)U=Delta _(r)H-P Delta V\Delta_r U = \Delta_r H – P \Delta V
This expresses how the internal energy change for a reversible reaction depends on the change in enthalpy and the volume change in the system.
2. (b) (ii) Describe the method for experimental determination of energy changes accompanying chemical reactions under constant volume conditions.
Answer:
The experimental determination of energy changes (Delta U\Delta U) accompanying chemical reactions under constant volume conditions is typically performed using a bomb calorimeter. This is a device designed to measure the heat released or absorbed during a reaction while keeping the volume constant, which allows for the determination of the internal energy change (Delta U\Delta U).
Method for Experimental Determination of Energy Changes
Here’s a step-by-step outline of the method:
Step 1: Set Up a Bomb Calorimeter
A bomb calorimeter consists of a sealed, rigid container known as the "bomb," which holds the sample (usually a fuel or reactant). The bomb is surrounded by water, and temperature sensors are placed inside both the bomb and the surrounding water.
The bomb is designed to withstand high pressures, especially when the reaction involves combustion.
The system is isolated to ensure no heat exchange with the external environment (adiabatic conditions).
Step 2: Place the Reactants in the Bomb
The reactants (e.g., a known mass of a substance like a fuel) are placed inside the bomb, typically in the form of a solid or liquid.
The bomb is filled with pure oxygen to ensure complete combustion or reaction in the case of a combustion reaction.
Step 3: Ignite the Reaction
The reaction is initiated (e.g., by using an electrically heated wire) to ensure it proceeds completely under controlled conditions.
Since the bomb is sealed and the volume is constant, no expansion of the gases is allowed, and the system is effectively at constant volume.
Step 4: Measure the Temperature Change
After the reaction is initiated, the heat released (or absorbed) by the reaction is transferred to the surrounding water.
The temperature of the water is carefully monitored using temperature sensors (often thermocouples or resistance thermometers).
Step 5: Calculate the Heat Released (or Absorbed)
The heat change (q_(“water”)q_{\text{water}}) in the surrounding water is calculated using the formula:
q_(“water”)=m_(w)C_(w)Delta Tq_{\text{water}} = m_w C_w \Delta T
Where:
m_(w)m_w = mass of the water surrounding the bomb.
C_(w)C_w = specific heat capacity of water.
Delta T\Delta T = temperature change of the water.
Step 6: Determine the Energy Change (Delta U\Delta U)
Under constant volume, the heat absorbed or released by the system is equal to the change in internal energy (Delta U\Delta U) of the system. This is because no work is done (since Delta V=0\Delta V = 0, and W=P Delta VW = P \Delta V).
The energy change (Delta U\Delta U) for the reaction at constant volume is thus:
Delta U=-q_(“water”)\Delta U = – q_{\text{water}}
Where the negative sign accounts for the heat lost by the system (the reaction) being absorbed by the surrounding water.
Step 7: Account for Heat Capacity of the Calorimeter
To improve accuracy, the heat capacity of the entire calorimeter (which includes the bomb, the water, and other components) is often measured beforehand. If the calorimeter is not perfectly insulated, a correction may be applied based on the heat capacity C_(“calorimeter”)C_{\text{calorimeter}} to determine the true energy change.
The energy change Delta U\Delta U is determined based on the temperature change measured in the water and the known calorimetric constants.
If the reaction involves a change in temperature, volume, or involves gases, additional corrections may be required to account for the properties of the reactants and products.
Final Answer:
The experimental determination of energy changes (Delta U\Delta U) under constant volume conditions is typically done using a bomb calorimeter. This method involves measuring the heat transferred to the surrounding water, from which the energy change is derived. The process assumes no work is done by the system (constant volume), and the heat released or absorbed corresponds directly to the change in internal energy of the system.