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Solved 2025: FYUG Even Semester Exam, 2025 CHEMISTRY (CHMDSC-251) Physical Chemistry-II

UNIT-I

1. (a) Define state and path functions, and give one example of each. 2

State Function: A thermodynamic property whose value depends only on the current state of the system (initial and final states) and is independent of the path taken to reach that state

.
  • Example: Internal Energy (U), Enthalpy (H), Entropy (S).
  • Path Function: A thermodynamic property whose value depends on the specific path or process followed during the change between states

    .
  • Example: Work (w), Heat (q).
  • 1. (b) State and explain the zeroth law of thermodynamics. 2

    The Zeroth Law of Thermodynamics states that if two systems are each in thermal equilibrium with a third system, then they are in thermal equilibrium with each other.

    Explanation: If system A is in thermal equilibrium with system C, and system B is also in thermal equilibrium with system C, then A and B are at the same temperature. This law provides the basis for the measurement of temperature using thermometers.

    1. (c) What are exact and inexact differentials? 2

    Exact Differential: A differential of a state function (like dU or dH) where the integral depends only on the initial and final points. Mathematically, it satisfies Euler's reciprocity relation.

    Inexact Differential: A differential of a path function (like dw or dq) where the integral depends on the path taken. These are often denoted by a cross or delta symbol (δw, δq).

    2. (a) (i) Distinguish between isothermal and adiabatic process. 2

    Isothermal Process Adiabatic Process Occurs at a constant temperature (ΔT = 0). Occurs with no heat exchange with surroundings (q = 0). System is in thermal contact with a heat reservoir. System is thermally insulated from the surroundings.

    2. (a) (ii) Derive a relation between temperature and volume in reversible adiabatic expansion. 3

    For an adiabatic process, dq = 0. From First Law: dU = dw = -P dV

    .

    For 1 mole of an ideal gas, dU = Cv dT and P = RT/V

    .

    Cv dT = -(RT/V) dV

    (Cv/R) (dT/T) = -(dV/V)

    Integrating both sides between (T1, V1) and (T2, V2):

    (Cv/R) ln(T2/T1) = -ln(V2/V1) = ln(V1/V2)

    Since R = Cp - Cv, then R/Cv = (Cp/Cv) - 1 = γ - 1

    .
    T V^(γ-1) = constant

    2. (a) (iii) One mole of an ideal gas expands against a constant external pressure of 1 atm from 10 dm³ to 30 dm³. Calculate work. 2

    Work done in irreversible expansion against constant external pressure (Pext):

    w = -Pext (V2 - V1)

    w = -1 atm * (30 dm³ - 10 dm³) = -1 atm * 20 dm³

    To convert to Joules (1 L-atm = 101.325 J):

    w = -20 * 101.325 J = -2026.5 J

    2. (a) (iv) Derive the expression for the work done in reversible isothermal expansion. 3

    In a reversible isothermal process, T is constant and P = nRT/V

    .

    w = -∫ P dV (from V1 to V2)

    w = -∫ (nRT/V) dV = -nRT ∫ (1/V) dV

    w = -nRT [ln V] (from V1 to V2)

    w = -nRT ln(V2/V1) or w = -2.303 nRT log(V2/V1)

    2. (b) (i) Calculate enthalpy of formation of glucose. 2

    Combustion of Glucose: C6H12O6(s) + 6O2(g) → 6CO2(g) + 6H2O(l)

    ΔH_comb = [6 * ΔHf(CO2) + 6 * ΔHf(H2O)] - [ΔHf(C6H12O6) + 6 * ΔHf(O2)]

    -2816 = [6 * (-393.5) + 6 * (-285.9)] - [ΔHf(C6H12O6) + 0]

    -2816 = [-2361 - 1715.4] - ΔHf(C6H12O6)

    -2816 = -4076.4 - ΔHf(C6H12O6)

    ΔHf(C6H12O6) = -4076.4 + 2816

    ΔHf(C6H12O6) = -1260.4 kJ/mol

    2. (b) (ii) Deduce Kirchhoff's equation. 3

    Kirchhoff's equation describes the variation of enthalpy of reaction with temperature

    .

    ΔH = H(products) - H(reactants)

    Differentiating with respect to T at constant pressure:

    (d(ΔH)/dT)p = (dH(prod)/dT)p - (dH(react)/dT)p

    Since (dH/dT)p = Cp:

    (d(ΔH)/dT)p = ΔCp

    Integrating between T1 and T2:

    ΔH2 - ΔH1 = ΔCp (T2 - T1)

    UNIT-II

    3. (a) Give the statement of second law of thermodynamics in terms of entropy. 2

    The entropy of the universe (an isolated system) increases in the course of any spontaneous change.

    Mathematically, for a spontaneous process: ΔS_total > 0

    .

    4. (a) (ii) Derive Gibbs-Helmholtz equation for a process at constant pressure. 3

    We know G = H - TS. For a process: ΔG = ΔH - TΔS.

    From Maxwell relations, (dΔG/dT)p = -ΔS

    .

    Substituting -ΔS in the ΔG equation:

    ΔG = ΔH + T(dΔG/dT)p

    Rearranging this gives the Gibbs-Helmholtz equation:

    [d(ΔG/T) / dT]p = -ΔH / T²

    4. (b) (ii) Show that -ΔA_T = w_max. 2

    Work function A is defined as A = U - TS. At constant temperature: ΔA = ΔU - TΔS.

    From Second Law, for a reversible process: ΔS = q_rev / T, so TΔS = q_rev

    .

    ΔA = ΔU - q_rev. From First Law: ΔU - q = w.

    Therefore, ΔA = w_rev

    .

    Since work done by the system is -w, then -ΔA = -w_rev = w_max.

    The decrease in work function (Helmholtz free energy) at constant temperature equals the maximum work obtainable from the system.

    UNIT-III

    5. (a) What is triple point? 2

    The triple point is the specific temperature and pressure at which all three phases (solid, liquid, and gas) of a substance coexist in thermodynamic equilibrium

    . For water, the triple point is at 273.16 K and 0.006 atm.

    6. (b) (iii) Explain the phase diagram of CO2 in detail. 3

    The phase diagram of CO2 consists of three areas representing Solid, Liquid, and Gas phases

    .
  • Triple Point: Occurs at 5.11 atm and -56.6°C. Below this pressure, liquid CO2 cannot exist.
  • Sublimation: At 1 atm, solid CO2 (dry ice) sublimes directly to gas at -78.5°C.
  • Critical Point: Occurs at 31.1°C and 73 atm. Beyond this, CO2 exists as a supercritical fluid.
  • Slope: Unlike water, the fusion curve (solid-liquid) has a positive slope, meaning melting point increases with pressure.
  • UNIT-IV

    7. (a) State and explain Le Chatelier's principle. 2

    If a system at equilibrium is subjected to a change in concentration, temperature, or pressure, the system will shift its equilibrium position in a direction that tends to counteract the effect of the change.

    Example: In the Haber process (exothermic), increasing pressure shifts equilibrium toward ammonia production to reduce the number of moles

    .

    8. (a) (i) Deduce Gibbs-Duhem equation. 2

    The total Gibbs free energy of a mixture is G = Σ ni μi

    .

    Differentiating G: dG = Σ ni dμi + Σ μi dni

    .

    Also, from the fundamental equation at constant T and P: dG = Σ μi dni

    .

    Comparing the two equations:

    Σ ni dμi = 0

    This shows that chemical potentials of components in a mixture are not independent

    .

    UNIT-V

    9. (a) Define pH. Calculate pH of 10⁻⁹ M HCl. 4

    pH Definition: pH is the negative logarithm (base 10) of the molar concentration of hydrogen ions: pH = -log[H+]

    .

    Calculation: Since the concentration is very dilute (10⁻⁹ M), we must include [H+] from water (10⁻⁷ M)

    .

    [H+]_total = [H+]_acid + [H+]_water ≈ 1.01 * 10⁻⁷ M.

    pH = -log(1.01 * 10⁻⁷) ≈ 6.99

    .

    Exam Focus Enhancements

    Exam Tips

  • For Unit-I, always distinguish clearly between system boundaries and surrounding interactions.
  • [span_55](start_span)
  • In Phase Rule problems, verify the number of components (C) carefully for reactive systems[span_55](end_span).
  • Common Mistakes

  • Forgetting to include the [H+] from water in very dilute acid/base solutions (below 10⁻⁷ M).
  • Confusing state functions with path functions; remember work and heat are path-dependent.
  • Important Formulas List

  • First Law: ΔU = q + w
  • Phase Rule: F = C - P + 2
  • pH: -log[H+]
  • Gibbs Free Energy: ΔG = ΔH - TΔS
  • Answer Presentation Strategy

    Always start long answers with a formal definition. Use bullet points for derivations and conclude with the physical significance of the final formula. [span_63](start_span)Insert diagrams for phase rule questions to score higher marks[span_63](end_span).


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