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NCERT Exemplar · Q33

Q.Identify the state functions and path functions out of the following :
enthalpy, entropy, heat, temperature, work, free energy.

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State functions depend only on the current state of the system, not how it got there; path functions depend on the route taken. State functions: enthalpy, entropy, temperature, free energy. Path functions: heat, work.

The Core Idea: Where You Are vs. How You Got There

Thermodynamics distinguishes between two types of quantities. A state function is a property that depends only on the present condition of the system—its pressure, temperature, composition, and so on. If you know the state, you know the value, regardless of the system's history. Think of altitude on a mountain: your elevation depends only on where you stand, not which trail you hiked.

A path function, by contrast, depends on the process itself—the specific route taken between two states. The work you do climbing that mountain depends on whether you took the steep direct path or the gentle winding trail, even though you end at the same elevation.

Mathematically, state functions have exact differentials: when you integrate around any closed loop, the net change is zero. Path functions do not; their integrals depend on the path.


Sorting the Six Quantities

Let's examine each in turn.

  1. Enthalpy, HH

    Defined as H=U+PVH = U + PV, where UU is internal energy. Both UU, PP, and VV are properties of the state. Once you specify temperature, pressure, and composition, HH is fixed. The enthalpy change ΔH\Delta H between two states is the same no matter whether you heat at constant pressure, do work, or follow any other route.

    State function.

  2. Entropy, SS

    A measure of disorder or the number of accessible microstates. For a reversible process, dS=δqrevT\mathrm{d}S = \frac{\delta q_{\text{rev}}}{T}, and the integral ∫dS\int \mathrm{d}S around a cycle is zero (second law). Entropy is a property of the equilibrium state.

    State function.

  3. Heat, qq

    Energy transferred due to a temperature difference. The amount of heat exchanged between two states depends entirely on the process: an adiabatic path transfers zero heat, an isothermal path transfers q=nRTln⁡(Vf/Vi)q = nRT \ln(V_f/V_i) for an ideal gas, and so on. Heat is not a property stored in the system.

    Path function.

  4. Temperature, TT

    An intensive property that characterizes thermal equilibrium. Once the state is fixed, so is the temperature. It does not depend on how the system reached that state.

    State function.

  5. Work, ww …

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