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Prove that: i. Cv = [dE/dT]v ii. Cp = [dH/dT]p

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2 parts
i
Shown:

CV=[∂E∂T]VC_V = \left[\frac{\partial E}{\partial T}\right]_V

ii
Shown:

CP=[∂H∂T]PC_P = \left[\frac{\partial H}{\partial T}\right]_P

Step-by-step solution

9 steps

Here's the proof for the definitions of heat capacities at constant volume and constant pressure.

Part i· 4 steps

Prove that CV=[∂E∂T]VC_V = \left[\frac{\partial E}{\partial T}\right]_V

  1. Start with the First Law of Thermodynamics.

    The change in internal energy (EE) for a system is given by:

    dE=δq+δwdE = \delta q + \delta w

    where δq\delta q is the heat absorbed by the system and δw\delta w is the work done on the system. For a reversible process, the work done is δw=−PdV\delta w = -P dV.
    Substituting this into the First Law:

    dE=δq−PdVdE = \delta q - P dV
  2. Consider a process at constant volume.

    If the volume (VV) is kept constant, then dV=0dV = 0. In this case, the work done is zero (δw=0\delta w = 0).
    The First Law simplifies to:

    dE=δqVdE = \delta q_V

    where δqV\delta q_V is the heat absorbed at constant volume.

  3. Define heat capacity at constant volume (CVC_V).

    Heat capacity at constant volume is defined as the amount of heat required to raise the temperature of a substance by one degree Celsius (or Kelvin) at constant volume:

    CV=(δqV∂T)VC_V = \left(\frac{\delta q_V}{\partial T}\right)_V
  4. Substitute dEdE into the definition of CVC_V.

    Since dE=δqVdE = \delta q_V at constant volume, we can replace δqV\delta q_V with dEdE:

    CV=(∂E∂T)VC_V = \left(\frac{\partial E}{\partial T}\right)_V

    This proves the first relation.

    CV=[∂E∂T]V\boxed{C_V = \left[\frac{\partial E}{\partial T}\right]_V}

Part ii

CP=[∂H∂T]PC_P = \left[\frac{\partial H}{\partial T}\right]_P

Prove that CP=[∂H∂T]PC_P = \left[\frac{\partial H}{\partial T}\right]_P

  1. Start with the definition of enthalpy (HH).

    Enthalpy is defined as:

    H=E+PVH = E + PV

    where EE is internal energy, PP is pressure, and VV is volume.
    Taking the total differential of HH:

    dH=dE+d(PV)=dE+PdV+VdPdH = dE + d(PV) = dE + P dV + V dP
  2. Substitute dEdE from the First Law of Thermodynamics.

    From Step 1 of part (i), we know dE=δq−PdVdE = \delta q - P dV.
    Substitute this into the expression for dHdH:

    dH=(δq−PdV)+PdV+VdPdH = (\delta q - P dV) + P dV + V dP dH=δq+VdPdH = \delta q + V dP
  3. Consider a process at constant pressure.

    If the pressure (PP) is kept constant, then dP=0dP = 0.
    The expression for dHdH simplifies to:

    dH=δqPdH = \delta q_P

    where δqP\delta q_P is the heat absorbed at constant pressure.

  4. Define heat capacity at constant pressure (CPC_P).

    Heat capacity at constant pressure is defined as the amount of heat required to raise the temperature of a substance by one degree Celsius (or Kelvin) at constant pressure:

    CP=(δqP∂T)PC_P = \left(\frac{\delta q_P}{\partial T}\right)_P
  5. Substitute dHdH into the definition of CPC_P.

    Since dH=δqPdH = \delta q_P at constant pressure, we can replace δqP\delta q_P with dHdH:

    CP=(∂H∂T)PC_P = \left(\frac{\partial H}{\partial T}\right)_P

    This proves the second relation.

    CP=[∂H∂T]P\boxed{C_P = \left[\frac{\partial H}{\partial T}\right]_P}
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