How to Solve Thermodynamics Relations for Liquid Alcohol?

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SUMMARY

This discussion focuses on solving thermodynamic relations for liquid alcohol, specifically addressing the molar heat capacity at constant volume (C_v,m), pressure variation with temperature at constant volume, and the work done during heating at constant pressure. The key equations utilized include the relationship C_p = C_v + TVa^2/B and the definitions of the isothermal coefficients of thermal expansion (a) and compressibility (B). The participants provide attempts at solutions, demonstrating the application of thermodynamic principles and relationships to derive necessary expressions.

PREREQUISITES
  • Understanding of thermodynamic principles, particularly the first law of thermodynamics.
  • Familiarity with the concepts of molar heat capacity (C_p and C_v).
  • Knowledge of isothermal coefficients of thermal expansion and compressibility.
  • Ability to perform algebraic manipulations and integrations in thermodynamic equations.
NEXT STEPS
  • Study the derivation and application of the first law of thermodynamics in various processes.
  • Learn about the relationships between different thermodynamic potentials, such as internal energy (U) and enthalpy (H).
  • Explore the implications of constant pressure and constant volume processes in thermodynamics.
  • Investigate the behavior of real fluids and the significance of compressibility and thermal expansion in practical applications.
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Students and professionals in thermodynamics, chemical engineering, and physical chemistry who are looking to deepen their understanding of liquid alcohol behavior under varying thermal conditions.

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Homework Statement



We propose to study simple processes of liquid alcohol. At T_1, the molar volume of alcohol is V_1 and its molar heat capacity at constant pressure is C_p,m. We assume that its isobaric coefficient of thermal expansion a, and the isothermal compressibilty coefficient B are constant.

a. Find the molar heat capacity (C_v,m) at constant volume and T_1, and the variation of the pressure with temperature at constant volume.

b. starting from an initial state (T_1, V_1), alcohol receives an amt. of heat at constant pressure P, and its final temp. is T_2. Evaluate the work received by alcohol during the process.

c. Find a formal expression for the rate of change with temperature of the internal energy of the liquid at constant pressure.


Homework Equations



isothermal coefficient of thermal expansion, a = 1/V * (dV/dT)_p
isothermal compressibilty coefficient B, -1/V * (dV/dP)_T

C_p = C_v + TVa^2/B ------ eqn (1)

The Attempt at a Solution



For qns a, i have no idea how to go about finding C_v,m. So i simply used the direct relatonship in eqn (1) to find C_v,m which i highly doubt its correct.
for the second part of the qns,
I used P=P(T,V)
-> dP = MdT + NdV
doing some algebric manipulation: dV = (1/N * dP) - (M/N * dT)
by comparing coefficients from the derived eqn of V=V(T,P)...
i got my final dP = (a/B * dT) - (1/VB *dV)
at constant volume: (dP/dt)_V = a/B

is this correct?

For qns b, here's what i attempted:

(T_1, V_1) ----> (T_2, V_2) at constant P.
Using U=U(T,P) thermodynamics relationship and letting dP=0
i get dU = (C_p - PVa)*dT
by integrating from T_1 to T_2, i will get the change in U.
then to find the Q received, i used H=H(T,P)
where in the end i get dH=Q=C_p * dT
again i integrate to find Q.
then finally i use first law U= Q+W to find W.
is this correct?

For qns c,

i used U=U(T,P)
at constant P, i get dU=(C_P-PVa)*dT

im not sure if this is correct or not...

thanks a lot for helping me out
 
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is there any kind soul who can help me?

Thanks!
 

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