Isobaric/isochoric (?) heating of an ideal gas

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SUMMARY

The discussion focuses on calculating the changes in enthalpy (ΔH) and internal energy (ΔU) for an ideal gas with a constant volume heat capacity (C_V) of 6.76 cal/(mol·K) when heated from 273.15 K to 373.15 K. The calculations confirm that for an isochoric process, ΔU equals the heat added (Q), resulting in ΔU = 6760 cal. The change in enthalpy is calculated using the relationship ΔH = ΔU + Δ(PV), leading to a final value of ΔH = 8777 cal after considering the change in pressure using the ideal gas law.

PREREQUISITES
  • Understanding of ideal gas laws, specifically PV=nRT
  • Knowledge of thermodynamic concepts such as internal energy and enthalpy
  • Familiarity with heat capacities, particularly C_V and C_P
  • Ability to perform calculations involving calorimetry and thermodynamic equations
NEXT STEPS
  • Study the derivation and applications of the ideal gas law (PV=nRT)
  • Learn about the differences between isochoric and isobaric processes in thermodynamics
  • Explore the relationship between heat capacities C_V and C_P for ideal gases
  • Investigate the implications of changes in pressure and volume on thermodynamic systems
USEFUL FOR

This discussion is beneficial for students and professionals in thermodynamics, particularly those studying ideal gas behavior, as well as anyone involved in physical chemistry or engineering applications related to heat transfer and energy calculations.

MexChemE
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Homework Statement


Consider an ideal gas with C_V=6.76 \frac{cal}{mol \cdot K}. Calculate \Delta H and \Delta U when ten moles of this gas are heated from 273.15 K to 373.15 K.

Homework Equations


\Delta H = \Delta U + P\Delta V
Q=n C_V \Delta T

The Attempt at a Solution


As I'm given the heat capacity at constant volume I'm assuming this is an isochoric process. That means W=0. Therefore, \Delta U=Q.
\Delta U=Q= (10 \ mol) \left(6.76 \frac{cal}{mol \cdot K} \right) (100 \ K) = 6760 \ cal
Now, for the change in enthalpy we have:
\Delta H = 6760 \ cal + P\Delta V
This is where I'm having trouble. Should I cancel the second term in the above equation? And so have: \Delta H=\Delta U. But, if the gas is heated at constant volume pressure should increase, that means I should consider the PV term in the last equation. I wasn't provided with initial or final values for pressure and volume, so there's not enough information to use PV=nRT. What should I do?
 
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But the last term isn't V, it's ΔV, so no matter what P is, PΔV for an isochoric process will be 0, because volume doesn't change (ΔV=0). I feel that this is a safe assumption, since you were given CV, which is the specific heat at constant volume.
 
Could the last term be Δ(PV)? I just realized I can get (PV)1 and (PV)2 from PV=nRT with the data I was provided.
 
Sorry to double post but I think I figured it out. The standard definition of the change of enthalpy: ΔH = ΔU + Δ(PV). The case ΔH = ΔU + PΔV is only for isobaric processes. The process here is isochoric, so we have no work done by the system, but we had a change in pressure. Therefore, ΔH = Q + PΔV + VΔP. I can cancel out the PΔV term, and I can get VΔP with the ideal gas law. So:
\Delta H = 6790 \ cal + (10 \ mol) \left(1.987 \ \frac{cal}{mol \cdot K} \right)(100 \ K) = 8777 \ cal

Is it right this time?
 
Last edited:
Nothing is said about the process of heating. The internal energy of n mol of an ideal gas is U=nCvT, so
##\Delta U=nCv \Delta T##
for any process. H is defined as H=U+PV. Substituting P=nRT/V from the ideal gaw law, H=nT(Cv+R) =nTCp.
##\Delta H=nCp \Delta T##.
Your method and result are correct.

ehild
 
Last edited:
Thank you!
 

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