Part of JTHERM-01 — Thermodynamics: Laws, Processes & Engines

Isobaric and Isochoric Processes

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  • id: JTHERM-01-N08
  • title: Constant Pressure and Constant Volume Processes
  • tags: isobaric, isochoric, Cv, Cp

Isobaric (P = constant): W=PΔV=nRΔTW = P\Delta V = nR\Delta T. Q=nCpΔTQ = nC_p\Delta T. ΔU=nCvΔT\Delta U = nC_v\Delta T. Verification: Q=ΔU+WnCpΔT=nCvΔT+nRΔTCp=Cv+RQ = \Delta U + W \Rightarrow nC_p\Delta T = nC_v\Delta T + nR\Delta T \Rightarrow C_p = C_v + R (Mayer's relation). On P-V diagram: horizontal line.

Isochoric (V = constant): W=0W = 0. Q=ΔU=nCvΔTQ = \Delta U = nC_v\Delta T. All heat goes to internal energy. On P-V diagram: vertical line. Heating in a rigid container is isochoric. Gay-Lussac's law: P/T=constantP/T = \text{constant}.

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