Summary

General Principles

First Law of Thermodynamics

ΔEth=W+Q

The first law is a general statement of energy conservation.

The figure illustrates the first law of thermodynamics.

Work W and heat Q depend on the process by which the system is changed.

Energy

Thermal energy Eth Microscopic energy of moving molecules and stretched molecular bonds. ΔEth depends on the initial/final states but is independent of the process.

Work W Energy transferred to the system by forces in a mechanical interaction.

Heat Q Energy transferred to the system via atomic-level collisions in a thermal interaction.

Important Concepts

Solving Problems of Work on an Ideal Gas

The work done on a gas is

W=−∫ViVfp dV=−(area under the pV curve)
The figure illustrates a pressure versus volume graph.

Solving Calorimetry Problems

When two or more systems interact thermally, they come to a common final temperature determined by

Qnet=Q1+Q2+⋯=0

An adiabatic process has Q=0. Gases move along an adiabat for which pVγ= constant, where γ=CP/CV is the specific heat ratio. An adiabatic process changes the temperature of the gas without heating it.

The figure illustrates a pressure versus volume graph.

The heat of transformation L is the energy needed to cause 1 kg of substance to undergo a phase change

Q=±ML

The specific heat c of a substance is the energy needed to raise the temperature of 1 kg by 1 K:

Q=Mc ΔT

The molar specific heat C is the energy needed to raise the temperature of 1 mol by 1 K:

Q=nC ΔT

The molar specific heat of gases depends on the process by which the temperature is changed:

  • CV= molar specific heat at constant volume

  • CP=CV+R= molar specific heat at constant pressure

Heat is transferred by conduction, convection, radiation, and evaporation.

  • Conduction: dQ/dt=kA(ΔT/L)

  • Radiation: dQ/dt=eσAT4

Summary of Basic Gas Processes

Process Definition Stays constant Work Heat
Isochoric ΔV=0 V and p/T W=0 Q=nCVΔT
Isobaric Δp=0 p and V/T W=−p ΔV Q=nCPΔT
Isothermal ΔT=0 T and pV W=−nRT ln (Vf /Vi) ΔEth=0
Adiabatic Q=0 pVγ W=ΔEth Q=0
All gas processes First law ΔEth=W+Q=nCVΔT Ideal-gas law pV=nRT

Terms and Notation