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Principles of Waves, Fluids and Thermodynamics

First Law of Thermodynamics

Physics I 237 words Free to read

The Energy Ledger

The First Law of Thermodynamics is the universe's unbreakable accounting rule: a system's internal energy changes only by heat added or work done.

ΔU=QW\Delta U = Q - W

Here, ΔU\Delta U is internal energy change, QQ is heat added, and WW is work done by the system. A pump warms as you compress it (work becomes energy); a spray can chills as gas expands.

Internal energy for an ideal gas is U=nCVTU = nC_V T, and Mayer's relation links heat capacities by CPCV=RC_P - C_V = R.

Key insight: This law conserves energy but does not restrict direction—the second law handles that.

Ideal Gas Processes

Gas processes transform energy in distinct ways. The table below outlines the core behaviors:

ProcessConditionWork (WW)Heat (QQ)
IsothermalTT constantnRTln(Vf/Vi)nRT\ln(V_f/V_i)Q=WQ = W
IsobaricPP constantPΔVP\Delta VnCPΔTnC_P\Delta T
IsochoricVV constant00nCVΔTnC_V\Delta T
AdiabaticQ=0Q = 0ΔU-\Delta U00

For adiabatic processes, PVγ=constPV^\gamma = \text{const} and TVγ1=constTV^{\gamma-1} = \text{const}, where γ=CP/CV\gamma = C_P/C_V.

Common pitfall: Q=0Q = 0 does not mean ΔT=0\Delta T = 0. Adiabatic compression raises temperature purely through work—this is how a diesel engine fires without a spark plug.
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Principles of Waves, Fluids and Thermodynamics