HCV Ch26 P1 – First Law of Thermodynamics: Internal Energy Change

Problem Statement

Solve the thermodynamics problem: A gas absorbs 500 J of heat and does 200 J of work on the surroundings. Find the change in internal energy of the gas. See problem statement for all given quantities. Thermodynamics governs energy transformations involving heat and work. The First Law $\Delta U = Q – W$ expresses energy conservation

Given Information

  • Temperatures, pressures, volumes, and process type as given
  • Universal gas constant $R = 8.314\,\text{J mol}^{-1}\text{K}^{-1}$
  • $C_p$ and $C_v$ or $\gamma = C_p/C_v$ as applicable

Physical Concepts & Formulas

The First Law of Thermodynamics $\Delta U = Q – W$ is an energy balance: internal energy increases when heat flows in and decreases when the gas does work. For ideal gases, internal energy depends only on temperature: $\Delta U = nC_v \Delta T$. Different processes have different constraints: isothermal ($T = \text{const}$, $W = nRT\ln(V_f/V_i)$), adiabatic ($Q=0$, $PV^\gamma = \text{const}$), isobaric ($P = \text{const}$, $W = P\Delta V$), isochoric ($V = \text{const}$, $W = 0$). Carnot efficiency sets the upper bound for any heat engine: $\eta = 1 – T_C/T_H$.

  • $\Delta U = Q – W$ — First Law
  • $PV = nRT$ — Ideal Gas Law
  • $W_{\text{isothermal}} = nRT\ln(V_f/V_i)$
  • $PV^\gamma = \text{const}$ — adiabatic process
  • $\eta_{\text{Carnot}} = 1 – T_C/T_H$ — maximum efficiency

Step-by-Step Solution

Step 1 — Identify the process (isothermal, adiabatic, isobaric, isochoric).

Step 2 — Write the appropriate work expression and compute $W$.

Step 3 — Find $\Delta U = nC_v\Delta T$.

Step 4 — Apply First Law: $Q = \Delta U + W$.

Worked Calculation

Substituting all values with units:

Carnot engine: $T_H = 600\,\text{K}$, $T_C = 300\,\text{K}$:

$$\eta = 1 – \frac{300}{600} = 1 – 0.5 = 0.50 = 50\%$$

Answer

$$\boxed{\eta_{\text{Carnot}} = 1 – \dfrac{T_C}{T_H}}$$

Physical Interpretation

A Carnot efficiency of 50% is the theoretical maximum — no real engine can do better between these temperatures. Real steam turbines achieve ~40%; petrol engines ~25–30%. The gap is due to irreversibilities: friction, heat transfer across finite temperature differences, and non-quasi-static processes. This result, derived purely from the Second Law, set a fundamental limit on the Industrial Revolution.


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