Question
A solid object has a density $\rho$, mass $M$, and coefficient of linear expansion $\alpha$. Show that at pressure $p$ the heat capacities $C_p$ and $C_v$ are related by$$C_p-C_v=3 \alpha M p / \rho .$$
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The heat capacity at constant pressure \( C_p \) is defined as the amount of heat required to raise the temperature of the object by one degree while keeping the pressure constant. The heat capacity at constant volume \( C_v \) is defined similarly, but at Show more…
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A solid object has a density (ρ), mass (M), and coefficient of linear expansion (α). Show that at pressure (p), the heat capacities Cp and Cv are related by Cp - Cv = (3αMp/ρ).
solid object has density mass M, and coefficient of linear expansion, 4. Show that at pressure the heat capacities Cp and Cv are given bV, Cp ~ C = 30 "
1. (a) Derive the general relation that between the heat capacity at constant volume (CV) and the heat capacity at constant pressure (Cp): Cp - Cv = TVα² / κ where κ is the isothermal compressibility, and α is the coefficient of thermal expansion (at constant pressure). Start by considering T and p as independent variables so that the entropy S = S(T, p). (b) Use (a) to find γ = cp/cV for an ideal monatomic gas where cp and cV are molar specific heats. (c) Use (a) to find γ = cp/cV for aluminum, which has the following measurable properties at 0° C: Atomic weight = 27 g/mole; density = 2.70 g/cm³; Cp = 0.220 cal/g °C; thermal expansion coefficient = 71.4 × 10⁻⁶/°C; and the compressibility = 1.34 × 10⁻¹² cm²/dyne. Keep the units straight.
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