1. A rigid, well-insulated metal container of volume
V=2.00×10−2 m3 holds
n=0.800 mol of helium gas. The gas is initially in thermal equilibrium at temperature
T1=300 K and pressure
P1. Helium can be treated as an ideal monatomic gas. The container is then placed in thermal contact with a large thermal reservoir at temperature
TR=450 K by pressing one flat wall of the container against a thick copper slab, as shown in Figure 1. Energy is transferred between the reservoir and the gas only by conduction through the copper slab. The copper slab has thickness
L=2.00×10−2 m and contact area with the container wall
A=5.00×10−3 m2. The thermal conductivity of copper is
k=400 Wm−1K−1. Assume the gas temperature remains uniform throughout the container at all times.
Figure 1. Rigid insulated container of helium pressed against a copper slab connected to a thermal reservoir (heat transfer only by conduction through copper).
Figure 2. Microscopic motion diagrams for helium at two equilibrium states (State 1 at 300 K, State 2 at 450 K).
Figure 3. Two microscopic collision-rate panels for helium atoms striking a container wall; compare momentum transfer rate (pressure).
i. Complete the following tasks in Figures 2 and 3.
• Indicate in Figure 2 whether State 1 or State 2 corresponds to a greater average translational kinetic energy of the helium atoms.
• Indicate in Figure 3 whether panel (a) or panel (b) corresponds to a greater gas pressure on the container wall, based on the rate of momentum transfer from atoms to the wall.
ii. As the container is brought into thermal contact with the reservoir, the helium warms from T1=300 K to T2=450 K while the volume remains constant. Derive an expression for the final pressure P2 in terms of P1, T1, and T2. Begin your derivation by writing a fundamental physics principle or an equation from the reference information. Figure 4. Pressure–volume (P–V) diagram for heating the helium at constant volume from T₁ = 300 K to T₂ = 450 K.
The copper slab remains in contact with the reservoir at
TR=450 K. While the gas is still at
T1=300 K, energy begins to transfer through the copper slab to the gas by conduction. Consider the direction of net energy transfer and the sign of the entropy change of the helium during this warming process.