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An ideal gas is in contact with a heat reservoir so that it remains at a constant temperature of \(300.0 \mathrm{K}\). The gas is compressed from a volume of \(24.0 \mathrm{L}\) to a volume of 14.0 L. During the process, the mechanical device pushing the piston to compress the gas is found to expend \(5.00 \mathrm{kJ}\) of energy. How much heat flows between the heat reservoir and the gas and in what direction does the heat flow occur?

Short Answer

Expert verified
Answer: The heat transfer between the gas and the heat reservoir is -5000 J, and the direction of the heat flow is from the gas into the heat reservoir.

Step by step solution

01

Write the First Law of Thermodynamics equation for the given problem

Since we know that the change in internal energy (\(\Delta U\)) is zero, we can rewrite the First Law of Thermodynamics equation as: $$Q = -W$$
02

Convert the work done into Joules

We are given the work done by the mechanical device as \(5.00 \mathrm{kJ}\). To be consistent with the units, we need to convert this value into Joules. We know that \(1 \mathrm{kJ} = 1000 \mathrm{J}\), so the work done is: $$W = 5.00 \times 1000 = 5000 \mathrm{J}$$
03

Calculate the heat transfer

Using the equation we derived in Step 1, we can now calculate the heat transfer as: $$Q = -W$$ $$Q = -5000 \mathrm{J}$$
04

Determine the direction of heat flow

Since the calculated heat transfer (\(Q\)) is negative, this means that the heat is flowing out of the gas and into the heat reservoir. In conclusion, the heat flows between the heat reservoir and the gas is \(-5000 \mathrm{J}\), and the direction of the heat flow is from the gas into the heat reservoir.

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Most popular questions from this chapter

A heat engine takes in \(125 \mathrm{kJ}\) of heat from a reservoir at $815 \mathrm{K}\( and exhausts \)82 \mathrm{kJ}\( to a reservoir at \)293 \mathrm{K}$ (a) What is the efficiency of the engine? (b) What is the efficiency of an ideal engine operating between the same two reservoirs?
The United States generates about \(5.0 \times 10^{16} \mathrm{J}\) of electric energy a day. This energy is equivalent to work, since it can be converted into work with almost \(100 \%\) efficiency by an electric motor. (a) If this energy is generated by power plants with an average efficiency of \(0.30,\) how much heat is dumped into the environment each day? (b) How much water would be required to absorb this heat if the water temperature is not to increase more than \(2.0^{\circ} \mathrm{C} ?\)
Show that in a reversible engine the amount of heat \(Q_{C}\) exhausted to the cold reservoir is related to the net work done \(W_{\text {net }}\) by $$ Q_{\mathrm{C}}=\frac{T_{\mathrm{C}}}{T_{\mathrm{H}}-T_{\mathrm{C}}} W_{\mathrm{net}} $$
A town is considering using its lake as a source of power. The average temperature difference from the top to the bottom is \(15^{\circ} \mathrm{C},\) and the average surface temperature is \(22^{\circ} \mathrm{C} .\) (a) Assuming that the town can set up a reversible engine using the surface and bottom of the lake as heat reservoirs, what would be its efficiency? (b) If the town needs about \(1.0 \times 10^{8} \mathrm{W}\) of power to be supplied by the lake, how many \(\mathrm{m}^{3}\) of water does the heat engine use per second? (c) The surface area of the lake is $8.0 \times 10^{7} \mathrm{m}^{2}$ and the average incident intensity (over \(24 \mathrm{h})\) of the sunlight is \(200 \mathrm{W} / \mathrm{m}^{2} .\) Can the lake supply enough heat to meet the town's energy needs with this method?
An engine releases \(0.450 \mathrm{kJ}\) of heat for every \(0.100 \mathrm{kJ}\) of work it does. What is the efficiency of the engine?
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