Problem 9
Question
If a gas at constant temperature and pressure expands, then its (a) internal energy decreases (b) entropy increases and then decreases (c) internal energy increases (d) internal energy remains constant
Step-by-Step Solution
Verified Answer
The correct answer is (d) internal energy remains constant.
1Step 1: Understanding the Ideal Gas Behavior
For an ideal gas undergoing an isothermal (constant temperature) process, the internal energy depends solely on temperature. Since the temperature is constant, the change in internal energy, according to the first law of thermodynamics, is zero.
2Step 2: Evaluating Changes in Entropy
When a gas expands at constant temperature, its entropy must increase because the gas molecules have more volume to occupy, increasing the disorder or randomness of the system.
3Step 3: Revisiting Internal Energy
Since the internal energy is not directly affected by volume changes in an ideal gas at constant temperature, it remains unchanged.
Key Concepts
Isothermal ProcessFirst Law of ThermodynamicsEntropy
Isothermal Process
In an isothermal process, the temperature remains constant throughout the change, which is a core concept for gases, especially ideal gases. When a gas expands isothermally, it does so at a steady temperature.
This means there's a delicate balance between heat exchange with surroundings and work done by the gas. Even though the system might exchange heat with its surroundings, it doesn’t lead to a temperature change.
This balancing act is crucial in understanding energy dynamics in physical systems.
This means there's a delicate balance between heat exchange with surroundings and work done by the gas. Even though the system might exchange heat with its surroundings, it doesn’t lead to a temperature change.
- Heat absorbed is equal to work done.
- Because temperature remains constant, the internal energy of an ideal gas doesn't change.
This balancing act is crucial in understanding energy dynamics in physical systems.
First Law of Thermodynamics
The first law of thermodynamics is essentially a principle of energy conservation. It is often summarized as, "energy cannot be created or destroyed, only transformed from one form to another."
In the context of an isothermal process for an ideal gas, the first law can be expressed as: ΔU = Q - W, where
This interplay between heat and work showcases how the first law governs energy exchange, particularly in efficient processes like those observed in engines and thermodynamic cycles.
In the context of an isothermal process for an ideal gas, the first law can be expressed as: ΔU = Q - W, where
- ΔU is the change in internal energy.
- Q is the heat added to the system.
- W is the work done by the system.
This interplay between heat and work showcases how the first law governs energy exchange, particularly in efficient processes like those observed in engines and thermodynamic cycles.
Entropy
Entropy is a measure of disorder or randomness in a system, and it plays a significant role in thermodynamic processes. During an isothermal expansion, the entropy of the ideal gas increases. This increase is due to the particles having more volume to spread out and move around, which increases randomness.
Entropy is closely linked to the second law of thermodynamics, which states that entropy of an isolated system always tends to increase over time. This principle helps explain the natural tendency towards equilibrium.
Entropy is closely linked to the second law of thermodynamics, which states that entropy of an isolated system always tends to increase over time. This principle helps explain the natural tendency towards equilibrium.
- Entropy change can be calculated using the equation: ΔS = rac{Q}{T}, where ΔS is the change in entropy, Q is the heat exchanged, and T is the temperature.
- In any real process, some energy will become unavailable for doing useful work, accounting for the natural tendency toward increasing disorder.
Other exercises in this chapter
Problem 7
In thermodynamics, a process is called reversible when (a) the surroundings are always in equilibrium with the system (b) there is no boundary between system an
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