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I An ideal gas expands at constant pressure. (a) Show that \(P \Delta V=n R \Delta T\). (b) If the gas is monatomic, start from the definition of internal energy and show that \(\Delta U=\frac{3}{2} W_{\mathrm{ew}}\), where \(W_{\mathrm{ew}}\) is the work done by the gas on its environment. (c) For the same monatomic ideal gas, show with the first law that \(Q=\frac{1}{2} W_{\text {eww }}\). (d) Is it possible for an ideal gas to expand at constant pressure while exhausting thermal energy? Explain.

Short Answer

Expert verified
Yes, it is possible for an ideal gas to expand at constant pressure while exhausting thermal energy only if heat is added to the system.

Step by step solution

01

Application of Ideal Gas Law

Remember the Ideal Gas Law: \( PV = nRT \) where P is pressure, V is volume, n is number of moles, R is the ideal gas constant, and T is temperature in Kelvin. Multiply both sides by delta (\( \Delta \)) and use the fact that pressure is constant to show that \( P \Delta V = n R \Delta T \).
02

Definition of Internal Energy

Recall that for an ideal gas, the change in internal energy (\( \Delta U \)) is related to the work done (\( W_{ew} \)) by the equation: \( \Delta U = \frac{3}{2}W_{ew} \).
03

Applying First Law of Thermodynamics

Using the First Law of Thermodynamics, which states that the change in internal energy of a system is equal to the heat added to the system (\( Q \)) minus the work done by the system (\( W_{ew} \)), you can substitute the equation from Step 2 into the First Law to derive: \( Q=\frac{1}{2} W_{ew} \).
04

Interpretation of Results

For an ideal gas to expand at constant pressure, the gas needs to perform work on its surroundings, which decreases the internal energy of the system. The internal energy can only be replenished if heat is added to the system. Therefore, if no heat is added (i.e. the system is adiabatic), the internal energy will decrease due to the work done, leading to a drop in temperature. Hence, a gas cannot expand adiabatically at constant pressure while exhausting thermal energy.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

First Law of Thermodynamics
The First Law of Thermodynamics is a fundamental principle which states that energy cannot be created or destroyed in an isolated system. It is often written as \[\begin{equation}\Delta U = Q - W\end{equation}\]where \(\Delta U\) is the change in internal energy of the system, \(Q\) is the heat added to the system, and \(W\) is the work done by the system on its surroundings. In the context of an ideal gas expanding at constant pressure, the work done by the gas (\(W_{\text{ew}}\)) is the force applied over distance, which translates to pressure times the change in volume (\[\begin{equation}W_{\text{ew}} = P \Delta V\end{equation}\]). Understanding the interplay between heat, work, and internal energy is crucial for interpreting physical processes and solving problems related to thermodynamics.Substituting the definition of work into the First Law allows you to relate heat transfer to the work done by the gas, offering a way to quantify how energy transfers occur in thermodynamic systems.
Internal Energy
Internal Energy is a key concept in thermodynamics, referring to the total energy contained within a system, attributable to the kinetic and potential energy of the molecules. In the case of an ideal gas, the internal energy is primarily kinetic energy since the potential energy between non-interacting particles is negligible. The equation \[\begin{equation}\Delta U = \frac{3}{2} W_{\text{ew}}\end{equation}\]shows that the change in internal energy (\(\Delta U\)) for a monatomic ideal gas, which has three degrees of freedom, is related to the work done on the environment (\(W_{\text{ew}}\)). When the gas expands under constant pressure, it does work on the surroundings, and this work directly affects its internal energy. This equation gives us a quantitative measure of how the energy of a gas changes as it does work during an expansion or compression process.
Thermal Expansion of Gases
Thermal Expansion of Gases is a concept that describes how gases change in volume in response to changes in temperature, assuming a constant pressure (known as Charles's Law). This is given by the equation \[\begin{equation}P \Delta V = nR \Delta T\end{equation}\]which is derived from the Ideal Gas Law. Here, \(\Delta V\) represents the change in volume, and \(\Delta T\) is the change in temperature in Kelvin. This behavior is crucial for understanding how gases will react in different situations, like when heat is added or removed. Thus, when a gas is heated, the increase in kinetic energy of the particles leads to an increase in volume if the pressure remains constant. Conversely, when a gas is cooled, its volume will decrease under the same conditions. The understanding of thermal expansion is significant in engineering applications and in real-life scenarios, such as when designing containers for gases that must withstand varying temperatures.

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Most popular questions from this chapter

BIO Sweating is one of the main mechanisms with which the body dissipates heat. Sweat evaporates with a latent heat of \(2430 \mathrm{~kJ} / \mathrm{kg}\) at body temperature, and the body can produce as much as \(1.5 \mathrm{~kg}\) of sweat per hour. If sweating were the only heat dissipation mechanism, what would be the maximum sustainable metabolic rate, in watts, if \(80 \%\) of the energy used by the body goes into waste heat?

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