In which of the following scenarios is no change in the internal energy of the system possible? O q<0, w=0 O q<0, w > 0 O q = 0, w > 0 O q<0, w < 0 O q> 0, w > 0

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### Understanding Changes in Internal Energy

**Question:** In which of the following scenarios is **no change** in the internal energy of the system possible?

1. \( q < 0, w = 0 \)
2. \( q < 0, w > 0 \)
3. \( q = 0, w > 0 \)
4. \( q < 0, w < 0 \)
5. \( q > 0, w > 0 \)

**Explanation:**
To identify the scenario where there is no change in the internal energy (\(\Delta U = 0\)) of the system, we can use the First Law of Thermodynamics, which is expressed as:

\[ \Delta U = q + w \]

Where
- \(\Delta U\) is the change in internal energy,
- \(q\) is the heat exchanged (with \(q > 0\) indicating heat absorbed by the system and \(q < 0\) indicating heat released by the system),
- \(w\) is the work done on the system (with \(w > 0\) indicating work done on the system and \(w < 0\) indicating work done by the system).

For the internal energy to remain unchanged (\(\Delta U = 0\)), the sum of \(q\) and \(w\) must be zero:

\[ q + w = 0 \]

Among the given options:

1. \( q < 0, w = 0 \): The system releases heat, but no work is done, so \(\Delta U \neq 0\).

2. \( q < 0, w > 0 \): The system releases heat (\( q < 0 \)), and work is done on the system (\( w > 0 \)). If the magnitudes of \(q\) and \(w\) are such that \( |q| = w \), then \( q + w = 0 \).
   
   This is the correct scenario where no change in internal energy is possible. 

3. \( q = 0, w > 0 \): No heat exchange, and work is done on the system, so \(\Delta U \neq 0\).

4. \( q < 0, w < 0 \): The system releases heat, and work is done by the system, so \(\Delta U \neq 0
Transcribed Image Text:### Understanding Changes in Internal Energy **Question:** In which of the following scenarios is **no change** in the internal energy of the system possible? 1. \( q < 0, w = 0 \) 2. \( q < 0, w > 0 \) 3. \( q = 0, w > 0 \) 4. \( q < 0, w < 0 \) 5. \( q > 0, w > 0 \) **Explanation:** To identify the scenario where there is no change in the internal energy (\(\Delta U = 0\)) of the system, we can use the First Law of Thermodynamics, which is expressed as: \[ \Delta U = q + w \] Where - \(\Delta U\) is the change in internal energy, - \(q\) is the heat exchanged (with \(q > 0\) indicating heat absorbed by the system and \(q < 0\) indicating heat released by the system), - \(w\) is the work done on the system (with \(w > 0\) indicating work done on the system and \(w < 0\) indicating work done by the system). For the internal energy to remain unchanged (\(\Delta U = 0\)), the sum of \(q\) and \(w\) must be zero: \[ q + w = 0 \] Among the given options: 1. \( q < 0, w = 0 \): The system releases heat, but no work is done, so \(\Delta U \neq 0\). 2. \( q < 0, w > 0 \): The system releases heat (\( q < 0 \)), and work is done on the system (\( w > 0 \)). If the magnitudes of \(q\) and \(w\) are such that \( |q| = w \), then \( q + w = 0 \). This is the correct scenario where no change in internal energy is possible. 3. \( q = 0, w > 0 \): No heat exchange, and work is done on the system, so \(\Delta U \neq 0\). 4. \( q < 0, w < 0 \): The system releases heat, and work is done by the system, so \(\Delta U \neq 0
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