A beaker with a metal bottom is filled with 17 g of water at 20 °C. It is brought into good thermal contact with a 4000 cm³ container holding 0.50 mol of a monatomic gas at 10 atm pressure. Both containers are well insulated from their surroundings. (Figure 1) Figure Insulation Water Gas 1 of 1 > Thin metal What is the gas pressure after a long time has elapsed? You can assume that the containers themselves are nearly massless and do not affect the outcome. Express your answer with the appropriate units. p= Value Submit Provide Feedback A Request Answer Units Big 11 ? Next >

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### Thermodynamics Problem: Gas Pressure in an Insulated Container

#### Problem Statement
A beaker with a metal bottom is filled with 17 g of water at 20 °C. It is brought into good thermal contact with a 4000 cm³ container holding 0.50 mol of a monatomic gas at 10 atm pressure. Both containers are well insulated from their surroundings.

![Figure 1](pathway/to/image)

**Figure 1:**
- **Description:**
    - The diagram shows a water-filled beaker mounted above a container with gas. 
    - The water is separated from the gas by a thin metal layer, facilitating heat transfer.
    - Both the beaker and the gas container are enclosed with insulation to ensure no heat exchange with the surroundings.

#### Task
Determine the gas pressure after a long time has elapsed. You can assume that the containers themselves are nearly massless and do not affect the outcome.

#### Solution
To find the final pressure of the gas, use the principle of conservation of energy. Here's the step-by-step approach:

1. **Conservation of Energy:** 
   - The heat lost by the gas equals the heat gained by the water.
   
2. **Heat Transfer Equation:**
   - \( Q = nC_v\Delta T \) for the gas, where \( Q \) is the heat, \( n \) is the number of moles, \( C_v \) is the specific heat capacity, and \( \Delta T \) is the temperature change.
   - \( Q = mC_w\Delta T \) for the water, where \( m \) is the mass, \( C_w \) is the specific heat capacity, and \( \Delta T \) is the temperature change.

3. **Ideal Gas Law:**
   - \( PV = nRT \)

4. **Heat Exchange:**
   - Let \( T_f \) be the final temperature for both the gas and the water after thermal equilibrium is reached.

5. **Expressing the Final Pressure:**
   - Relate the final temperature back to the pressure using the ideal gas law.

**Work through the equations carefully to solve for the final pressure, `p`, and ensure to express your answer in appropriate units. Provide inputs where needed, such as specific heat capacities and conversion constants.**

*Note: This problem involves a detailed step-by-step approach to reach the solution. If any steps are
Transcribed Image Text:### Thermodynamics Problem: Gas Pressure in an Insulated Container #### Problem Statement A beaker with a metal bottom is filled with 17 g of water at 20 °C. It is brought into good thermal contact with a 4000 cm³ container holding 0.50 mol of a monatomic gas at 10 atm pressure. Both containers are well insulated from their surroundings. ![Figure 1](pathway/to/image) **Figure 1:** - **Description:** - The diagram shows a water-filled beaker mounted above a container with gas. - The water is separated from the gas by a thin metal layer, facilitating heat transfer. - Both the beaker and the gas container are enclosed with insulation to ensure no heat exchange with the surroundings. #### Task Determine the gas pressure after a long time has elapsed. You can assume that the containers themselves are nearly massless and do not affect the outcome. #### Solution To find the final pressure of the gas, use the principle of conservation of energy. Here's the step-by-step approach: 1. **Conservation of Energy:** - The heat lost by the gas equals the heat gained by the water. 2. **Heat Transfer Equation:** - \( Q = nC_v\Delta T \) for the gas, where \( Q \) is the heat, \( n \) is the number of moles, \( C_v \) is the specific heat capacity, and \( \Delta T \) is the temperature change. - \( Q = mC_w\Delta T \) for the water, where \( m \) is the mass, \( C_w \) is the specific heat capacity, and \( \Delta T \) is the temperature change. 3. **Ideal Gas Law:** - \( PV = nRT \) 4. **Heat Exchange:** - Let \( T_f \) be the final temperature for both the gas and the water after thermal equilibrium is reached. 5. **Expressing the Final Pressure:** - Relate the final temperature back to the pressure using the ideal gas law. **Work through the equations carefully to solve for the final pressure, `p`, and ensure to express your answer in appropriate units. Provide inputs where needed, such as specific heat capacities and conversion constants.** *Note: This problem involves a detailed step-by-step approach to reach the solution. If any steps are
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