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200 cm^(3) of a gas is compressed to 100...

`200 cm^(3)` of a gas is compressed to `100cm^(3)` at atmospheric pressure `(10^(6) "dyne"//cm^(2))`. Find the resultant pressure if the change is (i) slow (ii) sudden Take `gamma= 1.4`.

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To solve the problem step by step, we will analyze both scenarios: (i) slow compression and (ii) sudden compression. ### Given Data: - Initial Volume, \( V_1 = 200 \, \text{cm}^3 \) - Final Volume, \( V_2 = 100 \, \text{cm}^3 \) - Initial Pressure, \( P_1 = 10^6 \, \text{dyne/cm}^2 \) - \( \gamma = 1.4 \) ### Part (i): Slow Compression (Isothermal Process) 1. **Understanding the Process**: - In a slow compression, the process is quasi-static, meaning the system is in equilibrium at all times. This results in an isothermal process (constant temperature). 2. **Using the Ideal Gas Law**: - For an isothermal process, the relationship between pressure and volume is given by: \[ P_1 V_1 = P_2 V_2 \] 3. **Rearranging the Equation**: - We can rearrange this equation to find the final pressure \( P_2 \): \[ P_2 = P_1 \frac{V_1}{V_2} \] 4. **Substituting the Values**: - Plugging in the values: \[ P_2 = 10^6 \, \text{dyne/cm}^2 \times \frac{200 \, \text{cm}^3}{100 \, \text{cm}^3} \] \[ P_2 = 10^6 \, \text{dyne/cm}^2 \times 2 = 2 \times 10^6 \, \text{dyne/cm}^2 \] 5. **Converting to Atmospheres**: - Since \( 1 \, \text{atm} = 10^6 \, \text{dyne/cm}^2 \): \[ P_2 = 2 \, \text{atm} \] ### Part (ii): Sudden Compression (Adiabatic Process) 1. **Understanding the Process**: - In a sudden compression, the gas does not have time to exchange heat with its surroundings, resulting in an adiabatic process. 2. **Using the Adiabatic Condition**: - For an adiabatic process, the relationship between pressure and volume is given by: \[ P_1 V_1^\gamma = P_2 V_2^\gamma \] 3. **Rearranging the Equation**: - Rearranging to find \( P_2 \): \[ P_2 = P_1 \left( \frac{V_1}{V_2} \right)^\gamma \] 4. **Substituting the Values**: - Plugging in the values: \[ P_2 = 10^6 \, \text{dyne/cm}^2 \left( \frac{200 \, \text{cm}^3}{100 \, \text{cm}^3} \right)^{1.4} \] \[ P_2 = 10^6 \, \text{dyne/cm}^2 \times (2)^{1.4} \] 5. **Calculating \( (2)^{1.4} \)**: - Using a calculator: \[ (2)^{1.4} \approx 2.639 \] 6. **Final Calculation**: - Therefore: \[ P_2 = 10^6 \, \text{dyne/cm}^2 \times 2.639 \approx 2.639 \times 10^6 \, \text{dyne/cm}^2 \] 7. **Converting to Atmospheres**: - Converting to atmospheres: \[ P_2 \approx 2.639 \, \text{atm} \] ### Final Answers: - (i) For slow compression, the resultant pressure is \( 2 \, \text{atm} \). - (ii) For sudden compression, the resultant pressure is approximately \( 2.639 \, \text{atm} \).

To solve the problem step by step, we will analyze both scenarios: (i) slow compression and (ii) sudden compression. ### Given Data: - Initial Volume, \( V_1 = 200 \, \text{cm}^3 \) - Final Volume, \( V_2 = 100 \, \text{cm}^3 \) - Initial Pressure, \( P_1 = 10^6 \, \text{dyne/cm}^2 \) - \( \gamma = 1.4 \) ...
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