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When the pressure of a gas is doubled un...

When the pressure of a gas is doubled under constant temperature the density becomes

A

double

B

halved

C

does not change

D

decrease to 1/4.

Text Solution

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The correct Answer is:
To solve the problem of how the density of a gas changes when its pressure is doubled at constant temperature, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Ideal Gas Law**: The ideal gas law is given by the equation: \[ PV = nRT \] where \( P \) is the pressure, \( V \) is the volume, \( n \) is the number of moles of gas, \( R \) is the ideal gas constant, and \( T \) is the temperature. 2. **Identify Constant Parameters**: Since the temperature is constant, \( R \) and \( n \) are also constant. Therefore, the product \( PV \) must remain constant. 3. **Set Up Initial and Final Conditions**: Let the initial pressure be \( P \) and the initial volume be \( V \). Thus, the initial state can be represented as: \[ P_1V_1 = PV \] After the pressure is doubled, the new pressure \( P_2 \) becomes: \[ P_2 = 2P \] Let the new volume be \( V' \). Then, the new state can be represented as: \[ P_2V' = (2P)V' \] 4. **Apply the Ideal Gas Law**: Since \( PV = nRT \) remains constant, we can equate the two states: \[ PV = (2P)V' \] Cancelling \( P \) from both sides (assuming \( P \neq 0 \)): \[ V = 2V' \] This implies: \[ V' = \frac{V}{2} \] Therefore, when the pressure is doubled, the volume is halved. 5. **Relate Density to Volume**: The density \( \rho \) of a gas is defined as: \[ \rho = \frac{m}{V} \] where \( m \) is the mass of the gas. 6. **Calculate New Density**: Initially, the density is: \[ \rho_1 = \frac{m}{V} \] After the pressure is doubled and the volume is halved, the new density \( \rho' \) becomes: \[ \rho' = \frac{m}{V'} = \frac{m}{\frac{V}{2}} = \frac{2m}{V} = 2\rho_1 \] 7. **Conclusion**: Thus, when the pressure of a gas is doubled under constant temperature, the density of the gas becomes doubled. ### Final Answer: The density becomes **doubled**. ---
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