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A diatomic gas of molecular mass 40 g/mo...

A diatomic gas of molecular mass 40 g/mol is filled in rigid container at temperature `30^@ C`. It is moving with velocity 200 m/s. If its is suddenly stopped, the rise in the temperature of the gas is

A

`(32)/(R ) ""^(@) C`

B

`(320)/(R ) ""^(@) C`

C

`(3200)/( R )""^(@ ) C`

D

`(3.2)/(R ) ""^@ C`

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The correct Answer is:
To solve the problem, we need to find the rise in temperature of a diatomic gas when it is suddenly stopped. The steps to solve this are as follows: ### Step 1: Identify the given data - Molecular mass of the gas, \( M = 40 \, \text{g/mol} \) - Initial temperature, \( T_i = 30^\circ C = 303 \, \text{K} \) - Velocity of the gas, \( v = 200 \, \text{m/s} \) ### Step 2: Convert the molecular mass to kg Since we need to work in SI units, we convert the molecular mass from grams to kilograms: \[ M = 40 \, \text{g/mol} = 40 \times 10^{-3} \, \text{kg/mol} \] ### Step 3: Calculate the kinetic energy of the gas The kinetic energy \( KE \) of the gas can be calculated using the formula: \[ KE = \frac{1}{2} m v^2 \] Where \( m \) is the mass of the gas in kg. If we have \( N \) moles of gas, then the total mass \( m \) is: \[ m = N \times M = N \times 40 \times 10^{-3} \, \text{kg} \] Thus, the kinetic energy becomes: \[ KE = \frac{1}{2} (N \times 40 \times 10^{-3}) v^2 \] Substituting \( v = 200 \, \text{m/s} \): \[ KE = \frac{1}{2} (N \times 40 \times 10^{-3}) (200)^2 \] \[ KE = \frac{1}{2} (N \times 40 \times 10^{-3}) \times 40000 \] \[ KE = 800N \, \text{J} \] ### Step 4: Relate kinetic energy to internal energy change When the gas is suddenly stopped, the kinetic energy is converted to internal energy. For a diatomic gas, the change in internal energy \( \Delta U \) is given by: \[ \Delta U = \frac{F}{2} N R \Delta T \] Where: - \( F = 5 \) (degrees of freedom for a diatomic gas) - \( R = 8.314 \, \text{J/(mol K)} \) ### Step 5: Set kinetic energy equal to change in internal energy Setting the kinetic energy equal to the change in internal energy: \[ 800N = \frac{5}{2} N R \Delta T \] We can cancel \( N \) from both sides (assuming \( N \neq 0 \)): \[ 800 = \frac{5}{2} R \Delta T \] ### Step 6: Solve for \( \Delta T \) Rearranging the equation to find \( \Delta T \): \[ \Delta T = \frac{800 \times 2}{5R} \] Substituting \( R = 8.314 \): \[ \Delta T = \frac{1600}{5 \times 8.314} \] \[ \Delta T = \frac{1600}{41.57} \approx 38.5 \, \text{K} \] ### Step 7: Conclusion The rise in temperature of the gas is approximately \( 38.5 \, \text{K} \).
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