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An ideal gas of one mole is kept in a ri...

An ideal gas of one mole is kept in a rigid container of negligible heat capacity. If `25J` of heat is supplied the gas temperature raises by `2^(@)C`. Then the gas may be

A

helium

B

argon

C

oxygen

D

carbon dioxide

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To solve the problem, we will follow these steps: ### Step 1: Understand the System We have an ideal gas in a rigid container with negligible heat capacity. This means that the volume of the gas does not change (rigid container) and that the container does not absorb heat. ### Step 2: Apply the First Law of Thermodynamics The first law of thermodynamics states: \[ \Delta U = Q - W \] Where: - \(\Delta U\) is the change in internal energy, - \(Q\) is the heat added to the system, - \(W\) is the work done by the system. Since the container is rigid, the work done \(W = 0\). Therefore, we can simplify the equation to: \[ \Delta U = Q \] ### Step 3: Substitute Known Values We know from the problem that: - Heat supplied \(Q = 25 \, \text{J}\) - The temperature change \(\Delta T = 2 \, \text{°C} = 2 \, \text{K}\) (since the size of the degree is the same in Celsius and Kelvin). Thus, we have: \[ \Delta U = 25 \, \text{J} \] ### Step 4: Relate Change in Internal Energy to Molar Heat Capacity The change in internal energy for an ideal gas can also be expressed as: \[ \Delta U = n C_v \Delta T \] Where: - \(n\) is the number of moles (given as 1 mole), - \(C_v\) is the molar heat capacity at constant volume, - \(\Delta T\) is the change in temperature. Substituting the known values: \[ 25 \, \text{J} = 1 \, \text{mol} \cdot C_v \cdot 2 \, \text{K} \] ### Step 5: Solve for \(C_v\) Rearranging the equation gives: \[ C_v = \frac{25 \, \text{J}}{2 \, \text{K}} = 12.5 \, \text{J/K} \] ### Step 6: Determine the Type of Gas The molar heat capacities for different types of gases are: - Monatomic gases (like Helium and Argon): \(C_v = \frac{3}{2} R\) - Diatomic gases (like Oxygen): \(C_v = \frac{5}{2} R\) - Polyatomic gases (like Carbon Dioxide): \(C_v\) is greater than for diatomic gases. Using the universal gas constant \(R \approx 8.31 \, \text{J/(mol K)}\): \[ C_v \text{ (monatomic)} = \frac{3}{2} R = \frac{3}{2} \times 8.31 \approx 12.46 \, \text{J/K} \] \[ C_v \text{ (diatomic)} = \frac{5}{2} R = \frac{5}{2} \times 8.31 \approx 20.78 \, \text{J/K} \] Since \(C_v \approx 12.5 \, \text{J/K}\) is close to the value for a monatomic gas, we conclude that the gas could be either Helium or Argon. ### Final Answer The gas may be Helium or Argon. ---
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