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The temperature of 4.0 mol of an ideal g...

The temperature of 4.0 mol of an ideal gas occupying `5dm^(3)` at 3.32 bar `(R="0.083 bar dm"^(3)K^(-1)"mol"^(-1))` is `nxx10K`. The value of n is

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To find the value of \( n \) in the temperature expression \( n \times 10^k \) for the given ideal gas, we will use the Ideal Gas Law equation: ### Step-by-Step Solution: 1. **Identify Given Values:** - Number of moles, \( n = 4.0 \, \text{mol} \) - Volume, \( V = 5 \, \text{dm}^3 \) - Pressure, \( P = 3.32 \, \text{bar} \) - Ideal Gas Constant, \( R = 0.083 \, \text{bar} \, \text{dm}^3 \, \text{K}^{-1} \, \text{mol}^{-1} \) 2. **Use the Ideal Gas Law:** The Ideal Gas Law is given by the equation: \[ PV = nRT \] Rearranging the equation to solve for temperature \( T \): \[ T = \frac{PV}{nR} \] 3. **Substitute the Known Values:** Now, substitute the values into the equation: \[ T = \frac{(3.32 \, \text{bar}) \times (5 \, \text{dm}^3)}{(4.0 \, \text{mol}) \times (0.083 \, \text{bar} \, \text{dm}^3 \, \text{K}^{-1} \, \text{mol}^{-1})} \] 4. **Calculate the Numerator:** Calculate the numerator: \[ 3.32 \times 5 = 16.6 \, \text{bar} \, \text{dm}^3 \] 5. **Calculate the Denominator:** Calculate the denominator: \[ 4.0 \times 0.083 = 0.332 \, \text{bar} \, \text{dm}^3 \, \text{K}^{-1} \, \text{mol}^{-1} \] 6. **Calculate Temperature \( T \):** Now, divide the numerator by the denominator: \[ T = \frac{16.6}{0.332} \approx 50 \, \text{K} \] 7. **Express Temperature in the Required Form:** We know that the temperature can be expressed as \( T = n \times 10^k \). Here, we have: \[ 50 \, \text{K} = n \times 10^1 \] This implies: \[ n = \frac{50}{10} = 5 \] ### Final Answer: The value of \( n \) is \( 5 \). ---

To find the value of \( n \) in the temperature expression \( n \times 10^k \) for the given ideal gas, we will use the Ideal Gas Law equation: ### Step-by-Step Solution: 1. **Identify Given Values:** - Number of moles, \( n = 4.0 \, \text{mol} \) - Volume, \( V = 5 \, \text{dm}^3 \) - Pressure, \( P = 3.32 \, \text{bar} \) ...
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