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Change in enthalpy and change in interna...

Change in enthalpy and change in internal energy are state functions. The value of `DeltaH, DeltaU` can be determined by using Kirchoff's equation.
Calculate `DeltaH` when `10dm^(3)` of helium at NTP is heated in a cylinder to `100^(@)C`, assuming that the gas behave ideally.

A

927.9J

B

279.2J

C

729.3J

D

999J

Text Solution

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The correct Answer is:
To calculate the change in enthalpy (ΔH) when heating 10 dm³ of helium at normal temperature and pressure (NTP) to 100°C, we can follow these steps: ### Step 1: Determine the number of moles of helium (N) At NTP, the molar volume of an ideal gas is approximately 22.4 dm³/mol. \[ N = \frac{\text{Volume}}{\text{Molar Volume}} = \frac{10 \, \text{dm}^3}{22.4 \, \text{dm}^3/\text{mol}} \approx 0.4464 \, \text{mol} \] ### Step 2: Calculate the heat capacity at constant pressure (Cₚ) For a monoatomic ideal gas like helium, the specific heat at constant volume (Cᵥ) is given by: \[ Cᵥ = \frac{3}{2} R \] Where R is the universal gas constant (8.314 J/(mol·K)). Therefore, \[ Cᵥ = \frac{3}{2} \times 8.314 \approx 12.471 \, \text{J/(mol·K)} \] Now, using the relation \(Cₚ = Cᵥ + R\): \[ Cₚ = Cᵥ + R = \frac{3}{2} R + R = \frac{5}{2} R \] Calculating \(Cₚ\): \[ Cₚ = \frac{5}{2} \times 8.314 \approx 20.785 \, \text{J/(mol·K)} \] ### Step 3: Calculate the change in temperature (ΔT) The initial temperature (T₁) is 0°C (or 273.15 K) and the final temperature (T₂) is 100°C (or 373.15 K). \[ \Delta T = T₂ - T₁ = 373.15 \, \text{K} - 273.15 \, \text{K} = 100 \, \text{K} \] ### Step 4: Calculate the change in enthalpy (ΔH) Using the formula for enthalpy change: \[ \Delta H = N \cdot Cₚ \cdot \Delta T \] Substituting the values we calculated: \[ \Delta H = 0.4464 \, \text{mol} \cdot 20.785 \, \text{J/(mol·K)} \cdot 100 \, \text{K} \] Calculating ΔH: \[ \Delta H \approx 0.4464 \cdot 20.785 \cdot 100 \approx 927.90 \, \text{J} \] ### Final Answer: The change in enthalpy (ΔH) when heating 10 dm³ of helium to 100°C is approximately **927.90 J**. ---
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