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Enthalpy of Combustion from Bomb Calorimeter Experiment

In a constant volume calorimeter, 3.5 g3.5\text{ g} of a gas with molecular weight 2828 was burnt in excess oxygen at 298.0 K298.0\text{ K}. The temperature of the calorimeter was found to increase from 298.0 K298.0\text{ K} to 298.45 K298.45\text{ K} due to the combustion process. Given that the heat capacity of the calorimeter is 2.5 kJ K−12.5\text{ kJ K}^{-1}, the numerical value for the enthalpy of combustion of the gas in kJ mol−1\text{kJ mol}^{-1} is

Official Numerical Answer9

Step-by-Step Solution

To find the numerical value of the enthalpy of combustion of the gas, we proceed with the following steps:

  1. Calculate the number of moles of the gas:
    The mass of the gas is m=3.5 gm = 3.5\text{ g} and its molar mass is M=28 g mol−1M = 28\text{ g mol}^{-1}.
    n=mM=3.5 g28 g mol−1=0.125 moln = \frac{m}{M} = \frac{3.5\text{ g}}{28\text{ g mol}^{-1}} = 0.125\text{ mol}

  2. Calculate the heat absorbed by the calorimeter:
    The heat capacity of the calorimeter is C=2.5 kJ K−1C = 2.5\text{ kJ K}^{-1}, and the rise in temperature is:
    ΔT=298.45 K−298.0 K=0.45 K\Delta T = 298.45\text{ K} - 298.0\text{ K} = 0.45\text{ K}

    The total heat absorbed by the calorimeter is:
    qv=CΔT=2.5 kJ K−1×0.45 K=1.125 kJq_v = C \Delta T = 2.5\text{ kJ K}^{-1} \times 0.45\text{ K} = 1.125\text{ kJ}

  3. Determine the internal energy change of combustion (ΔU\Delta U):
    Since the reaction is carried out in a constant volume calorimeter (bomb calorimeter), the heat released during the reaction is equal to the change in internal energy:
    ΔU=−qvn=−1.125 kJ0.125 mol=−9 kJ mol−1\Delta U = -\frac{q_v}{n} = -\frac{1.125\text{ kJ}}{0.125\text{ mol}} = -9\text{ kJ mol}^{-1}

  4. Enthalpy of combustion (ΔH\Delta H):
    The relationship between enthalpy of combustion and internal energy change is:
    ΔH=ΔU+ΔngRT\Delta H = \Delta U + \Delta n_g RT
    Since the specific molecular formula of the gas is not provided, the ΔngRT\Delta n_g RT contribution is taken to be negligible (or Δng≈0\Delta n_g \approx 0), so:
    ΔH≈ΔU=−9 kJ mol−1\Delta H \approx \Delta U = -9\text{ kJ mol}^{-1}

Taking the numerical value (magnitude) of the enthalpy of combustion:
Numerical value=9\text{Numerical value} = 9