the first law of thermodynamics
Step 1. Understanding the Work Done on the Gas
To find the work done on the gas, we use the formula for work done at constant pressure:
$$ \text{Work done} = p \Delta V $$
where:
- $$ p $$ is the pressure,
- $$ \Delta V $$ is the change in volume.
Given:
- $$ p = 2.0 \times 10^5 \, \text{Pa} $$,
- Initial volume $$ V_i = 0.038 \, \text{m}^3 $$,
- Final volume $$ V_f = 0.063 \, \text{m}^3 $$.
Calculate the change in volume:
$$ \Delta V = V_f - V_i = 0.063 - 0.038 = 0.025 \, \text{m}^3 $$
Now, calculate the work done:
$$ \text{Work done} = 2.0 \times 10^5 \times 0.025 = 5000 \, \text{J} $$
Step 2. Determining the Sign of the Work Done
Since the gas is expanding against an external pressure, the work is done by the gas on the surroundings.
Therefore, the work done on the gas is negative.
Step 3. Calculating the Thermal Energy Transferred
The first law of thermodynamics relates the change in internal energy ($$ \Delta U $$), the heat added to the system ($$ q $$), and the work done by the system ($$ W $$):
$$ \Delta U = q + W $$
Given:
- $$ \Delta U = 7600 \, \text{J} $$,
- Work done by the gas $$ W = -5000 \, \text{J} $$ (since work done on the gas is negative).
Rearrange the formula to solve for $$ q $$:
$$ q = \Delta U - W = 7600 - (-5000) = 7600 + 5000 = 12600 \, \text{J} $$
Step 4. Calculating the Specific Heat Capacity
The specific heat capacity ($$ c $$) is calculated using the formula:
$$ c = \frac{q}{m \Delta T} $$
where:
- $$ q = 12600 \, \text{J} $$,
- $$ m = 0.35 \, \text{kg} $$,
- $$ \Delta T = 56 \, \text{K} $$ (since the temperature change in Celsius is equivalent to Kelvin).
Substitute the values into the formula:
$$ c = \frac{12600}{0.35 \times 56} $$
Calculate:
$$ c = \frac{12600}{19.6} = 642.86 \, \text{J} \, \text{kg}^{-1} \, \text{K}^{-1} $$
Rounding to three significant figures, the specific heat capacity is:
$$ c = 640 \, \text{J} \, \text{kg}^{-1} \, \text{K}^{-1} $$
This completes the problem-solving process, confirming the calculations and understanding of the thermodynamic principles involved.