The formula for work done during an isothermal expansion of an ideal gas is given by:
\(\text{Work} = nRT \ln \left(\frac{V_f}{V_i}\right)\)
Where:
Now, plug the values into the formula:
\(\text{Work} = 2 \times 8.314 \times 300 \times \ln \left(\frac{3}{1}\right)\)
Calculating the natural logarithm:
\(\ln \left(\frac{3}{1}\right) = \ln(3) \approx 1.0986\)
Substitute into the equation:
\(\text{Work} = 2 \times 8.314 \times 300 \times 1.0986 \approx 5478.4 \text{ J}\)
Thus, the work done by the gas is approximately 5478.4 J.
The internal energy of air in $ 4 \, \text{m} \times 4 \, \text{m} \times 3 \, \text{m} $ sized room at 1 atmospheric pressure will be $ \times 10^6 \, \text{J} $. (Consider air as a diatomic molecule)
An ideal gas has undergone through the cyclic process as shown in the figure. Work done by the gas in the entire cycle is _____ $ \times 10^{-1} $ J. (Take $ \pi = 3.14 $) 