
The work done by the gas in a reversible isothermal process can be calculated using the formula:
\( W = nRT \ln\left(\frac{V_f}{V_i}\right) \)
Where:
Substitute the values into the formula:
\( W = 1 \times 0.08206 \times 291.15 \times \ln\left(\frac{100}{10}\right) \)
\( W = 23.89989 \times \ln(10) \)
\( \ln(10) = 2.302 \) (approx.)
\( W \approx 23.89989 \times 2.302 \approx 55.028 \)
To the nearest integer, \( W = 55 \, \text{L atm} \).
This value falls within the expected range of 55, verifying its correctness.
Work done ($W$) in an isothermal reversible expansion of an ideal gas is given by:
\[W = -nRT \ln \left( \frac{V_2}{V_1} \right)\]
Given:
\[n = 1 \, \text{mol}, \quad T = 18^\circ \text{C} = 18 + 273.15 = 291.15 \, \text{K}\]
\[V_1 = 10 \, \text{L}, \quad V_2 = 100 \, \text{L}\]
Substitute the values:
\[W = -1 \times 0.08206 \times 291.15 \times \ln \left( \frac{100}{10} \right)\]
\[W \approx -1 \times 0.08206 \times 291.15 \times \ln(10)\]
\[W \approx -55.0128 \, \text{L atm}\]
The work done by the system is approximately $-55 \, \text{L atm}$ (rounded to nearest integer).
A piston of mass M is hung from a massless spring whose restoring force law goes as F = -kx, where k is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature T) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $ L_0 $ to $ L_1 $, the total energy delivered by the filament is (Assume spring to be in its natural length before heating) 
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals:
Designate whether each of the following compounds is aromatic or not aromatic.

The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)