To solve the problem, we need to calculate the work done by one mole of helium when given 48 J of heat, causing its temperature to increase by \(2^\circ C\).
First, we understand the process: Helium is a monoatomic ideal gas. The given parameters are:
We use the first law of thermodynamics, which states:
\(Q = \Delta U + W\)
Where:
For a monoatomic ideal gas, the change in internal energy (\(\Delta U\)) can be given by:
\(\Delta U = \frac{3}{2}nR\Delta T\)
Since we have one mole of helium, \(n = 1\). Substituting the given values, we get:
\(\Delta U = \frac{3}{2} \times 1 \times 8.3 \times 2 = 24.9 \, \text{J}\)
Substituting \(\Delta U\) back into the first law equation:
\(48 = 24.9 + W\)
Solving for \(W\):
\(W = 48 - 24.9 = 23.1 \, \text{J}\)
Thus, the work done by the gas is 23.1 J. This matches the correct option provided.
Using the first law of thermodynamics:
\[\Delta Q = \Delta U + W\]
\[31\]
Given:
\[+48 = n C_V \Delta T + W\]
For helium (a monoatomic gas), \( C_V = \frac{3R}{2} \):
\[48 = (1) \left( \frac{3R}{2} \right) (2) + W\]
Simplifying:
\[W = 48 - 3 \times R\]
Substitute \( R = 8.3 \):
\[W = 48 - 3 \times (8.3)\]
\[W = 23.1 \, \text{Joule}\]
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:
The major product (A) formed in the following reaction sequence is
