The amount of heat needed to raise the temperature of a gas is given by the formula: \[ Q = n C \Delta T \] Where:
- \( n \) is the number of moles of the gas,
- \( C \) is the molar heat capacity at constant volume,
- \( \Delta T \) is the change in temperature.
Given: - The gas is hydrogen, so \( C = 8.31 \, \text{J mol}^{-1} \, \text{K}^{-1} \), - The cylinder's capacity is \( 44.81 \, \text{L} \), and at STP, 1 mole of gas occupies 22.4 L, so: \[ n = \frac{44.81}{22.4} \approx 2 \, \text{mol} \] - The temperature change is \( \Delta T = 20 \, \text{C} \). Now, substitute the values: \[ Q = 2 \, \text{mol} \times 8.31 \, \text{J mol}^{-1} \, \text{K}^{-1} \times 20 \, \text{K} \] \[ Q = 831 \, \text{J} \]
Thus, the amount of heat needed is 831 J.
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: