An ideal gas goes from state A to state B via three different processes as indicated in the p-V diagram. $ Q_1 $, $ Q_2 $, and $ Q_3 $ indicate the heat absorbed by the three processes and $ \Delta U_1 $, $ \Delta U_2 $, and $ \Delta U_3 $ indicate the change in internal energy along the three processes respectively, then
\( Q_1 > Q_2 > Q_3 \) and \( \Delta U_1 = \Delta U_2 = \Delta U_3 \)
\( Q_2 > Q_1 > Q_3 \) and \( \Delta U_1 = \Delta U_2 = \Delta U_3 \)
\( Q_3 > Q_2 > Q_1 \) and \( \Delta U_1 = \Delta U_2 = \Delta U_3 \)
\( Q_1 > Q_3 > Q_2 \) and \( \Delta U_1 = \Delta U_2 = \Delta U_3 \)
Solution:
We need to analyze the given problem using the first law of thermodynamics, which states:
\( \Delta U = Q - W \)
Where:
In a p-V diagram, the work done by the system is represented by the area under the process curve between two states. While it is not described explicitly, we conclude the relative sizes of these areas based on the options provided and likely paths implied by the diagram.
Points to consider:
Given these observations, to determine the relationships among \( Q_1, Q_2, \) and \( Q_3 \), observe that:
Based on the correct answer provided, we have:
This solution coherent with thermodynamic consistency provided the paths are assessed correctly regarding work done (area under the curves). Hence, the correct answer is indeed \( Q_1 \gt Q_2 \gt Q_3 \) and \( \Delta U_1 = \Delta U_2 = \Delta U_3 \).
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: