The root mean square velocity of gas molecules at a given temperature \( T \) is: \[ v_{\text{rms}} = \sqrt{\frac{3kT}{m}} \] where:
Alternatively, using the ideal gas law: \[ v_{\text{rms}} = \sqrt{\frac{3RT}{M}} \] where:
This shows that: \[ v_{\text{rms}} \propto \sqrt{T} \]
Let: \[ v_1 = \sqrt{T_1} = \sqrt{300}, \quad v_2 = \sqrt{T_2} = \sqrt{363} \] Ratio: \[ \frac{v_2}{v_1} = \frac{\sqrt{363}}{\sqrt{300}} = \sqrt{\frac{363}{300}} = \sqrt{1.21} \approx 1.1 \]
\[ \text{Percentage Increase} = (1.1 - 1) \times 100\% = 10\% \]
The increase in rms velocity due to heating is: \[ \boxed{10\%} \]
The motion of an airplane is represented by the velocity-time graph as shown below. The distance covered by the airplane in the first 30.5 seconds is km.
A 3 kg block is connected as shown in the figure. Spring constants of two springs \( K_1 \) and \( K_2 \) are 50 Nm\(^{-1}\) and 150 Nm\(^{-1}\) respectively. The block is released from rest with the springs unstretched. The acceleration of the block in its lowest position is ( \( g = 10 \) ms\(^{-2}\) )