



For an ideal gas, the mean squared velocity \( \langle v^2 \rangle \) is related to the temperature by the equation: \[ \langle v^2 \rangle = \frac{3kT}{m} \] where \( k \) is the Boltzmann constant, \( T \) is the temperature, and \( m \) is the mass of the gas molecules.
Step 1: The equation shows a linear relationship between mean squared velocity and temperature.
Step 2: Therefore, the correct graph is a straight line with a positive slope.
Final Conclusion: The graph representing a linear variation of mean squared velocity with temperature corresponds to Option (3).

Let \( \alpha = \dfrac{-1 + i\sqrt{3}}{2} \) and \( \beta = \dfrac{-1 - i\sqrt{3}}{2} \), where \( i = \sqrt{-1} \). If
\[ (7 - 7\alpha + 9\beta)^{20} + (9 + 7\alpha - 7\beta)^{20} + (-7 + 9\alpha + 7\beta)^{20} + (14 + 7\alpha + 7\beta)^{20} = m^{10}, \] then the value of \( m \) is ___________.