Step 1: {Formulas for RMS speed and speed of sound}
The root mean square (RMS) speed of gas molecules is \( v_{{rms}} = \sqrt{\frac{3RT}{M}} \). The velocity of sound in a gas is \( v_{{sound}} = \sqrt{\frac{\gamma RT}{M}} \), where \( \gamma \) is the adiabatic index.
Step 2: {Ratio of \( v_{{sound}} \) to \( v_{{rms}} \)}
Dividing the two equations yields: \[ \frac{v_{{sound}}}{v_{{rms}}} = \sqrt{\frac{\gamma}{3}} \]
Step 3: {Calculating \( \gamma \) from degrees of freedom}
For a gas mixture with an average degree of freedom \( f = 6 \), the adiabatic index is: \[ \gamma = 1 + \frac{2}{f} = 1 + \frac{2}{6} = \frac{4}{3} \]
Step 4: {Determining the velocity of sound}
Substituting \( \gamma \) into the ratio: \[ v_{{sound}} = \sqrt{\frac{4/3}{3}} v_{{rms}} = \frac{2}{3} v_{{rms}} \] Given that \( v_{{rms}} = c \), the velocity of sound is: \[ v_{{sound}} = \frac{2c}{3} \] The final answer is \( \frac{2c}{3} \).
A particle is moving in a straight line. The variation of position $ x $ as a function of time $ t $ is given as:
$ x = t^3 - 6t^2 + 20t + 15 $.
The velocity of the body when its acceleration becomes zero is: