Step 1: Recall the formula for velocity of sound in a gas.
The velocity of sound in a gas is given by:
\[
v=\sqrt{\frac{\gamma P}{\rho}}
\]
where \(\gamma\) is the ratio of specific heats, \(P\) is pressure, and \(\rho\) is density.
Step 2: Use the ideal gas equation.
From the ideal gas law:
\[
P=\rho RT
\]
Substitute this into the expression for velocity:
\[
v=\sqrt{\frac{\gamma (\rho RT)}{\rho}}
\]
Step 3: Simplify the expression.
\[
v=\sqrt{\gamma RT}
\]
Thus, density \(\rho\) cancels out.
Step 4: Identify the dependency.
From the simplified expression:
\[
v\propto \sqrt{T}
\]
Step 5: Analyze the options.
Velocity is proportional to the square root of temperature, not directly to \(T\), \(\rho\), or their powers.
Step 6: Interpret physically.
Higher temperature means molecules move faster, so sound waves travel faster.
Step 7: State the final answer.
\[
\boxed{\sqrt{T}}
\]
which matches option \((1)\).