Concept:
For an ideal gas,
\[
v_{\text{rms}}
=
\sqrt{\frac{3RT}{M}}
\]
and the speed of sound is
\[
v_s
=
\sqrt{\frac{\gamma RT}{M}}.
\]
Hence,
\[
\frac{v_{\text{rms}}}{v_s}
=
\sqrt{\frac{3}{\gamma}}.
\]
Step 1: Use the given condition.
Given,
\[
v_{\text{rms}}
=
\sqrt{2}\,v_s.
\]
Therefore,
\[
\sqrt{\frac{3}{\gamma}}
=
\sqrt{2}.
\]
Squaring both sides,
\[
\frac{3}{\gamma}=2.
\]
\[
\gamma=\frac{3}{2}.
\]
Step 2: Find the effective \(\gamma\) of the mixture.
For Helium (monoatomic),
\[
C_{V,\text{He}}=\frac{3}{2}R,
\qquad
C_{P,\text{He}}=\frac{5}{2}R.
\]
For Hydrogen (diatomic),
\[
C_{V,\text{H}_2}=\frac{5}{2}R,
\qquad
C_{P,\text{H}_2}=\frac{7}{2}R.
\]
For the mixture,
\[
C_P
=
2\left(\frac{5}{2}R\right)
+
n\left(\frac{7}{2}R\right)
=
\frac{10+7n}{2}R.
\]
\[
C_V
=
2\left(\frac{3}{2}R\right)
+
n\left(\frac{5}{2}R\right)
=
\frac{6+5n}{2}R.
\]
Thus,
\[
\gamma
=
\frac{C_P}{C_V}
=
\frac{10+7n}{6+5n}.
\]
Step 3: Equate \(\gamma\) to \(\dfrac{3}{2}\).
\[
\frac{10+7n}{6+5n}
=
\frac{3}{2}.
\]
\[
2(10+7n)
=
3(6+5n).
\]
\[
20+14n
=
18+15n.
\]
\[
n=2.
\]
Step 4: Write the final answer.
\[
\boxed{n=2}
\]
\[
\boxed{\text{Answer = (C)}}
\]