Step 1: Determine degrees of freedom.
For a non-rigid diatomic molecule with one vibrational mode active:
- Translational degrees of freedom \(=3\)
- Rotational degrees of freedom \(=2\)
- One vibrational mode contributes \(2\) degrees of freedom
Therefore, total degrees of freedom are
\[
f=3+2+2=7
\]
Step 2: Write the molar specific heat at constant volume.
For an ideal gas,
\[
C_V=\frac{f}{2}R
\]
Thus,
\[
C_V=\frac{7}{2}R
\]
Step 3: Find \(C_P\).
Using Mayer's relation,
\[
C_P=C_V+R
\]
\[
C_P=\frac{7}{2}R+R
\]
\[
C_P=\frac{9}{2}R
\]
Step 4: Find the relation between \(C_V\) and \(C_P\).
From
\[
C_V=\frac{7}{2}R
\]
and
\[
C_P=\frac{9}{2}R
\]
we get
\[
\frac{C_V}{C_P}=\frac{7}{9}
\]
Squaring both sides,
\[
\frac{C_V^2}{C_P^2}=\frac{49}{81}
\]
Cross multiplying,
\[
81C_V^2=49C_P^2
\]
Step 5: Final conclusion.
Hence, the correct relation is
\[
\boxed{81C_V^2=49C_P^2}
\]