For a body dropped from height \(x\),
\[
mgh=\frac12 mv^2
\]
So,
\[
v=\sqrt{2gx}
\]
Momentum:
\[
p=mv \propto \sqrt{x}
\]
de Broglie wavelength:
\[
\lambda=\frac{h}{p}
\]
Therefore,
\[
\lambda \propto \frac{1}{\sqrt{x}}
\]
Hence,
\[
\boxed{(B)\ \frac{1}{\sqrt{x}}}
\]