Step 1: Write the magnification expressions.
For final image at infinity,
\[
M_\infty
=
\frac{L}{f_o}\cdot\frac{D}{f_e}.
\]
For final image at the near point,
\[
M_D
=
\frac{L}{f_o}
\left(1+\frac{D}{f_e}\right).
\]
Step 2: Use the given condition.
The magnification at the near point is \(14\%\) greater than that at infinity.
\[
M_D
=
1.14\,M_\infty.
\]
Substituting,
\[
1+\frac{D}{f_e}
=
1.14\left(\frac{D}{f_e}\right).
\]
Let
\[
x=\frac{D}{f_e}.
\]
Then,
\[
1+x=1.14x,
\]
\[
1=0.14x,
\]
\[
x=\frac{50}{7}.
\]
Hence,
\[
\frac{f_e}{D}
=
\frac{7}{50}.
\]
Therefore,
\[
\boxed{f_e:D=7:50.}
\]
Thus,
\[
\boxed{(C)}
\]
is the correct answer.