Step 1: Write the formula for fundamental frequency.
For a stretched wire fixed at both ends, the fundamental frequency is
\[
f=\frac{1}{2L}\sqrt{\frac{T}{\mu}},
\]
where \(L\) is the length of the wire, \(T\) is the tension, and \(\mu\) is the mass per unit length.
Step 2: Relate tension to Young's modulus and strain.
Young's modulus is
\[
Y=\frac{\text{stress}}{\text{strain}}.
\]
So,
\[
\text{stress}=Y\times \text{strain}.
\]
Also,
\[
\text{stress}=\frac{T}{A},
\]
where \(A\) is the area of cross-section.
Thus,
\[
\frac{T}{A}=Y\times \text{strain}.
\]
So,
\[
T=AY\times \text{strain}.
\]
Mass per unit length is
\[
\mu=\rho A.
\]
Therefore,
\[
\frac{T}{\mu}
=
\frac{AY(\text{strain})}{\rho A}.
\]
Canceling \(A\),
\[
\frac{T}{\mu}
=
\frac{Y(\text{strain})}{\rho}.
\]
Step 3: Substitute the given values.
Given,
\[
L=1.25\ \text{m},
\]
\[
Y=2.2\times10^{11}\ \text{N m}^{-2},
\]
\[
\rho=7.7\times10^3\ \text{kg m}^{-3}.
\]
Elastic strain is
\[
0.14\%=\frac{0.14}{100}=0.0014.
\]
Therefore,
\[
f=\frac{1}{2L}\sqrt{\frac{Y(\text{strain})}{\rho}}.
\]
\[
f=\frac{1}{2(1.25)}
\sqrt{\frac{(2.2\times10^{11})(0.0014)}{7.7\times10^3}}.
\]
Step 4: Simplify the expression.
First,
\[
(2.2\times10^{11})(0.0014)
=
3.08\times10^8.
\]
Now,
\[
\frac{3.08\times10^8}{7.7\times10^3}
=
4.0\times10^4.
\]
So,
\[
\sqrt{\frac{Y(\text{strain})}{\rho}}
=
\sqrt{4.0\times10^4}.
\]
\[
=200\ \text{m s}^{-1}.
\]
Thus,
\[
f=\frac{200}{2.5}.
\]
\[
f=80\ \text{Hz}.
\]
Step 5: Final conclusion.
Therefore, the fundamental frequency of the wire is
\[
\boxed{80\ \text{Hz}}
\]
Hence, the correct option is
\[
\boxed{(3)}
\]