Step 1: Determine the component of magnetic field normal to the loop.
The magnetic field direction is
\[
\hat{i}+\hat{j}+\hat{k}
\]
Magnitude of this vector:
\[
\sqrt{1^2+1^2+1^2}=\sqrt{3}
\]
Therefore, the unit vector along magnetic field is
\[
\frac{\hat{i}+\hat{j}+\hat{k}}{\sqrt{3}}
\]
Since the total magnetic field magnitude is
\[
1.73\,\text{T},
\]
the component along
\[
\hat{k}
\]
is
\[
B_k=1.73\left(\frac{1}{\sqrt{3}}\right)
\]
\[
B_k\approx \frac{1.73}{1.732}
\]
\[
B_k\approx 1\,\text{T}
\]
Step 2: Convert area into SI unit.
Given,
\[
A=10\,\text{cm}^2
\]
\[
A=10\times10^{-4}\,\text{m}^2
\]
\[
A=10^{-3}\,\text{m}^2
\]
Step 3: Find the initial magnetic flux.
Magnetic flux is
\[
\Phi=BA
\]
\[
\Phi=1\times10^{-3}
\]
\[
\Phi=10^{-3}\,\text{Wb}
\]
Step 4: Use Faraday’s law.
The magnetic field becomes zero uniformly in
\[
10\,\text{s}
\]
Hence,
\[
\mathcal{E}=\frac{\Delta\Phi}{\Delta t}
\]
\[
\mathcal{E}=\frac{10^{-3}}{10}
\]
\[
\mathcal{E}=10^{-4}\,\text{V}
\]
\[
\mathcal{E}=0.10\,\text{mV}
\]
Step 5: Final conclusion.
Hence, the induced emf is
\[
\boxed{0.10\,\text{mV}}
\]