Step 1: Motor emf equation.
\[
E_{a} = V - I_{a}R_{a}
\]
and
\[
E_{a} \propto N \Phi
\]
For constant field ($\Phi$ constant), $E_{a} \propto N$.
Step 2: At rated conditions.
Given: $V=400 \,\text{V}, I_{a}=15 \,\text{A}, R_{a}=1.2 \,\Omega, N=1500 \,\text{RPM}$.
\[
E_{a1} = 400 - (15)(1.2) = 400 - 18 = 382 \,\text{V}.
\]
Step 3: New conditions (10% drop in voltage).
New supply: $V' = 0.9 \times 400 = 360 \,\text{V}$.
Armature current remains same ($I_{a}=15$ A) because load torque is constant.
\[
E_{a2} = V' - I_{a}R_{a} = 360 - 18 = 342 \,\text{V}.
\]
Step 4: Relating emf and speed.
\[
\frac{E_{a1}}{E_{a2}} = \frac{N_{1}}{N_{2}}
\]
\[
N_{2} = N_{1} \cdot \frac{E_{a2}}{E_{a1}} = 1500 \cdot \frac{342}{382}.
\]
\[
N_{2} \approx 1343.5 \,\text{RPM}.
\]
Step 5: Rounding off.
\[
N_{2} \approx 1344 \,\text{RPM} \;\; \approx 1340 \,\text{to nearest 10}.
\]
% Final Answer
\[
\boxed{1344 \,\text{RPM (rounded to 1340 or 1344 depending on rounding rule)}}
\]
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