A third approach checks each option by assuming it is the correct percentage increase, computing the resulting emf at \(20\) rev/s, and seeing which one actually reproduces the required \(250\) V.
Baseline relationship: for a fixed constant of proportionality, \( E = k \Phi N \), and originally \(200 = k \Phi_1 (30)\), so \(k\Phi_1 = 6.667\).
- 87.5% increase: New flux \( = 1.875\, \Phi_1 \). Resulting emf at \(20\) rev/s: \( 6.667 \times 1.875 \times 20 = 250.0 \) V, exactly matching the required generated emf.
- 85.5% increase: New flux \(= 1.855\,\Phi_1\). Resulting emf: \(6.667 \times 1.855 \times 20 \approx 247.3\) V, short of \(250\) V.
- 75.5% increase: New flux \(=1.755\,\Phi_1\). Resulting emf: \(6.667 \times 1.755 \times 20 \approx 234.0\) V, well short of \(250\) V.
- 70.5% increase: New flux \(=1.705\,\Phi_1\). Resulting emf: \(6.667\times1.705\times20\approx227.3\) V, the largest shortfall among the options.
Only the \(87.5\%\) increase reproduces the required \(250\) V exactly when run at \(20\) rev/s.
Therefore, the correct answer is 87.5%.