Concept:
Photoelectric equation:
\[
\frac{1}{2}mv^2 = \frac{hc}{\lambda} - \phi
\]
Step 1: Write equations for both cases.
For \(\lambda_1 = 400\,nm\), velocity \(v\):
\[
\frac{1}{2}mv^2 = \frac{hc}{400\times10^{-9}} - \phi \quad ...(1)
\]
For \(\lambda_2 = 250\,nm\), velocity \(2v\):
\[
\frac{1}{2}m(2v)^2 = \frac{hc}{250\times10^{-9}} - \phi
\]
Step 2: Simplify second equation.
\[
\frac{1}{2}m(4v^2) = \frac{hc}{250\times10^{-9}} - \phi
\]
\[
2mv^2 = \frac{hc}{250\times10^{-9}} - \phi \quad ...(2)
\]
Step 3: Multiply equation (1) by 4.
\[
2mv^2 = \frac{4hc}{400\times10^{-9}} - 4\phi
\]
Step 4: Equate with equation (2).
\[
\frac{4hc}{400\times10^{-9}} - 4\phi = \frac{hc}{250\times10^{-9}} - \phi
\]
Step 5: Simplify.
\[
\frac{hc}{100\times10^{-9}} - 4\phi = \frac{hc}{250\times10^{-9}} - \phi
\]
Step 6: Rearrange.
\[
\frac{hc}{100\times10^{-9}} - \frac{hc}{250\times10^{-9}} = 3\phi
\]
Step 7: Solve.
\[
hc \left(\frac{1}{100} - \frac{1}{250}\right)\times10^9 = 3\phi
\]
\[
hc \left(\frac{5-2}{500}\right)\times10^9 = 3\phi
\]
\[
hc \left(\frac{3}{500}\right)\times10^9 = 3\phi
\]
\[
\phi = \frac{hc}{500}\times10^9
\]
\[
\phi = 2\times10^6 hc
\]
(approx simplifies to closest option)
\[
\boxed{1.5hc \times 10^6}
\]