Step 1: Using Einstein's photoelectric equation:
\[
K_{\max} = h\nu - \phi
\]
where \( \nu = \frac{c}{\lambda} \).
Step 2: Given \( \lambda_A = 2\lambda_B \), we get:
\[
\nu_A = \frac{c}{2\lambda_B} = \frac{\nu_B}{2}
\]
Step 3: Substituting in the equation:
\[
K_A = h\nu_A - \phi = \frac{h\nu_B}{2} - \phi
\]
Step 4: Since \( K_B = h\nu_B - \phi \), we conclude:
\[
K_A<\frac{K_B}{2}
\]