Step 1: Use Einstein’s photoelectric equation.
\[ K_{\max} = h\nu - \phi \] where \( K_{\max} \) = maximum kinetic energy of the emitted electrons, \( \nu \) = frequency of incident light, \( \phi \) = work function of the metal.
Step 2: For wavelength \( \lambda \):
\[ K_1 = h\nu_1 - \phi = 2\,\text{eV} \] and given \( \phi = 1\,\text{eV} \), \[ h\nu_1 = K_1 + \phi = 2 + 1 = 3\,\text{eV}. \]
Step 3: For wavelength \( \frac{\lambda}{2} \):
Frequency doubles, since \( \nu \propto \frac{1}{\lambda} \): \[ \nu_2 = 2\nu_1. \] Hence the new photon energy: \[ h\nu_2 = 2h\nu_1 = 2 \times 3 = 6\,\text{eV}. \]
Step 4: Compute new kinetic energy.
\[ K_2 = h\nu_2 - \phi = 6 - 1 = 5\,\text{eV}. \]
\[ \boxed{K_{\max} = 5\,\text{eV}} \]
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}