To solve this problem, we will use the photoelectric equation:
E = hf - φ
Where:
E is the kinetic energy of the emitted photoelectron.
h is Planck's constant (6.626 × 10⁻³⁴ J·s).
f is the frequency of the incident light.
φ is the work function of the metal, which is related to the threshold frequency.
Step 1: Find the work function (φ) of the metal. The work function is given by:
φ = h × f₀
Where f₀ is the threshold frequency. Given that the threshold frequency (f₀) is 3.3 × 10¹⁴ Hz, we calculate:
φ = 6.626 × 10⁻³⁴ J·s × 3.3 × 10¹⁴ Hz φ = 2.187 × 10⁻² J
Step 2: Calculate the energy of the incident photons. The energy of the incident light is given by:
E = h × f
Where f is the frequency of the incident light (8.2 × 10¹⁴ Hz). So,
E = 6.626 × 10⁻³⁴ J·s × 8.2 × 10¹⁴ Hz E = 5.428 × 10⁻² J
Step 3: Calculate the kinetic energy of the emitted photoelectron. The kinetic energy is given by the difference between the energy of the incident light and the work function:
K.E. = E - φ K.E. = 5.428 × 10⁻² J - 2.187 × 10⁻² J K.E. = 3.24 × 10⁻² J
Step 4: Relate kinetic energy to the cut-off voltage (V). The kinetic energy of the emitted electron is also related to the cut-off voltage by the equation:
K.E. = eV
Where:
e is the charge of the electron (1.6 × 10⁻¹⁹ C).
V is the cut-off voltage.
Solving for V:
V = K.E. / e V = 3.24 × 10⁻² J / 1.6 × 10⁻¹⁹ C V = 2.025 × 10³ V
Converting to volts:
V ≈ 2V
Thus, the cut-off voltage for the photoelectric emission is nearly 2V.
The correct answer is (A) 2V.