Step 1: Rydberg's Formula for Energy:
The energy emitted during a transition from orbit $n_2$ to $n_1$ in a hydrogen atom is given by:
\[ \Delta E = R_H \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \]
Where Rydberg constant for energy $R_H \approx 2.18 \times 10^{-18} \, J$.
Step 2: Substitute Known Values:
Given $\Delta E = 0.4578 \times 10^{-18} \, J$.
\[ 0.4578 \times 10^{-18} = 2.18 \times 10^{-18} \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \]
Canceling $10^{-18}$ from both sides:
\[ 0.4578 = 2.18 \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \]
\[ \frac{1}{n_1^2} - \frac{1}{n_2^2} = \frac{0.4578}{2.18} \approx 0.21 \]
Step 3: Analyze Options (Trial Method):
Looking at the options, $n_1$ is consistently 2 (which corresponds to the Balmer series in the visible region). Let's substitute $n_1 = 2$:
\[ \frac{1}{2^2} - \frac{1}{n_2^2} = 0.21 \]
\[ 0.25 - \frac{1}{n_2^2} = 0.21 \]
\[ \frac{1}{n_2^2} = 0.25 - 0.21 = 0.04 \]
\[ n_2^2 = \frac{1}{0.04} = \frac{100}{4} = 25 \]
\[ n_2 = \sqrt{25} = 5 \]
Step 4: Final Verification:
The transition is from $n_2 = 5$ to $n_1 = 2$.