To solve this problem, we need to understand the concept of spectral series in hydrogen and hydrogen-like atoms. Each series in the hydrogen spectrum corresponds to electron transitions from higher energy levels to a lower fixed energy level. Let us examine the two series mentioned: the Lyman series and the Paschen series.
We use Rydberg's formula to calculate the wavelength (\lambda) in each transition:
\frac{1}{\lambda} = R \left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right)
For the longest wavelength in the Paschen series (transition from n_2 = 4 to n_1 = 3), substitute into the Rydberg formula:
\frac{1}{\lambda} = R \left(\frac{1}{3^2} - \frac{1}{4^2}\right) = R \left(\frac{1}{9} - \frac{1}{16}\right)
\frac{1}{\lambda} = R \left(\frac{16 - 9}{144}\right) = R \left(\frac{7}{144}\right)
Substitute the value of R:
\frac{1}{\lambda} = 1.097 \times 10^7 \times \frac{7}{144}
\lambda = \frac{144}{7 \times 1.097 \times 10^7} \approx 1.87 \times 10^{-6} \text{ m}
Thus, the longest wavelength in the Paschen series is approximately 1.87 μm, which matches the given correct option.
In single slit diffraction pattern, the wavelength of light used is \(628\) nm and slit width is \(0.2\) mm. The angular width of central maximum is \(\alpha \times 10^{-2}\) degrees. The value of \(\alpha\) is ____.