To solve the problem of finding the ratio of the minimum wavelength of the Balmer series to the maximum wavelength in the Brackett series in the hydrogen spectrum, we employ the Rydberg formula for hydrogen:
\( \frac{1}{\lambda} = R \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \)
where \( R \) is the Rydberg constant, \( n_1 \) and \( n_2 \) are integers representing the final and initial energy levels, respectively, with \( n_2 > n_1 \).
For the Balmer series:
The Balmer series has \( n_1 = 2 \). The minimum wavelength \((\lambda_{\text{min}})\) occurs at the transition from the \( n_2 = \infty \) to \( n_1 = 2 \):
\( \frac{1}{\lambda_{\text{min\, Balmer}}} = R \left( \frac{1}{2^2} \right) = \frac{R}{4} \)
For the Brackett series:
The Brackett series has \( n_1 = 4 \). The maximum wavelength \((\lambda_{\text{max}})\) occurs at the transition from \( n_2 = 5 \) to \( n_1 = 4 \):
\( \frac{1}{\lambda_{\text{max\, Brackett}}} = R \left( \frac{1}{4^2} - \frac{1}{5^2} \right) = R \left( \frac{1}{16} - \frac{1}{25} \right) = R \left( \frac{25-16}{400} \right) = \frac{9R}{400} \)
Ratio Calculation:
We need the ratio \( \frac{\lambda_{\text{min\, Balmer}}}{\lambda_{\text{max\, Brackett}}} \):
\[\frac{\lambda_{\text{min\, Balmer}}}{\lambda_{\text{max\, Brackett}}} = \frac{\frac{4}{R}}{\frac{400}{9R}} = \frac{4 \times 9}{400} = \frac{36}{400} = \frac{9}{100}\]
Thus, the ratio of the minimum wavelength of the Balmer series to the maximum wavelength in the Brackett series is \( 9:100 \).
In the given circuit, the electric currents through $15\, \Omega$ and $6 \, \Omega$ respectively are

Two bar magnets A and B are identical and arranged as shown. Their lengths are negligible compared to the separation between them. A magnetic needle placed between the magnets at point P gets deflected through an angle \( \theta \) under their influence. The ratio of distances \( d_1 \) and \( d_2 \) is:
