The wavelength of a spectral line in the hydrogen spectrum is given by:
\[ \frac{1}{\lambda} = RZ^2 \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right), \]
where \( R \) is the Rydberg constant, \( Z \) is the atomic number, \( n_1 \) is the lower energy level, and \( n_2 \) is the higher energy level.
For the shortest wavelength in the Balmer series:
\[ n_1 = 2, \quad n_2 = \infty \]
\[ \frac{1}{\lambda_B} = RZ^2 \left( \frac{1}{2^2} - \frac{1}{\infty^2} \right) = RZ^2 \left( \frac{1}{4} \right). \]
For the shortest wavelength in the Lyman series:
\[ n_1 = 1, \quad n_2 = \infty \]
\[ \frac{1}{\lambda_L} = RZ^2 \left( \frac{1}{1^2} - \frac{1}{\infty^2} \right) = RZ^2 (1). \]
Taking the ratio of wavelengths:
\[ \frac{\lambda_B}{\lambda_L} = \frac{\frac{1}{RZ^2 \frac{1}{4}}}{\frac{1}{RZ^2 (1)}} = 4 : 1. \]
Thus, the ratio is:
\[ \lambda_B : \lambda_L = 4 : 1. \]
Final Answer: 4:1 (Option 1)
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is: