The ratio of the longest wavelength to the shortest wavelength in Balmer series is $\frac{9}5$
Concept: The spectral lines of hydrogen atom arise due to electron transitions between energy levels. The wavelength of emitted radiation is given by:
\[ \frac{1}{\lambda} = R_H \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \] where \( R_H = 1.097 \times 10^7 \, \text{m}^{-1} \) is the Rydberg constant, \( n_1 \) is the lower energy level and \( n_2 \) is the higher energy level.
Lyman Series: \( n_1 = 1 \), \( n_2 = 2, 3, 4, \ldots \)
Balmer Series: \( n_1 = 2 \), \( n_2 = 3, 4, 5, \ldots \)
Conclusion:
The Lyman series lies entirely in the UV region (91–122 nm) while the Balmer series lies in the visible region (365–656 nm), so there is no overlap between the two.
Correct Answer: Option (D): The wavelength ranges of Lyman and Balmer series do not overlap
Two identical concave mirrors each of focal length $ f $ are facing each other as shown. A glass slab of thickness $ t $ and refractive index $ n_0 $ is placed equidistant from both mirrors on the principal axis. A monochromatic point source $ S $ is placed at the center of the slab. For the image to be formed on $ S $ itself, which of the following distances between the two mirrors is/are correct:
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The least energy that is needed to emit an electron from the surface of a metal can be supplied to the loose electrons.
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