Embibe Experts Solutions for Chapter: Atomic Physics, Exercise 3: Exercise-3

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Embibe Experts Physics Solutions for Exercise - Embibe Experts Solutions for Chapter: Atomic Physics, Exercise 3: Exercise-3

Attempt the practice questions on Chapter 33: Atomic Physics, Exercise 3: Exercise-3 with hints and solutions to strengthen your understanding. Alpha Question Bank for Medical: Physics solutions are prepared by Experienced Embibe Experts.

Questions from Embibe Experts Solutions for Chapter: Atomic Physics, Exercise 3: Exercise-3 with Hints & Solutions

MEDIUM
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An electron of a stationary hydrogen atom passes from the fifth energy level to the ground level. The velocity that the atom acquired as a result of photon emissiór will be

MEDIUM
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The ratio of kinetic enerav to the total energy of an electron in a Bohr orbit of the hydrogen atom, is

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Find the energy required for the electron excitation in Li2+from the first to the third Bohr orbit .

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An electron bean is acceleration by a potential difference V to hit a metallic target to produce X-rays. It produces continuous as well as characteristic X-rays. If λmin is the smallest possible wavelength of λmin ray in the spectrum, the variation of log λmin with logVis correctly represented in

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If the series limit frequency of the Lyman series is νL, then the series limit frequency of the Pfund series is,

HARD
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An electron from various excited states of hydrogen atom emit radiation to come to the ground state. Let λn,λg  be the de Broglie wavelength of the electron in the nth state and the ground state respectively. Let  n be the wavelength of the emitted photon in the transition from the nthstate to the ground state. For large n, (A,Bare constants).

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A hydrogen atom, initially in the ground state is excited by absorbing a photon of wavelength 980 A. The radius of the atom in the excited state, in terms of Bohr radius ao, will be: hc=12500 eV A

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A particle of mass m moves in a circular orbit in a central potential field Ur=12kr2. If Bohr's quantization conditions are applied, radii of possible orbitals and energy levels vary with quantum number n as