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13 Questions around this concept.
Two identical non-relativistic particles have more right angles to each other, possessing De-Broglie wavelengths and The De-Broglie wavelength of each particle in the frame of their centre of mass.
An electron of mass' m ' and charge ' e ' initially at rest gets accelerated by a constant electric field E. The rate of change of the de-Broglie wavelength of this electron at time t, ignoring relativistic effects, is-
The de-Broglie wavelengths of a proton and -particle are equal. The ratio of their velocities is-
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The potential energy of a particle of mass m is given by are de-Broglie wavelength of the particle, when and x>1 respectively. If the total energy of the particle is then the ratio will be -
A proton and an alpha are accelerated in a field of same potential energy. Then, the ratio of the Broglie wavelengths associated with the moving particles are -
Radiation from the hydrogen gas excited to the first excited state is used for illuminating certain photoelectric plates. When the radiation from some unknown hydrogen-like gas excited to the same level is used to expose the same plate, it is found that the de–-Broglie wavelength of the fastest photoelectron has decreased 2.3 times. It is given that the energy corresponding to the longest wavelength of the Lyman series of the unknown gas is 3 times the ionization energy of hydrogen gas (13.6 eV). Find the work function of the photoelectric plate in eV. (Take
An electron and a photon have the same energy 4 E. The ratio of de -Broglie wavelength of an electron to the wavelength of a photon (Mass of electron is m and speed of light is c)
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De-broglie's explanation of Bohr's second postulate-
Since the Bohr gave many postulates in his theory, but the second postulate is not very clear and little puzzling. The Scientist De Broglie explained this puzzle very clearly that why the angular momentum of the revolving electron is the integral multiple of the . De broglie in his experiment proved that the electron revolving the circular orbit has wave nature also in the last chapter we have seen the experiment performed by the Davison and Germer which proved that the electron shows the wave nature. In analogy to waves travelling on a string, particle waves too can lead to standing waves under resonant conditions. During the chapter Waves and Oscillation, we know that when a string is plucked, a vast number of wavelengths are excited. However only those wavelengths survive which have nodes at the ends and form the standing wave in the string. It means that in a string, standing waves are formed when the total distance travelled by a wave down the string and back is any integral number of wavelengths. Waves with other wavelengths interfere with themselves upon reflection and their amplitudes quickly drop to zero.
For an electron moving in circular orbit of radius , the total distance is the circumference of the orbit, .
Figure given above illustrates a standing particle wave on a circular orbit for n = 4, i.e., 2πrn = 4λ, where λ is the de Broglie wavelength of the electron moving in nth orbit. From the last chapter we have studied that λ = h/p, where p is the magnitude of the electron’s momentum. If the speed of the electron is much less than the speed of light, the momentum is mvn.
Thus,
.
From the above equation, we have,
This is the quantum condition proposed by Bohr for the angular momentum of the electron. Thus de Broglie hypothesis provided an explanation for Bohr’s second postulate for the quantisation of angular momentum of the orbiting electron.
The quantised electron orbits and energy states are due to the wave nature of the electron and only resonant standing waves can persist. Bohr’s model, involving classical trajectory picture (planet-like electron orbiting the nucleus), correctly predicts the gross features of the hydrogenic atoms(Hydrogenic atoms are the atoms consisting of a nucleus with positive charge +Ze and a single electron, where Z is the proton number. Examples are hydrogen atom, singly ionised helium, doubly ionised lithium, and so forth.), in particular, the frequencies of the radiation emitted or selectively absorbed.
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