Time Period and Frequency of Revolution of an Electron in the nth Bohr orbit
Although the precise equations for time period and frequency of revolution are not required but still it is a good idea to look at the variations of these with the atomic number (Z) and the orbit number (n).
We know that Time period (T) is the time required for one complete revolution and that Frequency ($\nu$) is inverse of the time period
$\therefore T=\frac{\text { distance }}{\text { time }}=\frac{2 \pi r}{v}$
$\because r \propto \frac{\mathrm{n}^2}{\mathrm{Z}}$ and $\mathrm{v} \propto \frac{\mathrm{Z}}{\mathrm{n}}$
$\therefore T \propto\left(\frac{n^2}{Z} \times \frac{n}{Z}\right) \propto\left(\frac{n^3}{Z^2}\right)$
$\therefore \nu=\left(\frac{1}{T}\right) \propto\left(\frac{Z^2}{n^3}\right)$
It is important that you remember all the above formula and relations
| Exam | Chapter |
| JEE MAIN | Atomic Structure |
The de Broglie wavelength () associated with a photoelectron varies with the frequency (
) of the incident radiation as, [
is threshold frequency] :
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Ratio of frequency of revolution of electron in the excited state of
state of hydrogen is.
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Time taken for an electron to complete one revolution in the Bohr orbit of hydrogen atom is
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Determine the frequency of revolution of the electron in 3rd Bohr's orbit in hydrogen atom:
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Ratio of orbital frequency of electron of hydrogen in 3rd and 2nd orbital is:
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The graph between $|\psi|^2$ and r ( radial distance ) is shown below.
This represents :
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The electrons are more likely to be found:

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Ratio of orbital frequency of electron of hydrogen in 3rd and 2nd orbital is:
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It is observed that characteristic X-ray spectra of elements show regularity. When frequency to the power n i.e. $v^n$ of X - rays emitted is plotted against atomic number " Z ", following graph is obtained.
The value of "n" is
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In an atom two electrons move around the nucleus in circular orbits of radii R and 4R. The ratio of the time taken by them to complete one revolution is:
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Classical mechanics, based on Newton’s laws of motion, successfully describes the motion of all macroscopic objects such as a falling stone, orbiting planets etc., which have essentially a particle-like behaviour as shown in the previous section.