Chapter 13: Problem 38
In the Bohr's atomic model, the electrostatic force of attraction between nuclear charge \(\left(Z_{\mathrm{e}}\right)\) and electron of charge \(e\) is balanced by the centripetal force acting towards the centre of atom. If \(\epsilon_{0}\) be the permittivity of vacuum and \(r\) be the radius of orbit in which electron is revolving, the speed of electron is (a) \(\sqrt{\frac{Z e^{2}}{\left(4 \pi \varepsilon_{0}\right) m r}}\) (b) \(\sqrt{\frac{\left(4 \pi \varepsilon_{0}\right) m r}{Z e^{2}}}\) (c) \(\sqrt{\left(4 \pi \varepsilon_{\mathrm{o}}\right) m r Z e^{2}}\) (d) \(\frac{e}{\sqrt{\left(4 \pi \varepsilon_{\mathrm{o}}\right) m r}}\)
Short Answer
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Key Concepts
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