A) zero
B) \[\frac{e}{\sqrt{{{\varepsilon }_{0}}{{a}_{0}}m}}\]
C) \[\frac{e}{\sqrt{4\pi {{\varepsilon }_{0}}{{a}_{0}}m}}\]
D) \[\frac{\sqrt{4\pi {{\varepsilon }_{0}}{{a}_{0}}m}}{e}\]
Correct Answer: C
Solution :
| Key Idea: According to the Newtons second law, a radially inward centripetal force is needed to the electron which is being provided by the Coulombs attraction between the proton and electron. |
| Coulombs attraction between the positive proton and negative electron \[=\frac{1}{4\pi {{\varepsilon }_{0}}}\frac{{{e}^{2}}}{{{r}^{2}}}\] |
| Centripetal force has magnitude |
| \[F=\frac{m{{v}^{2}}}{r}\] |
| As per key idea, |
| \[\frac{m{{v}^{2}}}{r}=\frac{1}{4\pi {{\varepsilon }_{0}}}\frac{{{e}^{2}}}{{{r}^{2}}}\] |
| \[\Rightarrow \] \[{{v}^{2}}=\frac{1}{4\pi {{\varepsilon }_{0}}}\frac{{{e}^{2}}}{mr}\] |
| \[\Rightarrow \] \[v=\frac{e}{\sqrt{4\pi {{\varepsilon }_{0}}mr}}\] |
| For ground state of H-atom, \[r={{a}_{0}}\] |
| \[\therefore \] \[v=\frac{e}{\sqrt{4\pi {{\varepsilon }_{0}}m{{a}_{0}}}}\] |
You need to login to perform this action.
You will be redirected in
3 sec