In the hydrogen atom, the energy of the electron in the \( n^{th} \) orbit is given by: \[ E_n = - \frac{13.6}{n^2} \text{ eV} \] The wavelength of the emitted photon when the electron transitions from an upper orbit \( n_2 \) to a lower orbit \( n_1 \) can be found using the relation: \[ E_{\text{photon}} = E_{n_2} - E_{n_1} \] The energy of the photon is related to the wavelength \( \lambda \) by the equation: \[ E_{\text{photon}} = \frac{hc}{\lambda} \] where \( h \) is Planck's constant and \( c \) is the speed of light. For the transition from the 3rd orbit to the 2nd orbit, the energy difference is: \[ \Delta E_{3 \rightarrow 2} = E_3 - E_2 = - \frac{13.6}{9} - \left( - \frac{13.6}{4} \right) = \frac{13.6}{4} - \frac{13.6}{9} \] The wavelength of the emitted photon for this transition is: \[ \lambda = \frac{hc}{\Delta E_{3 \rightarrow 2}} = \frac{5}{27} \cdot \lambda \] For the transition from the 2nd orbit to the 1st orbit, the energy difference is: \[ \Delta E_{2 \rightarrow 1} = E_2 - E_1 = - \frac{13.6}{4} - \left( - \frac{13.6}{1} \right) = \frac{13.6}{1} - \frac{13.6}{4} \] The wavelength of the emitted photon for this transition is: \[ \lambda_{\text{new}} = \frac{hc}{\Delta E_{2 \rightarrow 1}} = \frac{5}{27} \cdot \lambda \]
Thus, the wavelength of the photon emitted when the electron jumps from the second to the first orbit is \( \frac{5\lambda}{27} \).
A hydrogen atom consists of an electron revolving in a circular orbit of radius r with certain velocity v around a proton located at the nucleus of the atom. The electrostatic force of attraction between the revolving electron and the proton provides the requisite centripetal force to keep it in the orbit. According to Bohr’s model, an electron can revolve only in certain stable orbits. The angular momentum of the electron in these orbits is some integral multiple of \(\frac{h}{2π}\), where h is the Planck’s constant.
Ion | Q4+ | Xb+ | Yc+ | Zd+ |
---|---|---|---|---|
Radius (pm) | 53 | 66 | 40 | 100 |
Q4+, Xb+, Yc+, Zd+ are respectively
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: