In this hypothetical world, we assume that the angular momentum of electrons in a hydrogen atom is quantized to even integral multiples of \( \frac{h}{2} \), instead of integral multiples of \( \frac{h}{2\pi} \) as in Bohr's model. This affects the allowed energy levels and, consequently, the wavelengths of light emitted. Using Bohr's model, the energy levels of the hydrogen atom are given by the formula: \[ E_n = - \frac{13.6 \, \text{eV}}{n^2} \] In the hypothetical world, this quantization would result in modified energy levels. However, the largest wavelength emitted corresponds to the transition from the highest possible energy level to the second-highest level. This transition will give the longest wavelength, which lies in the visible range. Given the value \( h_e = 1224 \, \text{MeV-fm} \), and the conditions stated, the largest possible wavelength for hydrogen atoms in the visible range is: \[ \boxed{487 \, \text{nm}} \]
An electron in the hydrogen atom initially in the fourth excited state makes a transition to \( n^{th} \) energy state by emitting a photon of energy 2.86 eV. The integer value of n will be 1cm.
A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: