In the Bohr model, the radius of the \(n^{th}\) orbit is given by:
\[ r_n = n^2 r_1 \]
Given \(r_4 = 8.48\times10^{-10}\) and \(r_1 = 5.3\times10^{-11}\):
\[ \frac{r_4}{r_1} = \frac{8.48\times10^{-10}}{5.3\times10^{-11}} \approx 16 \]
Thus, \(r_4 = 16r_1 \Rightarrow n^2 = 16 \Rightarrow n = 4.\)
The de Broglie wavelength of the electron in the \(n^{th}\) orbit is related by Bohr’s quantization condition:
\[ 2\pi r_n = n\lambda_n \Rightarrow \lambda_n = \frac{2\pi r_n}{n} \]
Therefore, the ratio of wavelengths in ground and fourth states is:
\[ \frac{\lambda_1}{\lambda_4} = \frac{r_1/n_1}{r_4/n_4} = \frac{r_1}{r_4}\cdot\frac{n_4}{n_1} \] \[ \frac{\lambda_1}{\lambda_4} = \frac{1}{16}\times4 = \frac{1}{4} \]
Hence, the ratio of de Broglie wavelengths of the electron in the ground state to that in the excited state is:
\[ \boxed{\frac{\lambda_1}{\lambda_4} = \frac{1}{4}} \]
Or equivalently, \(\lambda_4 : \lambda_1 = 4 : 1\).
Option \(\lambda_4 : \lambda_1 = 4 : 1\).
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.
Considering the Bohr model of hydrogen like atoms, the ratio of the radius $5^{\text {th }}$ orbit of the electron in $\mathrm{Li}^{2+}$ and $\mathrm{He}^{+}$is
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: