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 \(\lambda_4 : \lambda_1 = 4 : 1\).
For a given reaction \( R \rightarrow P \), \( t_{1/2} \) is related to \([A_0]\) as given in the table. Given: \( \log 2 = 0.30 \). Which of the following is true?
| \([A]\) (mol/L) | \(t_{1/2}\) (min) |
|---|---|
| 0.100 | 200 |
| 0.025 | 100 |
A. The order of the reaction is \( \frac{1}{2} \).
B. If \( [A_0] \) is 1 M, then \( t_{1/2} \) is \( 200/\sqrt{10} \) min.
C. The order of the reaction changes to 1 if the concentration of reactant changes from 0.100 M to 0.500 M.
D. \( t_{1/2} \) is 800 min for \( [A_0] = 1.6 \) M.