To determine the atomic number Z of an H-like ion where the wavelength matches between two different transitions, we analyze the energy transitions in hydrogen-like atoms.
1. Lyman Series Transition (Hydrogen Atom):
For the Lyman series (transition to n=1):
$ \frac{hc}{\lambda} = R_h c \left(1 - \frac{1}{n_2^2}\right) $
For the first line (n=2 → n=1):
$ \frac{hc}{\lambda} = R_h c \left(1 - \frac{1}{4}\right) = \frac{3}{4} R_h c $
2. Balmer Series Transition (H-like Ion):
For the second line of Balmer series (n=4 → n=2) in an H-like ion:
$ \frac{hc}{\lambda} = Z^2 R_h c \left(\frac{1}{4} - \frac{1}{16}\right) = \frac{3}{16} Z^2 R_h c $
3. Equating the Transitions:
Since both transitions produce the same wavelength:
$ \frac{3}{4} R_h c = \frac{3}{16} Z^2 R_h c $
Canceling common terms:
$ \frac{3}{4} = \frac{3}{16} Z^2 $
4. Solving for Z:
$ Z^2 = \frac{3/4}{3/16} = 4 $
$ Z = \sqrt{4} = 2 $
Final Answer:
The atomic number of the H-like ion is $2$.
To find the atomic number \( Z \) of the H-like ion, we use the Rydberg formula for the wavelength of emitted light during electron transitions in hydrogen-like atoms:
For hydrogen, the Rydberg formula for the Lyman series transition (from \( n = 2 \) to \( n = 1 \)) is:
\[\frac{1}{\lambda_1} = R_H \left(1 - \frac{1}{4}\right) = \frac{3R_H}{4}\]
For the H-like ion, the formula for the Balmer series (from \( n = 4 \) to \( n = 2 \)) is:
\[\frac{1}{\lambda_2} = RZ^2 \left(\frac{1}{4} - \frac{1}{16}\right) = \frac{3RZ^2}{16}\]
We are given that the wavelength of the first line of the Lyman series for hydrogen is equal to the second line of the Balmer series for the ion. Thus:
\[\frac{3R_H}{4} = \frac{3RZ^2}{16}\]
Simplifying and solving for \( Z \):
\[R_H = \frac{RZ^2}{4} \Rightarrow Z^2 = 4 \Rightarrow Z = 2\]
Therefore, the atomic number \( Z \) of the H-like ion is 2.
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: