The transition from the state n=3 to n=1
a hydrogen like atom results in ultraviolet
radiation. Infrared radiation will be obtained
in the transition from
(a)
(b)
(c)
(d)
The wavelength of the first line of Lyman series for hydrogen atom is equal to that of the second line of Balmer series for a hydrogen-like ion. The atomic number Z of hydrogen-like ion is:
(1) 4
(2) 1
(3) 2
(4) 3
An electron in the hydrogen atom jumps from nth excited state to the ground state. The wavelength so emitted illuminates a photosensitive material having work function 2.75 eV. If the stopping potential of the photo-electron is 10V, the value of n is
(1) 3
(2) 4
(3) 5
(4) 2
An alpha nucleus of energy bombards a heavy nuclear target of charge Ze. Then the distance of closest approach for the alpha nucleus will be proportional to
(a) (b)
(c) (d)
The electron in the hydrogen atom jumps from excited state to its ground state and the photons thus emitted irradiate a photosensitive material. If the work function of the material is the stopping potential is estimated to be (the energy of the electron in the nth state )
1.
2.
3.
4.
In a Rutherford scattering experiment when a projectile of charge and mass approaches a target nucleus of charge and mass the distance of closest approach is . What is the energy of the projectile?
1. | Directly proportional to \(M_1 \times M_2\) |
2. | Directly proportional to \(Z_1Z_2\) |
3. | Inversely proportional to \(Z_1\) |
4. | Directly proportional to mass \(M_1\) |
The ionization energy of the electron in the hydrogen atom in its ground state is 13.6 eV. The atoms are excited to higher energy levels to emit radiations of 6 wavelengths. Maximum wavelength of emitted radiation corresponds to the transition between
(a) n=3 to n=2 states
(b) n=3 to n=1 states
(c) n=2 to n=1 states
(d) n=4 to n=3 states
The ground state energy of hydrogen atom is -13.6 eV. When its electron is in the first excited state, its excitation energy is:
(1) 3.4 eV
(2) 6.8 eV
(3) 10.2 eV
(4) zero
In the phenomenon of electric discharge through gases at low pressure, the coloured glow in the tube appears as a result of:
(1) excitation of electrons in the atoms
(2) the collision between the atoms of the gas
(3) the collisions between the charged particles emitted from the cathode and the atoms of the gas
(4) the collision between different electrons of the atoms of the gas