Q 1 :

A metal target with atomic number Z = 46 is bombarded with a high energy electron beam. The emission of X-rays from the target is analyzed. The ratio r of the wavelengths of the Kα-line and the cut-off is found to be r=2. If the same electron beam bombards another metal target with Z = 41, the value of r will be               [2024]

  • 2.53

     

  • 1.27

     

  • 2.24

     

  • 1.58

     

(1)

The ratio of the wavelengths of the Kα-line and the cut-off i.e.

λKαλ0(=r)1(Z-1)2

  r2r1=(Z1-1)2(Z2-1)2=(46-1)2(41-1)2=452402

or,  r2=1.265×r1=1.265×2=2.53



Q 2 :

In a hydrogen-like atom electron make transition from an energy level with quantum number n to another with quantum number (n-1). If n1, the frequency of radiation emitted is proportional to:                          [2012]

  • 1n

     

  • 1n2

     

  • 1n3/2

     

  • 1n3

     

(4)

ΔE=hν

ν=ΔEh=k[1(n-1)2-1n2]=k(2n-1)n2(n-1)22kn3  or,  ν1n3



Q 3 :

The wavelength of the first spectral line in the Balmer series of hydrogen atom is 6561 Å. The wavelength of the second spectral line in the Balmer series of singly-ionized helium atom is                    [2011]

  • 1215 Å

     

  • 1640 Å

     

  • 2430 Å

     

  • 4687 Å

     

(1)

We know for hydrogen or hydrogen-like atom,

1λ=RZ2[1n12-1n22]

For the first spectral line in the Balmer series of hydrogen atom, n1=2 and n2=3. Here Z=1

  16561=R(1)2(14-19)=5R36       (i)

For the second spectral line in the Balmer series of singly ionised helium ion, n2=4 and n1=2 ; Z=2

  1λ=R(2)2[14-116]=3R4        (ii)

Dividing Eq. (i) by Eq. (ii),

λ6561=5R36×43R=527

   λ=1215 Å



Q 4 :

The largest wavelength in the ultraviolet region of the hydrogen spectrum is 122 nm. The smallest wavelength in the infrared region of the hydrogen spectrum (to the nearest integer) is                          [2007]

  • 802 nm

     

  • 823 nm

     

  • 1882 nm

     

  • 1648 nm

     

(2)

The smallest frequency and longest wavelength in the ultraviolet region will be for transition of electron from n=2 to n=1, i.e., Lyman series.

  1λ=R(1n12-1n22)

  1122×10-9m=R(112-122)=R(1-14)=3R4

  R=43×122×10-9 m-1

The highest frequency and smallest wavelength for the infrared region will be for transition of electron n=, n=3 corresponding to Paschen series.

  1λ=R(1n12-1n22)1λ=43×122×10-9(132-1)

  λ=3×122×9×10-94=823.5 nm



Q 5 :

A photon collides with a stationary hydrogen atom in the ground state inelastically. Energy of the colliding photon is 10.2 eV. After a time interval of the order of microsecond another photon collides with same hydrogen atom inelastically with an energy of 15 eV. What will be observed by the detector?                     [2005]

  • One photon of energy 10.2 eV and an electron of energy 1.4 eV

     

  • 2 photon of energy of 1.4 eV

     

  • 2 photon of energy 10.2 eV

     

  • One photon of energy 10.2 eV and another photon of energy 1.4 eV

     

(1)

Initially, a photon of energy 10.2 eV collides inelastically with a hydrogen atom in the ground state. For hydrogen atom,

E1=-13.6 eV,  E2=-13.64eV=-3.4 eV

  E2-E1=10.2 eV

The electron of the hydrogen atom will jump to the second orbit after absorbing the photon of energy 10.2 eV. Another photon of energy 15 eV strikes the hydrogen atom inelastically. This energy is sufficient to knock out the electron from the atom as the ionisation energy is 13.6 eV. The remaining energy, 15-13.6=1.4 eV is left, which is released by the second photon.



Q 6 :

If the atom Fm100257 follows the Bohr model and the radius of Fm100257 is n times the Bohr radius, then find n.                  [2003]

  • 100

     

  • 200

     

  • 4

     

  • 14

     

(4)

For an atom following Bohr's model, the radius of the fifth orbit.

rm=r0m2Z, where r0 = Bohr's radius.

For Fm100257,  m=5  (Fifth orbit in which the outermost electron is present) and Z=100

  rm=r0×52100=nr0  (given)

  n=14