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Atoms Test - 41

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Atoms Test - 41
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  • Question 1
    1 / -0
    White light is passed through sodium vapours contained in a thin walled glass flask and the transmitted light is examined with the help of a spectrometer. The spectrum so obtained is.
    Solution
    By definition, absorption spectra is the spectra of the light transmitted through a material. 
  • Question 2
    1 / -0
    If $$E_P$$ and $$E_k$$ represent potential energy and kinetic energy respectively, of an orbital electron, then according to Bohr's theory:
    Solution
    Potential energy of an orbital electron $$E_p=-\dfrac{Ze^2}{r}$$
    Kinetic energy of an electron$$E_k=\dfrac{Ze^2}{2r}$$, where Z=atomic number
    So, $$E_k=-\dfrac{E_p}{2}$$
  • Question 3
    1 / -0
    If the minimum energy of photons needed to produce photoelectric effect is 3eV, bombarding the photoelectric material by a number of photons of 2.5eV also one can get
    Solution
    Work function of metal is given as  $$\phi = 3 \ eV$$
    Energy of incident photon  $$E_{incident} = 2.5 \ eV$$
    Emission of photo electrons from the metal surface takes place only when the energy of the incident photon is greater than the work function of the metal surface.
    Since here, energy of incident photon is less than work function of metal surface. So emission of electron is not possible.
  • Question 4
    1 / -0
    When a beam of white light is passed through sodium vapours and then through a spectrometer, spectrum so obtained has two dark lines present in the yellow region. This spectrum is called
    Solution
    By definition, absorption spectrum is the spectrum of the light transmitted through a material. 
  • Question 5
    1 / -0
     In the hydrogen atom an electron is moving in nth orbit. The circumference s of the orbit and the de Broglie wavelength, of the moving electron are related by the equation
    Solution
    It is a postulate by Bohr , written as $$2 \pi r =n \lambda$$ 
    circumference $$S=n\times wavelength$$
  • Question 6
    1 / -0
    If the electron in the hydrogen atoms is excited to n = 5 state, the number of frequencies present in the radiation emitted is :
    Solution
    The given excited state  $$n = 5$$
    Thus number of frequencies (or spectral lines)  $$N = \dfrac{n(n-1)}{2}$$
    $$\implies \ N = \dfrac{5\times (5-1)}{2} =10$$
  • Question 7
    1 / -0
    Radius of the second Bohr orbit of a singly ionised helium atom is
    Solution
    Radius of nth Bohr orbit   $$r_n = \dfrac{0.529 n^2}{Z} \ A^o$$
    For ionised Helium atom  $$Z = 2$$
    Second Bohr orbit  $$n=2$$
    $$\implies \ r_2 = \dfrac{0.529\times 2^2}{2} = 1.06 \ A^o$$
  • Question 8
    1 / -0
    The wave length of K-ray line of an anti cathode element of atomic number Z is nearly proportional to:
    Solution
    Frequency of K-ray   $$\nu\propto (Z-1)^2$$
    We know that  $$\lambda = \dfrac{v}{\nu}$$
    Thus   $$\lambda \propto \dfrac{1}{(Z-1)^2}$$
  • Question 9
    1 / -0
    Linear momentum of an electron in Bohr orbit of H-atom (principal quantum number $$n$$) is proportional to :
    Solution
    The angular momentum in a Bohr orbit is given as 
    $$L=mvr=\dfrac{nh}{2\pi}$$
    $$\implies mv=\dfrac{nh}{2\pi r}$$
    $$\implies p=mv\propto n$$
  • Question 10
    1 / -0
    When electron in hydrogen atom jumps from second orbit to first orbit, the wavelength of radiation emitted is $$\lambda$$. When electron jumps from third orbit to first orbit, the wavelength of emitted radiation would be 
    Solution
    Wavelength of photon emitted   $$\dfrac{1}{\lambda} = R \bigg(\dfrac{1}{n_2^2} - \dfrac{1}{n_1^2}\bigg)$$              $$(\because Z = 1)$$
    Transaction from second orbit to first orbit :  
    We have,  $$n_1 = 2$$           $$n_2 = 1$$
    $$\therefore$$  $$\dfrac{1}{\lambda} = R \bigg(\dfrac{1}{1^2} - \dfrac{1}{2^2}\bigg)$$         $$\implies R = \dfrac{4}{3\lambda}$$
    Transaction from third orbit to first orbit :  
    We have,  $$n_1 = 3$$           $$n_2 = 1$$
    $$\therefore$$  $$\dfrac{1}{\lambda'} = R \bigg(\dfrac{1}{1^2} - \dfrac{1}{3^2}\bigg)$$         
    $$\implies \lambda' =\dfrac{9}{8R}= \dfrac{9}{8}\times \dfrac{3\lambda}{4} = \dfrac{27}{32}\lambda$$
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