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Atoms Test - 44

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Atoms Test - 44
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  • Question 1
    1 / -0
    Given mass number of gold = 197,
    Density of gold = 19.7 g/cm$$^3$$
    Avogadro's number = $$6  \times 10^{23} $$. The radius of the gold atom is approximately
    Solution
    Volume occupied by one gram atom of gold  $$=\dfrac{m}{\rho}= \dfrac{197 g}{19.7 g/cm^3} = 10 cm^3$$
    Volume of one atom $$=\dfrac{10}{N_A}= \dfrac{10}{6 \times 10^{-23}}$$ $$= \dfrac{5}{3} \times 10^{23} cm^3$$
    Let $$r$$ be the radius of the atom.
    $$\therefore  \ \dfrac{4}{3} \pi r^3 = \dfrac{5}{3} \times 10^{23}$$
    $$r^3 = \dfrac{50 \times 10^{-24}}{4 \times 3.14}$$
    $$r = 1.5 \times 10^{-10} m$$
  • Question 2
    1 / -0
    In an electron gun, the control grid is given negative potential, relative to cathode in order to.
    Solution
    In an electron gun, the control grid is given a negative potential relative to cathode in order to repel the electrons so that a converging beam of electrons emerges from gun.
  • Question 3
    1 / -0
    The ratio of the wavelength for $$2\rightarrow 1$$ transition in $${ Li }^{ + },{ He }^{ + }$$ and $$H$$ is :
    Solution
    Using $$\cfrac { 1 }{ \lambda  } =R{ Z }^{ 2 }\left( \cfrac { 1 }{ { n }_{ 1 }^{ 2 } } -\cfrac { 1 }{ { n }_{ 2 }^{ 2 } }  \right) \Rightarrow \lambda \propto \cfrac { 1 }{ { Z }^{ 2 } } $$
    $$\Rightarrow { \lambda  }_{ Li }:{ \lambda  }_{ He }:{ \lambda  }_{ H }=\cfrac { 1 }{ 9 } :\cfrac { 1 }{ 4 } :\cfrac { 1 }{ 1 } =4:9:36$$
  • Question 4
    1 / -0
    Which of the following is true?
    Solution
    Lyman series lies in the ultraviolet region, Balmer series lies in the visible region and Paschen series onwards lie in the infrared region.
  • Question 5
    1 / -0
    The ratio of kinetic energy and the total energy of the electron in the nth quantum state of Bohr's atomic model of hydrogen atom is 
    Solution
    The kinetic energy of the electron in the nth state
    $$K=\dfrac {mZ^2e^4}{8\varepsilon ^2_0h^2n^2}$$
    The total energy of the electron in the nth state
    $$T=\dfrac {-mZ^2e^4}{8\varepsilon ^2_0h^2n^2}$$
    $$\therefore \dfrac {K}{T}=-1$$
  • Question 6
    1 / -0
    If the atom $$^{257}_{100}{Fm}$$ follows the Bohr model and the radius of $$^{257}_{100}{Fm}$$ is n times the Bohr radius, then the value of n is :
    Solution
    According to Bohr's model
    $$r_m=\dfrac{m^2}{2}.r_0$$
    where, m is orbit number and $$r_0$$ is the Bohr's radius for $$^{257}_{100}{FM}$$,
    $$Z=100, m=5, r_m=nr_0$$
    $$nr_0=\dfrac{5^2r_0}{100}$$ or $$n=\dfrac{1}{4}$$
  • Question 7
    1 / -0
    The photoelectric effect represent that
    Solution
    According to Einstein's quantum theory, light propagates in the form of bundles (packets or quanta) of energy, each bundle is called a photon. The photoelectric effect represents that light has a particle nature.
  • Question 8
    1 / -0
    The ratio of areas of the electron orbits for the first excited state and the ground state for the hydrogen atom is 
    Solution

  • Question 9
    1 / -0
    If the series limit of Lymen series for hydrogen atom is equal to the series limit of Balmer series for a hydrogen like atom, then atomic number of this hydrogen like atom is
    Solution
    By using, $$\dfrac {1}{\lambda} = RZ^{2} \left [\dfrac {1}{n_{1}^{2}} - \dfrac {1}{n_{2}^{2}}\right ]$$
    For hydrogen atom $$\dfrac {1}{(\lambda_{min})_{H}} = R\left [\dfrac {1}{1^{2}} - \dfrac {1}{\alpha}\right ] = R$$
    $$\dfrac {1}{(\lambda_{min})_{H}} = R$$ or $$(\lambda_{min})_{H} = \dfrac {1}{R} .... (i)$$
    For another atom
    $$\dfrac {1}{(\lambda_{min})_{atom}} = RZ^{2} \left (\dfrac {1}{2^{2}} - \dfrac {1}{\alpha}\right ) = \dfrac {RZ^{2}}{4}$$
    $$\dfrac {1}{(\lambda_{min})_{atom}} = \dfrac {4}{RZ^{2}} .... (ii)$$
    From Eqs. (i) and (ii), we get
    $$\dfrac {1}{R} = \dfrac {4}{RZ^{2}} = Z = 2$$.
  • Question 10
    1 / -0
    The adjoining diagram shows the energy levels for an electron in a certain, which transition shown represents the emission of a photon with the maximum energy

    Solution
    Energy released during emission of photon is maximum for transition III.
    Energy of photon, $$E={ E }_{ 2 }-{ E }_{ 1 }=\left( -\cfrac { { E }_{ 1 } }{ { (2) }^{ 2 } }  \right) -(-{ E }_{ 1 })=\cfrac { 3{ E }_{ 1 } }{ 4 } $$
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