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Atoms Test - 10

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Atoms Test - 10
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  • Question 1
    1 / -0
    A diatomic molecule is made of two masses $$m_1$$ and $$m_2$$ which are separated by a distance $$r$$. If we calculate its rotational energy by applying Bohr's rule of angular momentum,its energy will be given by  ($$n$$ is an integer)
    Solution
    $$\displaystyle r_1= \frac{m_2}{m_1+m_2}r$$
    $$\displaystyle r_2= \frac{m_1}{m_1+m_2}r$$
    $$\displaystyle (I_1+I_2)\omega= \frac{nh}{2\pi}$$
    $$\displaystyle KE= \frac{1}{2}(I_1+I_2)\omega^2=\frac{(m_{1}+m_{2})n^{2}h^{2}}{2m_{1}m_{2}r^{2}}$$
  • Question 2
    1 / -0
    Hydrogen atom is excited from ground state to another state with principal quantum number equal to $$4$$. Then the number of spectral lines in the emission spectra will be.
    Solution
    Total number of spectral lines,
         $$N = \dfrac {n(n - 1)}{2}$$
    here, $$n$$ is principal quantum number, given $$n = 4$$
    $$\Rightarrow N = \dfrac {4(4 - 1)}{2} = 6$$

    Hence, the number of spectra lines in the emission spectrum will be $$6$$.
  • Question 3
    1 / -0
    The transition from the state $$n = 4$$ to $$n = 3$$ in a hydrogen like atom results in ultraviolet radiation. Infrared radiation will be obtained in the transition from
    Solution
    IR corresponds to least value of $$\displaystyle (\frac{1}{n_1^2}-\frac{1}{n_2^2})$$ i.e. from Paschen, Bracket and Pfund series.
    Energy of transition is less only in this case.
  • Question 4
    1 / -0
    The acceleration of an electron in the first orbit of the hydrogen atom $$(n =1)$$ is : 
    Solution
    Orbital Angular momentum 
    $$mvr=\dfrac{nh}{2\pi }$$          n=1

    $$mvr=\dfrac{h}{2\pi }$$

    $$v=\dfrac{h}{2\pi mr}$$

    $$v^{2}=\left ( \dfrac{h}{2\pi mr} \right )^{2}$$

    $$a=\dfrac{V^{2}}{r}=\dfrac{h^{2}}{4\pi ^{2}m^{2}r^{3}}$$
  • Question 5
    1 / -0
    An alpha nucleus of energy $$\overline{2}$$ mv bombards a heavy nuclear target of charge Ze. Then the distance of closest approach for the alpha nucleus will be proportional to 

    Solution
    Let  $$r$$  be the distance of closest approach.
    At the closest approach, all the kinetic energy of alpha nucleus has converted into the potential energy i.e. $$K.E = P.E$$
    $$\therefore$$    $$\dfrac{1}{2}mv^2  = \dfrac{kZe^2}{r}$$
    We get, $$r = \dfrac{2kZe^2}{mv^2}$$              
    $$\implies r\propto  \dfrac{1}{m}$$
  • Question 6
    1 / -0
    The time by a photo-electron to come out after the photon strikes is approximately 
    Solution
    From experimental aspect, the photoelectric effect is an instantaneous phenomenon. The photon strikes the metallic surface is approximately $$10^{-10}$$ s. 
  • Question 7
    1 / -0
    According to Bohr's theory, the time averaged magnetic field at the centre (i.e nucleus) of a bydrogen atom due to the motion of electrons in the $$n^{th}$$ orbit is propotional to : $$(n =$$ principal quantum number$$)$$
    Solution
    The magnetic field induced at the centre of an orbit due to an electron revolving in the nth orbit of hydrogen atom is given by
    $$B=\mu_0i_{n/(2r_n)}$$,
    Where $$i_n$$ is the current in the nth orbit $$r_n$$ the nth orbit and $$\mu_0$$ the magnetic permeablity of free space.
    $$r_n\ \alpha\ n^2$$
    $$i_n\ \alpha\ n^{-3}$$
    Therefore 
    $$\beta\ \alpha\ n^{-5}$$
    So the answer is (c) $$n^{-5}$$.
  • Question 8
    1 / -0
    If one were to apply Bohr model to a particle '$$m$$' and charge '$$q$$' moving in a plane under the influence of a magnetic field 'B', the energy of the charged particle in the $$ n^{th}$$ level will be.
    Solution
    According to Bohr model 
    $$\vec{L}=\dfrac{nh}{2\pi}$$
    $$mvr=\dfrac{nh}{2\pi}$$
    $$vr=\dfrac{nh}{2m \pi}$$...(i)
    $$\dfrac{mv^2}{r}=qvB$$
    $$\dfrac{v}{r}=\dfrac{qB}{m}$$...(ii)
    multiplying (i) and (ii)
    $$\dfrac{v}{r}=\dfrac{qB}{m}$$
    $$v^2=\dfrac{nhqB}{2  \pi m^2}$$
    K.E.=$$\dfrac{1}{2}mv^2=\dfrac{nhqB}{4 \pi m}$$
    The potential energy due to magnetic field will be zero as magnetic field is always perpendicular to velocity, hence work done by magnetic force will be zero.
  • Question 9
    1 / -0
    The time period of revolution of electron in its ground state orbit in a hydrogen atom is $$1.6\times 10^{-16}$$ s. The frequency of revolution of the electron in its first excited state (in $$s^{-1}$$) is:
    Solution
    Angular momentum of the electron is given by
    $$L_n=\dfrac{nh}{2\pi}$$, where $$n$$ is the principle quantum

    For the ground state, $$n=1$$
    $$L_1=\dfrac{h}{2\pi}=mv_1r_1$$

    For the first excited state, $$n=2$$
    $$L_2=\dfrac{2h}{2\pi}=\dfrac{h}{\pi}mv_2r_2=2\left(\dfrac{h}{2\pi}\right)$$
    $$=2L_1$$
    $$\therefore L_2=2L_1$$
    $$mv_2r_2=2mv_1r_1$$
    $$v_2r_2=2v_1r_1$$
    $$w_2r^2_2=2w_1r^2_1$$

    $$w_2=\dfrac{2w_1r^2_1}{r^2_2},$$ or $$f_2=\dfrac{2f_1r^2_1}{r^2_2}=\dfrac{2r^2_1}{r^2_2T_1}$$

    Now, the radius of orbit in a hydrogen is given by
    $$r=\dfrac{r_1n^2}{z}=r_1n^2$$
    For the first excited state, $$r_2=r_1(2)^2=4r_1$$
    $$\therefore \dfrac{r_2}{r_1}=4$$

    time period of revolution of electron in its ground state orbit in a hydrogen atom is $$1.6\times 10^{-16}$$ sec

    $$\therefore f_2=\dfrac{2r^2_1}{r^2_2 T_1}=\dfrac{2}{16}\times \dfrac{1}{1.6\times 10^{-16}}$$

    $$=\dfrac{2\times 10^{16}}{1.6\times 16}=7.812\times 10^{14}$$

    option (D) is the answer
  • Question 10
    1 / -0
    Match List - I (Experiment performed) with List - II (Phenomena discovered/ associated) and select the correct option from the options given below the lists :
    List - I
    List - II
    (a)Davisson and Germer Experiment(i)Wave nature of electrons
    (b)Millikan's oil drop experiment(ii)Charge of an electron
    (c)Rutherford experiment(iii)Quantisation of energy levels
    (d)Franck - Hertz experiment(iv)Existence of nucleus
    Solution
    Davisson and Germer Experiment$$\Rightarrow$$Wave nature of electrons
    Millikan's oil drop experiment$$\Rightarrow$$Charge of an electron
    Rutherford experiment$$\Rightarrow$$Existence of nucleus
    Franck - Hertz experiment$$\Rightarrow$$Quantisation of energy levels .
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