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Dual Nature of Radiation and Matter Test - 59

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Dual Nature of Radiation and Matter Test - 59
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  • Question 1
    1 / -0
    The photo-electrons emitted from a surface of sodium metal are such that
    Solution
    The photo-electrons emitted from a surface of sodium metal are such that
    they have the same de-Broglie wavelength as
    $$\lambda = \dfrac h{\sqrt{2mE}}$$ where,
    $$E= h(\nu-\nu _0)$$
  • Question 2
    1 / -0
    The log-log graph between the energy $$E$$ of an electron and its de-Broglie wavelength $$\lambda$$ will be
    Solution
    As we know,
    $$\lambda =\dfrac h{\sqrt{2mE}}$$

    taking log on both sides, we get,
    $$log\lambda=logh-\dfrac 12 log 2m -\dfrac 12logE$$
    hence, graph will be a straight line with negative slope.
    option C is correct.
  • Question 3
    1 / -0
    Which one is correct
    Solution
    Momentum $$p=\dfrac {E}{c}\Rightarrow E^2=p^2c^2$$
  • Question 4
    1 / -0
    By photoelectric effect, Einstien proved
    Solution
    By photoelectric effect, Einstien proved:
    $$E=h\nu $$
  • Question 5
    1 / -0
    According to Bohr's theory, the electron in orbits have definite energy values, then according to uncertainty principle, the life time of an excited state will be
    Solution
    According to Bohr's theory $$\Delta E=0,$$ since $$\Delta E.\Delta t \ge h$$
    $$\Rightarrow \Delta t\rightarrow \infty$$
  • Question 6
    1 / -0
    The figure shows different graph between stopping potential $$(V_0)$$ and frequency $$(v)$$ for photosensitive surface of cesium, potassium, sodium and lithium. The plots are parallel. Correct ranking of the targets according to their work function greatest first will be 

    Solution
    The graph between $$v_0$$ and $$v$$ cut the $$v-axis$$ at $$v$$.
    For the given graphs $$(v_0)_{(iv)} > (v_0)_{(iii)} > (v_0)_{(ii)} > (v_0)_{(i)}$$
    $$\therefore (W_0)_(iv) > (W_0)_(iii) > (W_0)_(ii) > (W_0)_(i)$$
  • Question 7
    1 / -0
    An electron is moving through a field. It is moving (i) opposite an electric field (ii) perpendicular to a magnetic field as shown. For each situation the de-Broglie wave length of electron

    Solution
    $$\lambda=\dfrac{h}{mv}$$. Since $$v$$ increasing in case (i), but it is not changing in case (ii). Hence, in the first case de-Broglie wavelength will change, but it second case, it remain the same
  • Question 8
    1 / -0
    According to Uncertainty principle if position of a any particle is measured by cent percent value., then the uncertainty in its momentum will be :
    Solution
    From Heisenberg Uncertainty principle 
    $$ \Delta p_x \Delta x > \dfrac{h}{2 \pi} $$ 

    For accuracy in position change $$ \Delta x = 0 $$ 
    $$ \therefore \, \Delta p_x = \dfrac{h}{2 \pi \times 0} = \infty $$ 
  • Question 9
    1 / -0
    Find out the de-Broglie wavelength related to an electron of kinetic energy $$10$$ eV:
    Solution
    $$ \lambda = \dfrac{h}{\sqrt{2mE}} $$ 

    $$ \lambda = \dfrac{6.63 \times 10^{-34}}{\sqrt{2 \times 9.1 \times 10^{-31} \times 10 \times 1.6 \times 10^{-19}}} $$ 

    $$ = 3.9 \mathring A $$ 
  • Question 10
    1 / -0
    An electron and a proton are bound in a linear box of dimension $$10A $$. Then the uncertainties in their momentum is:
    Solution
    From de-Broglie wavelength.
    The uncertainty in their momentum 
    $$ \Delta x \Delta p_x = \dfrac{h}{2 \pi} $$ 

    $$ \therefore $$            $$ \Delta p_x = \dfrac{h}{2 \pi \times \Delta x} $$ 

    $$ \therefore $$            $$ \dfrac{\Delta px_e}{\Delta px_p} = \dfrac{h}{2 \pi \Delta x_e} \times \dfrac{\Delta x_p \times 2 \pi}{h} $$ 

    $$ \therefore $$             $$ \dfrac{\Delta px_e}{\Delta px_p} = \dfrac{\Delta x_p}{\Delta x_e} = \dfrac{10 \times 10^{-10}}{10 \times 10^{-10}} $$ 
               
                 $$ \dfrac{\Delta px_e}{\Delta px_p} = \dfrac{1}{1} $$
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