Dual Nature of Radiation and Matter

JEE Physics · 163 questions · Page 3 of 17 · Click an option or "Show Solution" to reveal answer

Q21
This question has Statement 1 and Statement 2. Of the four choices given after the statements, choose the one that best describes the two statements. Statement 1 : Davisson - Germer experiment established the wave nature of electrons. Statement 2 : If electrons have wave nature, they can interfere and show diffraction.
A Statement 1 is true, Statement 2 is false
B Statement 1 is true, Statement 2 is true, Statement 2 is the correct explanation for Statement 1.
C Statement 1 is true, Statement 2 is true, Statement 2 is not the correct explanation of Statement 1.
D Statement 1 is false, Statement 2 is true.
Correct Answer
Option B
Solution

Davisson-Germer experiment showed that electron beams can undergo diffraction when passed through atomic crystals.

This shows the wave nature of electrons as waves can exhibit interference and diffraction.

Q22
Radiation of wavelength λ,\lambda , is incident on a photocell. The fastest emitted electron has speed v.v. If the wavelength is changed to 3λ4,{{3\lambda } \over 4}, the speed of the fastest emitted electron will be:
A =v(43)12 = v{\left( {{4 \over 3}} \right)^{{1 \over 2}}}
B =v(34)12 = v{\left( {{3 \over 4}} \right)^{{1 \over 2}}}
C >v(43)12 > v{\left( {{4 \over 3}} \right)^{{1 \over 2}}}
D <v(43)12 < v{\left( {{4 \over 3}} \right)^{{1 \over 2}}}
Correct Answer
Option C
Solution
hv02hv0=12mv2h{v_0}^2 - h{v_0} = {1 \over 2}m{v^2}

\therefore

43hv0hv0=12mv2{4 \over 3}h{v_0} - h{v_0} = {1 \over 2}mv{'^2}

\therefore

v2v2=43vv0vv0{{v{'^2}} \over {{v^2}}} = {{{4 \over 3}v - {v_0}} \over {v - {v_0}}}

\therefore

v=v43vv0vv0v' = v\sqrt {{{{4 \over 3}v - {v_0}} \over {v - {v_0}}}}

\therefore

v>v43v' > v\sqrt {{4 \over 3}}
Q23
A particle moving with kinetic energy E has de Broglie wavelength λ\lambda . If energy Δ\Delta E is added to its energy, the wavelength become λ\lambda /2. Value of Δ\Delta E, is :
A E
B 3E
C 2E
D 4E
Correct Answer
Option B
Solution
λ=h2mE\lambda = {h \over {\sqrt {2mE} }}

Also,

h2m(E+ΔE){h \over {\sqrt {2m\left( {E + \Delta E} \right)} }}

=

λ2{\lambda \over 2}

\therefore

E+ΔEE=4{{E + \Delta E} \over E} = 4

\Rightarrow

Δ\Delta

E = 3E

Q24
When radiation of wavelength λ\lambda is incident on a metallic surface, the stopping potential of ejected photoelectrons is 4.8 V. If the same surface is illuminated by radiation of double the previous wavelength, then the stopping potential becomes 1.6 V. The threshold wavelength of the metal is :
A 2λ\lambda
B 4λ\lambda
C 8λ\lambda
D 6λ\lambda
Correct Answer
Option B
Solution
Vs=hvϕ{V_s} = hv - \phi
4.8=hcλϕ4.8 = {{hc} \over \lambda } - \phi

..... (i)

1.6=hc2λϕ1.6 = {{hc} \over {2\lambda }} - \phi

..... (ii) Using above equation (i) - (ii)

3.2=hcλhc2λ3.2 = {{hc} \over \lambda } - {{hc} \over {2\lambda }}
3.2=hc2λ3.2 = {{hc} \over {2\lambda }}

..... (iii)

[λ=hc6.4]\left[ {\lambda = {{hc} \over {6.4}}} \right]

Put in equation (ii) ϕ\phi = 1.6

hcλth=1.6{{hc} \over {{\lambda _{th}}}} = 1.6
λth=hc1.6{\lambda _{th}} = {{hc} \over {1.6}}
=(hc6.4)×4=4λ= \left( {{{hc} \over {6.4}}} \right) \times 4 = 4\lambda
Q25
A proton, a neutron, an electron and an α\alpha particle have same energy. If λ\lambdap, λ\lambdan, λ\lambdae and λ\lambdaa are the de Broglie's wavelengths of proton, neutron, electron and α\alpha particle respectively, then choose the correct relation from the following :
A λ\lambdap = λ\lambdan > λ\lambdae > λ\lambdaa
B λ\lambdaa n p e
C λ\lambdae p = λ\lambdan > λ\lambdaa
D λ\lambdae = λ\lambdap = λ\lambdan = λ\lambdaa
Correct Answer
Option B
Solution
λ=hp=h(2mKE)\lambda=\frac{h}{p}=\frac{h}{\sqrt{(2 m K E)}}

λ1m\lambda \propto \dfrac{1}{\sqrt{m}} as all the particles have same KE.

Since meλp>λn>λαm_e \lambda_p > \lambda_{\mathrm{n}} > \lambda_\alpha $

Q26
With reference to the observations in photo-electric effect, identify the correct statements from below : (A) The square of maximum velocity of photoelectrons varies linearly with frequency of incident light. (B) The value of saturation current increases on moving the source of light away from the metal surface. (C) The maximum kinetic energy of photo-electrons decreases on decreasing the power of LED (light emitting diode) source of light. (D) The immediate emission of photo-electrons out of metal surface can not be explained by particle nature of light/electromagnetic waves. (E) Existence of threshold wavelength can not be explained by wave nature of light/ electromagnetic waves. Choose the correct answer from the options given below :
A (A) and (B) only
B (A) and (E) only
C (C) and (E) only
D (D) and (E) only
Correct Answer
Option B
Solution

\because

12mvm2=hνϕ{1 \over 2}mv_m^2 = h\nu - \phi
vm2\Rightarrow v_m^2

varies linearly with frequency. And, threshold wavelength can be explained by particle nature of light.

Q27
Electron beam used in an electron microscope, when accelerated by a voltage of 20 kV, has a de-Broglie wavelength of λ0\lambda_0. IF the voltage is increased to 40 kV, then the de-Broglie wavelength associated with the electron beam would be :
A 3 λ0\lambda_0
B 9 λ0\lambda_0
C λ02\dfrac{\lambda_0}{\sqrt2}
D λ02\dfrac{\lambda_0}{2}
Correct Answer
Option C
Solution

When electron is accelerated through potential difference VV, then

 K.E. =eVλ=h2 m(KE)=h2meVλα1Vλλ0=2040λ=λ02\begin{aligned} & \text{ K.E. }=\mathrm{eV} \\\\ & \Rightarrow \lambda=\frac{\mathrm{h}}{\sqrt{2 \mathrm{~m}(\mathrm{KE})}}=\frac{\mathrm{h}}{\sqrt{2 \mathrm{meV}}} \\\\ & \therefore \lambda \alpha \frac{1}{\sqrt{\mathrm{V}}} \\\\ & \therefore \frac{\lambda}{\lambda_0}=\sqrt{\frac{20}{40}} \\\\ & \therefore \lambda=\frac{\lambda_0}{\sqrt{2}} \end{aligned}
Q28
A sub-atomic particle of mass 1030 kg10^{-30} \mathrm{~kg} is moving with a velocity 2.21×106 m/s2.21 \times 10^6 \mathrm{~m} / \mathrm{s}. Under the matter wave consideration, the particle will behave closely like \qquad (h=6.63×1034 J.s)\left(\mathrm{h}=6.63 \times 10^{-34} \mathrm{~J} . \mathrm{s}\right)
A X-rays
B Infra-red radiation
C Gamma rays
D Visible radiation
Correct Answer
Option A
Solution

To find the matter wave behavior of the particle, we use the de Broglie wavelength formula:

λ=hmv\lambda = \frac{h}{mv}

where:

h=6.63×1034Jsh = 6.63 \times 10^{-34} \, \mathrm{J \cdot s}

is Planck’s constant,

m=1030kgm = 10^{-30} \, \mathrm{kg}

is the mass of the particle, and

v=2.21×106m/sv = 2.21 \times 10^6 \, \mathrm{m/s}

is its velocity. Follow these steps: Substitute the values into the formula:

λ=6.63×1034(1030)(2.21×106)\lambda = \frac{6.63 \times 10^{-34}}{(10^{-30})(2.21 \times 10^6)}

Calculate the denominator:

1030×2.21×106=2.21×102410^{-30} \times 2.21 \times 10^6 = 2.21 \times 10^{-24}

Now compute the wavelength:

λ6.63×10342.21×10243×1010m\lambda \approx \frac{6.63 \times 10^{-34}}{2.21 \times 10^{-24}} \approx 3 \times 10^{-10} \, \mathrm{m}

This wavelength, roughly

3×1010m3 \times 10^{-10} \, \mathrm{m}

(or 0.3 nm), lies within the X-ray portion of the electromagnetic spectrum, since X-rays typically have wavelengths in the range of about 0.01 nm to 10 nm.

Therefore, under the matter wave consideration, the particle will behave closely like: Option A: X-rays.

Q29
The speed of electrons in a scanning electron microscope is 1 ×\times 107 ms-1. If the protons having the same speed are used instead of electrons, then the resolving power of scanning proton microscope will be changed by a factor of :
A 11837{1 \over {1837}}
B 1837
C 1837{\sqrt {1837} }
D 11837{1 \over {\sqrt {1837} }}
Correct Answer
Option B
Solution

Resolving power (RP) \propto

1λ{1 \over \lambda }

We know, de-Broglie wavelength

λ=hmv\lambda = {h \over {mv}}

\therefore RP \propto

mvh{mv \over {h}}

\therefore

RPeRPp=memp=1837{{R{P_e}} \over {R{P_p}}} = {{{m_e}} \over {{m_p}}} = 1837
Q30
When the wavelength of radiation falling on a metal is changed from 500 nm to 200 nm, the maximum kinetic energy of the photoelectrons becomes three times larger. The work function of the metal is close to :
A 1.02 eV
B 0.81 eV
C 0.61 eV
D 0.52 eV
Correct Answer
Option C
Solution

K1 =

hc500ϕ0{{hc} \over {500}} - {\phi _0}

K2 =

hc200ϕ0{{hc} \over {200}} - {\phi _0}

\because K2 = 3K1 \Rightarrow

3[hc500ϕ0]=[hc200ϕ0]3\left[ {{{hc} \over {500}} - {\phi _0}} \right] = \left[ {{{hc} \over {200}} - {\phi _0}} \right]

\Rightarrow ϕ\phi0 = 0.61 eV

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