Dual Nature of Radiation and Matter

NEET Physics · 96 questions · Page 4 of 10 · Click an option or "Show Solution" to reveal answer

Q31
If the kinetic energy of the particle is increased to 16 times its previous value, the percentage change in the de Broglie wavelength of the particle is
A 25
B 75
C 60
D 50
Correct Answer
Option B
Solution

de-Broglie wavelength of particle, λ\lambda =

hp{h \over p}

=

h2mE{h \over {\sqrt {2mE} }}

\therefore

λλ=EE{{\lambda '} \over \lambda } = \sqrt {{E \over {E'}}}

\Rightarrow λ\lambda' =

λ4{\lambda \over 4}

So, % change in the de Broglie wavelength =

λλ4λ×100{{\lambda - {\lambda \over 4}} \over \lambda } \times 100

= 75%

Q32
When the energy of the incident radiation is increased nby 20%, the kinetic energy of the photoelectrons emitted from a metal surface increased from 0.5 eV to 0.8 eV. The work function of the metal is
A 0.65 eV
B 1.0 eV
C 1.3 eV
D 1.5 eV
Correct Answer
Option B
Solution

0.5 = E – ϕ\phi \Rightarrow 0.8 = 1.2 E – ϕ\phi From above expressions, work function ϕ\phi = 1 eV

Q33
The de-broglie wavelength of neutrons in thermal equilibrium at temperature T is
A 3.08TA{{3.08} \over {\sqrt T }}\mathop A\limits^ \circ
B 0.308TA{{0.308} \over {\sqrt T }}\mathop A\limits^ \circ
C 0.0308TA{{0.0308} \over {\sqrt T }}\mathop A\limits^ \circ
D 30.8TA{{30.8} \over {\sqrt T }}\mathop A\limits^ \circ
Correct Answer
Option D
Solution

de Broglie wavelength of neutrons in thermal equilibrium at temperature T is

λ=h2mkBT\lambda = {h \over {\sqrt {2m{k_B}T} }}

=

6.63×10342×1.67×1027×1.38×1023×T{{6.63 \times {{10}^{ - 34}}} \over {\sqrt {2 \times 1.67 \times {{10}^{ - 27}} \times 1.38 \times {{10}^{ - 23}} \times T} }}

=

30.8TA{{30.8} \over {\sqrt T }}\mathop A\limits^ \circ
Q34
A source of light is placed at a distance of 50 cm from a photo cell and the stopping potential is found to be V 0 . If the distance between the light source and photo cell is made 25 cm, the new stopping potential will be :
A V 0 /2
B V 0
C 4V 0
D 2V 0
Correct Answer
Option B
Solution

Since, stopping potential is independent of distance hence new stopping potential will remain unchanged i.e., new stopping potential = V 0 .

Q35
The wavelength λ\lambda e of an electron and λ\lambda p of a photon of same energy E are related by
A λpλe{\lambda _p} \propto \sqrt {{\lambda _e}}
B λp1λe{\lambda _p} \propto {1 \over {\sqrt {{\lambda _e}} }}
C λpλe2{\lambda _p} \propto {\lambda _e}^2
D λpλe{\lambda _p} \propto {\lambda _e}
Correct Answer
Option C
Solution

Wavelength of an electron of energy E is

λe=h2meE{\lambda _e} = {h \over {\sqrt {2{m_e}E} }}

\Rightarrow

λe2=h22meE\lambda _e^2 = {{{h^2}} \over {2{m_e}E}}

.....(1) Wavelength of a photon of same energy E is

λp=hcE{\lambda _p} = {{hc} \over E}

\Rightarrow

E=hcλpE = {{hc} \over {{\lambda _p}}}

.....(2) Equating (1) and (2), we get

hcλp=h22meλe2{{hc} \over {{\lambda _p}}} = {{{h^2}} \over {2{m_e}\lambda _e^2}}

\Rightarrow

λp=2mechλe2{\lambda _p} = {{2{m_e}c} \over h}\lambda _e^2

\Rightarrow

λpλe2{\lambda _p} \propto {\lambda _e}^2
Q36
For photoelectric emission from certain metal the cutoff frequency is υ\upsilon . If radiation of frequency 2υ\upsilon impinges on the metal plate, the maximum possible velocity of the emitted electron will be (m is the electron mass)
A 2hυm\sqrt {{{2h\upsilon } \over m}}
B 2hυm2\sqrt {{{h\upsilon } \over m}}
C hυ(2m)\sqrt {{{h\upsilon } \over {\left( {2m} \right)}}}
D hυm\sqrt {{{h\upsilon } \over m}}
Correct Answer
Option A
Solution

Work function, ϕ\phi = hν\nu According to Einstein’s photoelectric equation

12mvmax2{1 \over 2}mv_{\max }^2

= h(2ν\nu) - hν\nu \Rightarrow

12mvmax2=hν{1 \over 2}mv_{\max }^2 = h\nu

\Rightarrow

vmax2=2hνmv_{\max }^2 = {{2h\nu } \over m}

\Rightarrow v max =

2hυm\sqrt {{{2h\upsilon } \over m}}
Q37
A parallel beam of fast moving electrons is incident normally on a narrow slit. A fluorescent screen is placed at a large distance from the slit. If the speed of the electrons is increased, which of the following statements is correct ?
A The angular width of the central maximum will decrease.
B The angular wifth of the central maximum will be unaffected.
C Diffraction pattern is not observed on the screen in the case of electrons.
D The angular width of the central maximum of the diffraction pattern will increase.
Correct Answer
Option A
Solution

As speed of an electron increases. Its de-Broglie wavelength decreases

λ=hmv\lambda = {h \over {mv}}

and angular width for central maxima is ω\omega =

2λd{{2\lambda } \over d}
ωλ1v\omega \propto \lambda \propto {1 \over v}
Q38
Two radiations of photons energies 1 eV and 2.5 eV, successively illuminate a photosensitive metallic surface of work function 0.5 eV. The ratio of the maximum speeds of the emitted electrons is
A 1 : 4
B 1 : 2
C 1 : 1
D 1 : 5
Correct Answer
Option B
Solution

According to Einsten’s photoelectric effect, the K.E. of the radiated electrons K.E max = E – W

12mv12{1 \over 2}mv_1^2

= (1 - 0.5) eV = 0.5 eV

12mv22{1 \over 2}mv_2^2

= (2.5 - 0.5) eV = 2 eV

v1v2=0.52{{{v_1}} \over {{v_2}}} = \sqrt {{{0.5} \over 2}}

= 1 : 2

Q39
If the momentum of an electron is changed by P, then the de Broglie wavelength associated with changes by 0.5%. The initial momentum of electron will be
A 200 P
B 400 P
C P200{P \over {200}}
D 100 P
Correct Answer
Option A
Solution

de Broglie wavelength associated with an electron is

λ=hP\lambda = {h \over P}

\Rightarrow P =

hλ{h \over \lambda }
ΔPP=Δλλ{{\Delta P} \over P} = - {{\Delta \lambda } \over \lambda }
PPinitial=0.5100{P \over {{P_{initial}}}} = {{0.5} \over {100}}

P initial = 200P

Q40
An α\alpha -particle moves in a circular path of radius 0.83 cm in the presence of a magnetic field of 0.25 Wb/m 2 . The de Broglie wavelength associated with the particle will be
A 1 A\mathop A\limits^ \circ
B 0.1 A\mathop A\limits^ \circ
C 10 A\mathop A\limits^ \circ
D 0.01 A\mathop A\limits^ \circ
Correct Answer
Option D
Solution

Wavelength λ\lambda =

hp{h \over p}

\Rightarrow

hp{h \over p}

=

hmv{h \over {mv}}

For circular motion = F c = qvB \Rightarrow

mv2r{{m{v^2}} \over r}

= qvB \Rightarrow mv = rBq \Rightarrow mv = (0.83 × 10 –2 )(0.25)(2 × 1.6 × 10 –19 ) de Broglie wavelength, λ\lambda =

hmv{h \over {mv}}

=

6.6×10340.83×102×0.25×2×1.6×1019{{6.6 \times {{10}^{ - 34}}} \over {0.83 \times {{10}^{ - 2}} \times 0.25 \times 2 \times 1.6 \times {{10}^{ - 19}}}}

= 0.01

A\mathop A\limits^ \circ
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