Dual Nature of Radiation and Matter

JEE Physics · 163 questions · Page 2 of 17 · Click an option or "Show Solution" to reveal answer

Q11
The de Broglie wavelengths for an electron and a photon are λ\lambdae and λ\lambdap respectively. For the same kinetic energy of electron and photon, which of the following presents the correct relation between the de Broglie wavelengths of two ?
A λpλe2{\lambda _p} \propto \lambda _e^2
B λpλe{\lambda _p} \propto {\lambda _e}
C λpλe{\lambda _p} \propto \sqrt {{\lambda _e}}
D λp1λe{\lambda _p} \propto \sqrt {{1 \over {{\lambda _e}}}}
Correct Answer
Option A
Solution
λp=hp=hcE{\lambda _p} = {h \over p} = {{hc} \over E}

...... (i)

λe=h2mE{\lambda _e} = {h \over {\sqrt {2mE} }}

...... (ii) From (i) and (ii)

λpλe2{\lambda _p} \propto \lambda _e^2
Q12
A particle A of mass 'm' and charge 'q' is accelerated by a potential difference of 50 V. Another particle B of mass ' 4 m' and charge 'q' is accelerated by a potential difference of 2500 V. The ratio of de-Broglie wavelengths λAλB{{{\lambda _A}} \over {{\lambda _B}}} is close to :
A 4.47
B 10.00
C 14.14
D 0.07
Correct Answer
Option C
Solution

K.E. acquired by charge = K = qV λ\lambda =

hP{h \over P}

=

h2mK{h \over {\sqrt {2mK} }}

=

h2mqV{h \over {\sqrt {2mqV} }}

\therefore

λAλB=2mBqBVB2mAqAVA=4m.q.2500m.q.50=250{{{\lambda _A}} \over {{\lambda _B}}} = {{\sqrt {2m{}_B{q_B}{V_B}} } \over {\sqrt {2m{}_A{q_A}{V_A}} }} = \sqrt {{{4m.q.2500} \over {m.q.50}}} = 2\sqrt {50}
=2×7.07=14.14= 2 \times 7.07 = 14.14
Q13
In an electron microscope, the resolution that can be achieved is of the order of the wavelength of electrons used. To resolve a width of 7.5 × 10–12 m, the minimum electron energy required is close to -
A 25 keV
B 500 keV
C 100 keV
D 1 keV
Correct Answer
Option A
Solution

λ\lambda =

hp{h \over p}

{λ\lambda = 7.5 ×\times 10-12} P =

hλ{h \over \lambda }

KE =

P22m=(h/λ)22m{{{P^2}} \over {2m}} = {{{{\left( {h/\lambda } \right)}^2}} \over {2m}}
={6.6×10347.5×1012}2×9.1×1031= {{\left\{ {{{6.6 \times {{10}^{ - 34}}} \over {7.5 \times {{10}^{ - 12}}}}} \right\}} \over {2 \times 9.1 \times {{10}^{ - 31}}}}

J KE = 25 Kev

Q14
The ratio of wavelengths of proton and deuteron accelerated by potential Vp and Vd is 1 : 2\sqrt2. Then the ratio of Vp to Vd will be :
A 1 : 1
B 2\sqrt2 : 1
C 2 : 1
D 4 : 1
Correct Answer
Option D
Solution
λ=hmv=h2meV\lambda = {h \over {mv}} = {h \over {\sqrt {2m\,eV} }}

so

λpλd=mdVdmpVp=12{{{\lambda _p}} \over {{\lambda _d}}} = {{\sqrt {{m_d}{V_d}} } \over {\sqrt {{m_p}{V_p}} }} = {1 \over {\sqrt 2 }}
2VdVp=12{{2{V_d}} \over {{V_p}}} = {1 \over 2}
VpVd=41{{{V_p}} \over {{V_d}}} = {4 \over 1}
Q15
Proton (P)(\mathrm{P}) and electron (e) will have same de-Broglie wavelength when the ratio of their momentum is (assume, mp=1849 me\mathrm{m}_{\mathrm{p}}=1849 \mathrm{~m}_{\mathrm{e}} ):
A 1 : 1
B 1 : 43
C 1 : 1849
D 43 : 1
Correct Answer
Option A
Solution

The de Broglie wavelength of a particle is given by the formula:

λ=hp\lambda = \frac{h}{p}

where hh is Planck's constant and pp is the momentum of the particle.

If the de Broglie wavelengths of the proton and electron are the same, then:

hpp=hpe\frac{h}{p_p} = \frac{h}{p_e}

where ppp_p and pep_e are the momenta of the proton and electron, respectively.

Solving this equation for the ratio of their momenta gives:

pppe=1\frac{p_p}{p_e} = 1

So, the ratio of their momenta is 1:1

Q16
An α\alpha particle and a carbon 12 atom has same kinetic energy K. The ratio of their de-Broglie wavelengths (λα:λC12)({\lambda _\alpha }:{\lambda _{C12}}) is :
A 1:31:\sqrt 3
B 3:1\sqrt 3 :1
C 3:13:1
D 2:32:\sqrt 3
Correct Answer
Option B
Solution
Kα=KC{K_\alpha } = {K_C}
pα22mα=pC22mC{{p_\alpha ^2} \over {2{m_\alpha }}} = {{p_C^2} \over {2{m_C}}}
pαpC=mαmC{{{p_\alpha }} \over {{p_C}}} = \sqrt {{{{m_\alpha }} \over {{m_C}}}}

So

λαλC=h/pαh/pC=mCmα{{{\lambda _\alpha }} \over {{\lambda _C}}} = {{h/{p_\alpha }} \over {h/{p_C}}} = \sqrt {{{{m_C}} \over {{m_\alpha }}}}

So

λαλC=3{{{\lambda _\alpha }} \over {{\lambda _C}}} = \sqrt 3
Q17
The threshold wavelength for photoelectric emission from a material is 5500 Ao\mathop A\limits^o . Photoelectrons will be emitted, when this material is illuminated with monochromatic radiation from a A. 75 W infra-red lamp B. 10 W infra-red lamp C. 75 W ultra-violet lamp D. 10 W ultra-violet lamp Choose the correct answer from the options given below :
A C only
B A and D only
C C and D only
D B and C only
Correct Answer
Option C
Solution

Wavelength of infra-red =700 nm=700 \mathrm{~nm} (minimum) Wavelength of UV =100400 nm=100-400 \mathrm{~nm} Since we need λ<5000\lambda<5000 Å \Rightarrow Only UV would be able to emit photoelectrons.

Q18
If a source of electromagnetic radiation having power 15 kW15 \mathrm{~kW} produces 101610^{16} photons per second, the radiation belongs to a part of spectrum is. (Take Planck constant h=6×1034Jsh=6 \times 10^{-34} \mathrm{Js} )
A Gamma rays
B Radio waves
C Micro waves
D Ultraviolet rays
Correct Answer
Option A
Solution
 Energy of one photon = Power  Photon frequency E=hv=15×1031016v=15×10136×1034=2.5×1021\begin{aligned} & \text{ Energy of one photon }=\frac{\text{ Power }}{\text{ Photon frequency }} \\\\ & \mathrm{E}=\mathrm{h} v=\frac{15 \times 10^3}{10^{16}} \\\\ & \Rightarrow v=\frac{15 \times 10^{-13}}{6 \times 10^{-34}}=2.5 \times 10^{21} \end{aligned}

So gamma Rays.

Q19
Photon of frequency vv has a momentum associated with it. If cc is the velocity of light, the momentum is
A hv/chv/c
B v/cv/c
C hh vv cc
D hv/c2hv/{c^2}
Correct Answer
Option A
Solution

Energy of a photon of frequency

vv

is given by

E=hv.E = hv.

Also,

E=mc2,mc2=hvE = m{c^2},\,\,m{c^2} = hv
mc=hvCp=hvc\Rightarrow mc = {{hv} \over C} \Rightarrow p = {{hv} \over c}
Q20
A Laser light of wavelength 660 nm is used to weld Retina detachment. If a Laser pulse of width 60 ms and power 0.5 kW is used the approximate number of photons in the pulse are : [Take Planck's constant h == 6.62 × \times 10-34 Js]
A 1020
B 1018
C 1022
D 1019
Correct Answer
Option A
Solution

The power of the given laser light is expressed as

P=nhcλtP = {{nhc} \over {\lambda t}}

from which the number of photons per second is given by

n=P(λthc)=(5×102)×[(660×109)(60×103)(6.6×1034)(3×108)]n = P\left( {{{\lambda t} \over {hc}}} \right) = (5 \times {10^2}) \times \left[ {{{(660 \times {{10}^{ - 9}})(60 \times {{10}^{ - 3}})} \over {(6.6 \times {{10}^{ - 34}})(3 \times {{10}^8})}}} \right]
=100×1018=1020= 100 \times {10^{18}} = {10^{20}}
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