Atoms and Nuclei

JEE Physics · 201 questions · Page 3 of 21 · Click an option or "Show Solution" to reveal answer

Q21
A nucleus of mass M+M+Δm\Delta m is at rest and decays into two daughter nuclei of equal mass M2{M \over 2} each. Speed of light is c.c. The binding energy per nucleon for the parent nucleus is E1{E_1} and that for the daughter nuclei is E2.{E_2}. Then
A E2=2E1{E_2} = 2{E_1}
B E1>E2{E_1} > {E_2}
C E2>E1{E_2} > {E_1}
D E1=2E2{E_1} = 2{E_2}
Correct Answer
Option C
Solution

In nuclear fission, the binding energy per nucleon of daughter nuclei is greater than the parent nucleon of daughter nuclei is greater than the parent nucleus.

Q22
A radioactive nucleus (initial mass number AA and atomic number ZZ emits 3α3\,\alpha - particles and 22 positrons. The ratio of number of neutrons to that of protons in the final nucleus will be
A AZ8Z4{{A - Z - 8} \over {Z - 4}}
B AZ4Z8{{A - Z - 4} \over {Z - 8}}
C AZ12Z4{{A - Z - 12} \over {Z - 4}}
D AZ4Z2{{A - Z - 4} \over {Z - 2}}
Correct Answer
Option B
Solution
ZAXA12Z8Y+324Xe+t0e{}_Z^AX\mathop \to \limits^{A - 12} {}_{Z - 8}Y + 3{}_2^4{X_e} + {}_t^0e

Number of protons, Np = Z - 8 Number of neutrons, Nn =

A12(Z8)A - 12 - \left( {Z - 8} \right)

\therefore Required ratio

=AZ4Z8= {{A - Z - 4} \over {Z - 8}}
Q23
In the nuclear fusion reaction 12H+13H24He+n{}_1^2H + {}_1^3H \to {}_2^4He + ngiventhattherepulsivepotentialenergybetweenthetwonucleiis given that the repulsive potential energy between the two nuclei is 7.7×1014J \sim 7.7 \times {10^{ - 14}}J,thetemperatureatwhichthegasesmustbeheatedtoinitiatethereactionisnearly[BoltzmannsConstant, the temperature at which the gases must be heated to initiate the reaction is nearly [ Boltzmann's Constant k=1.38×1023J/Kk = 1.38 \times {10^{ - 23}}\,J/K$ ]
A 107K{10^7}\,\,K
B 105K{10^5}\,\,K
C 103K{10^3}\,\,K
D 109K{10^9}\,\,K
Correct Answer
Option D
Solution

The average kinetic energy per molecule

=32kT= {3 \over 2}kT

This kinetic energy should be able to provide the repulsive potential energy \therefore

32kT=7.7×1014{3 \over 2}kT = 7.7 \times {10^{ - 14}}
T=2×7.7×10143×1.38×1023=3.7×109\Rightarrow T = {{2 \times 7.7 \times {{10}^{ - 14}}} \over {3 \times 1.38 \times {{10}^{ - 23}}}} = 3.7 \times {10^9}
Q24
If 13.613.6 eVeV energy is required to ionize the hydrogen atom, then the energy required to remove an electron from n=2n=2 is
A 10.210.2 eVeV
B 00 eVeV
C 3.43.4 eVeV
D 6.86.8 eV.eV.
Correct Answer
Option C
Solution

KEY CONCEPT : The energy of nth orbit of hydrogen is given by

En=13.6n2eV/{E_n} = {{13.6} \over {{n^2}}}eV/

atom For

n=2,n=2,
En=13.64=3.4eV{E_n} = {{ - 13.6} \over 4} = - 3.4eV

Therefore the energy required to remove electron from

n=2n = 2

is

+3.4eV.+3.4eV.
Q25
A nucleus with Z=92Z=92 emits the following in a sequence: α,β,β,α,α,α,α,α,β,β,α,β+,β+,α\alpha ,{\beta ^ - },{\beta ^ - },\alpha ,\alpha ,\alpha ,\alpha ,\alpha ,{\beta ^ - },{\beta ^ - },\alpha ,{\beta ^ + },{\beta ^ + },\alpha Then Then ZZ$ of the resulting nucleus is
A 7676
B 7878
C 8282
D 7474
Correct Answer
Option B
Solution

The number of α\alpha - particles released

=8=8

Therefore the atomic number should decrease by

1616

The number of

β{\beta ^ - }

- particles released

=4=4

Therefore the atomic number should increase by

4.4.

Also the number of

β+{\beta ^ + }

particles released is

2,2,

which should decrease the atomic number by

2.2.

Therefore the final atomic number is

9216+42=7892-16+4-2=78
Q26
When a U238{U^{238}} nucleus originally at rest, decays by emitting an alpha particle having a speed u,'u', the recoil speed of the residual nucleus is
A 4μ238{{4\mu } \over {238}}
B 4μ234 - {{4\mu } \over {234}}
C 4μ234 {{4\mu } \over {234}}
D 4μ238 - {{4\mu } \over {238}}
Correct Answer
Option C
Solution

Here, conservation of linear momentum can be applied

238×0=4u+234v238 \times 0 = 4u + 234v

\therefore

v=4234uv = - {4 \over {234}}u

\therefore speed

=v=4234u= |\overrightarrow v | = {4 \over {234}}u
Q27
The wavelengths involved in the spectrum of deuterium (12D)\left( {{}_1^2\,D} \right) are slightly different from that of hydrogen spectrum, because
A the size of the two nuclei are different
B the nuclear forces are different in the two cases
C the masses of the two nuclei are different
D the attraction between the electron and the nucleus is different in the two cases
Correct Answer
Option C
Solution

The wavelength of spectrum is given by

1λ=Rz2(1n121n22){1 \over \lambda } = R{z^2}\left( {{1 \over {n_1^2}} - {1 \over {n_2^2}}} \right)

where

R=1.097×1071+mMR = {{1.097 \times {{10}^7}} \over {1 + {m \over M}}}

where

m=m=

mass of electron

M=M=

mass of nucleus. For different

M,RM,R

is different and therefore λ\lambda is different

Q28
The binding energy per nucleon of deuteron (12H)\left( {{}_1^2\,H} \right) and helium nucleus (24He)\left( {{}_2^4\,He} \right) is 1.11.1 MeVMeV and 77 MeVMeV respectively. If two deuteron nuclei react to form a single helium nucleus, then the energy released is
A 23.6MeV23.6\,\,MeV
B 26.9MeV26.9\,\,MeV
C 13.9MeV13.9\,\,MeV
D 19.2MeV19.2\,\,MeV
Correct Answer
Option A
Solution

The nuclear reaction of process is

212H422_1^2H \to {4 \over 2}

He Energy released

=4×(7)4(1.1)=23.6MeV= 4 \times \left( 7 \right) - 4\left( {1.1} \right) = 23.6\,MeV
Q29
A nucleus disintegrated into two nuclear parts which have their velocities in the ratio of 2:1.2:1. The ratio of their nuclear sizes will be
A 31/2:1{3^{{{1}/{2}}}}:1
B 1:21/31:{2^{1/3}}
C 21/3:1{2^{1/3}}:1
D 1:31/21:{3^{{{1}/{2}}}}
Correct Answer
Option B
Solution

From conservation of momentum

m1v1=m2v2{m_1}{v_1} = {m_2}{v_2}
(m1m2)=(v2v1)\Rightarrow \left( {{{{m_1}} \over {{m_2}}}} \right) = \left( {{{{v_2}} \over {{v_1}}}} \right)\,\,

given

v1v2=2\,\,{{{v_1}} \over {v{}_2}} = 2
m1m2=12\Rightarrow {{{m_1}} \over {{m_2}}} = {1 \over 2}
r13r23=12\Rightarrow {{r_1^3} \over {r_2^3}} = {1 \over 2}
(r1r2)=(12)1/3\Rightarrow \left( {{{{r_1}} \over {{r_2}}}} \right) = {\left( {{1 \over 2}} \right)^{1/3}}
Q30
An α\alpha -particle of energy 55 MeVMeV is scattered through 180{180^ \circ } by a fixed uranium nucleus. The distance of closest approach is of the order of
A 1012cm{10^{ - 12}}\,cm
B 1010cm{10^{ - 10}}\,cm
C 1A1A
D 1015acm{10^{ - 15a}}\,cm
Correct Answer
Option A
Solution

KEY NOTE : Distance of closest approach

r0=Ze(2e)4πε0E{r_0} = {{Ze\left( {2e} \right)} \over {4\pi {\varepsilon _0}E}}

Energy,

E=5×106×1.6×1019JE = 5 \times {10^6} \times1.6 \times {10^{ - 19}}J

\therefore

r0=9×109×(92×1.6×1019)(2×1.6×1019)5×106×1.6×1019{r_0} = {{9 \times {{10}^9} \times \left( {92 \times 1.6 \times {{10}^{ - 19}}} \right)\left( {2 \times 1.6 \times {{10}^{ - 19}}} \right)} \over {5 \times {{10}^6} \times 1.6 \times {{10}^{ - 19}}}}
r=5.2×1014m=5.3×1012cm\Rightarrow r = 5.2 \times {10^{ - 14}}m = 5.3 \times {10^{ - 12}}cm
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