Atoms and Nuclei

JEE Physics · 201 questions · Page 5 of 21 · Click an option or "Show Solution" to reveal answer

Q41
This question contains Statement- 1 and Statement- 2. Of the four choices given after the statements, choose the one that best describes the two statements: Statement- 1: Energy is released when heavy nuclei undergo fission or light nuclei undergo fusion and Statement- 2: For heavy nuclei, binding energy per nucleon increases with increasing ZZ while for light nuclei it decreases with increasing Z.Z.
A Statement - 11 is false, Statement - 22 is true
B Statement - 11 is true, Statement - 22 is true; Statement - 22 is a correct explanation for Statement - 11
C Statement - 11 is true, Statement - 22 is true; Statement - 22 is not a correct explanation for Statement - 11
D Statement - 11 is true, Statement - 22 is false
Correct Answer
Option D
Solution

We know that energy is released when heavy nuclei undergo fission or light nuclei undergo fusion. Therefore statement

(1)(1)

is correct.

The second statement is false because for heavy nuclei the binding energy per nucleon decreases with increasing

ZZ

and for light nuclei, B.E/nucleon increases with increasing

ZZ

and for light nuclei,

B.E/B.E/

nucleon increases with increasing

Z.Z.
Q42
Suppose an electron is attracted towards the origin by a force kr{k \over r} where k'k' is a constant and r'r' is the distance of the electron from the origin. By applying Bohr model to this system, the radius of the nth{n^{th}} orbital of the electron is found to be rn'{r_n}' and the kinetic energy of the electron to be Tn.'{T_n}'. Then which of the following is true?
A Tn1n2,rnn2{T_n} \propto {1 \over {{n^2}}},{r_n} \propto {n^2}
B Tn{T_n} independent of n,rnnn,{r_n} \propto n
C Tn1n,rnn{T_n} \propto {1 \over n},{r_n} \propto n
D Tn1n,rnn2{T_n} \propto {1 \over n},{r_n} \propto {n^2}
Correct Answer
Option B
Solution

When

F=kr=F = {k \over r} =

centripetal force, then

kr=mv2r{k \over r} = {{m{v^2}} \over r}
mv2=\Rightarrow m{v^2} =

constant \Rightarrow kinetic energy is constant

T\Rightarrow T

is independent of

n.n.
Q43
The transition from the state n=4n=4 to n=3n=3 in a hydrogen like atom result in ultra violet radiation. Infrared radiation will be obtained in the transition from :
A 323 \to 2
B 424 \to 2
C 545 \to 4
D 212 \to 1
Correct Answer
Option C
Solution

It is given that transition from the state

n=4n=4

to

n=3n=3

in a hydrogen like atom result in ultraviolet radiation.

For infrared radiation the energy gap should be less.

The only option is

55
4.\to 4.
Q44
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 speed of daughter nuclei is
A cΔmM+Δmc{{\Delta m} \over {M + \Delta m}}
B c2ΔmMc\sqrt {{{2\Delta m} \over M}}
C cΔmMc\sqrt {{{\Delta m} \over M}}
D cΔmM+Δmc\sqrt {{{\Delta m} \over {M + \Delta m}}}
Correct Answer
Option B
Solution

By conservation of energy,

(M+Δm)c2=2M2c2+12.2M2v2,\left( {M + \Delta m} \right){c^2} = {{2M} \over 2}{c^2} + {1 \over 2}.{{2M} \over 2}{v^2},

where

vv

is the speed of the daughter nuclei

Δmc2=M2v2\Rightarrow \Delta m{c^2} = {M \over 2}{v^2}

\therefore

v=c2ΔmMv = c\sqrt {{{2\Delta m} \over M}}
Q45
The half life of a radioactive substance is 2020 minutes. The approximate time interval (t2t1)\left( {{t_2} - {t_1}} \right) between the time t2{{t_2}} when 23{2 \over 3} of it had decayed and time t1{{t_1}} when 13{1 \over 3} of it had decayed is :
A 1414 min
B 2020 min
C 2828 min
D 77 min
Correct Answer
Option B
Solution

Number of undecayed atom after time

t2;{t_2};
N03=N0eλt2...(i){{{N_0}} \over 3} = {N_0}{e^{ - \lambda {t_2}}}\,\,\,\,\,\,\,\,\,\,\,\,\,...\left( i \right)

Number of undecayed atom after time

t1;{t_1};
2N03=N0eλt1...(ii){{2{N_0}} \over 3} = {N_0}{e^{ - \lambda {t_1}}}\,\,\,\,\,\,\,\,\,\,\,\,\,...\left( {ii} \right)

From

(i),(i),
eλt2=13{e^{ - \lambda {t_2}}} = {1 \over 3}
λt2=loge(13)...(iii)\Rightarrow - \lambda {t_2} = {\log _e}\left( {{1 \over 3}} \right)\,\,\,\,\,\,\,\,...\left( {iii} \right)

From

(ii)(ii)
eλt2=23- {e^{ - \lambda {t_2}}} = {2 \over 3}
λt1=loge(23)...(iv)\Rightarrow - \lambda {t_1} = {\log _e}\left( {{2 \over 3}} \right)\,\,\,\,\,\,\,\,\,\,...\left( {iv} \right)

Solving

(iii)(iii)

and

(iv),(iv),

we get

t2t1=20{t_2} - {t_1} = 20\,

min

Q46
Energy required for the electron excitation in Li++L{i^{ + + }} from the first to the third Bohr orbit is :
A 36.336.3 eVeV
B 108.8108.8 eVeV
C 122.4122.4 eVeV
D 12.112.1 eVeV
Correct Answer
Option B
Solution

Energy of excitation,

ΔE=13.6Z2(1n121n22)eV\Delta E = 13.6\,{Z^2}\left( {{1 \over {n_1^2}} - {1 \over {n_2^2}}} \right)eV
ΔE=13.6(3)2(112132)=108.8eV\Rightarrow \Delta E = 13.6{\left( 3 \right)^2}\left( {{1 \over {{1^2}}} - {1 \over {{3^2}}}} \right) = 108.8\,eV
Q47
Hydrogen atom is excited from ground state to another state with principal quantum number equal to 4.4. Then the number of spectral lines in the emission spectra will be :
A 22
B 33
C 55
D 66
Correct Answer
Option D
Solution

The possible number of the spectral lines is given

=n(n1)2=4(41)2=6= {{n\left( {n - 1} \right)} \over 2} = {{4\left( {4 - 1} \right)} \over 2} = 6
Q48
Assume that a neutron breaks into a proton and an electron. The energy released during this process is : (mass of neutron =1.6725×1027kg, = 1.6725 \times {10^{ - 27}}kg, mass of proton =1.6725×1027kg, = 1.6725 \times {10^{ - 27}}\,kg, mass of electron =9×1031kg = 9 \times {10^{ - 31}}\,kg ).
A 0.510.51 MeVMeV
B 7.10MeV7.10\,MeV
C 6.30MeV6.30\,MeV
D 5.4MeV5.4\,MeV
Correct Answer
Option A
Solution
01n11H+1e0+v+Q{}_0^1n \to {}_1^1H + {}_{ - 1}{e^0} + \overrightarrow v + Q

The mass defect during the process

Δm=mnmHme\Delta m = {m_n} - {m_H} - {m_e}
=1.6725×1027(1.6725×1027+9×1031kg)= 1.6725 \times {10^{ - 27}} - \left( {1.6725 \times {{10}^{ - 27}} + 9 \times {{10}^{ - 31}}kg} \right)
=9×1031kg= - 9 \times {10^{ - 31}}kg

The energy released during the process

E=Δmc2E = \Delta m{c^2}
E=9×1031×9×1016E = 9 \times {10^{ - 31}} \times 9 \times {10^{16}}
=81×1015joules= 81 \times {10^{ - 15}}\,joules
E=81×10151.6×1019=0.511MeVE = {{81 \times {{10}^{ - 15}}} \over {1.6 \times {{10}^{ - 19}}}} = 0.511MeV
Q49
A diatomic molecule is made of two masses m1{m_1} and m2{m_2} which are separated by a distance r.r. If we calculate its rotational energy by applying Bohr's rule of angular momentum quantization, its energy will be given by: (nn is an integer)
A (m1+m2)2n2h22m12m22r2{{{{\left( {{m_1} + {m_2}} \right)}^2}{n^2}{h^2}} \over {2m_1^2m_2^2{r^2}}}
B n2h22(m1+m2)r2{{{n^2}{h^2}} \over {2\left( {{m_1} + {m_2}} \right){r^2}}}
C 2n2h2(m1+m2)r2{{2{n^2}{h^2}} \over {\left( {{m_1} + {m_2}} \right){r^2}}}
D (m1+m2)n2h22m1m2r2{{\left( {{m_1} + {m_2}} \right){n^2}{h^2}} \over {2{m_1}{m_2}{r^2}}}
Correct Answer
Option D
Solution

The energy of the system of two atoms of diatomic molecule

E=12IωE = {1 \over 2}I\omega

where

I=I=

moment of inertia

ω=\omega =

Angular velocity

=LI.= {L \over I}.
L=L=

Angular momentum

I=12(m1r12+m2r22)I = {1 \over 2}\left( {{m_1}{r_1}^2 + {m^2}{r_2}^2} \right)

Thus,

E=12(m1r12+m2r22)ω2...(i)E = {1 \over 2}\left( {{m_1}{r_1}^2 + m{}_2{r_2}^2} \right){\omega ^2}\,\,\,\,\,\,\,\,\,...\left( i \right)
E=12(m1r12+m2r22)L2I2E = {1 \over 2}\left( {{m_1}{r_1}^2 + {m_2}{r_2}^2} \right){{{L^2}} \over {{I^2}}}
L=nnh2nL = n{{nh} \over {2n}}

(According Bohr's Hypothesis)

E=12(m1r12+m2r22)L2(m1r12+m2r22)2E = {1 \over 2}\left( {{m_1}{r_1}^2 + {m_2}{r_2}^2} \right){{{L^2}} \over {{{\left( {{m_1}{r_1}^2 + {m_2}{r_2}^2} \right)}^2}}}
E=12L2(m1r12+m2r22)E = {1 \over 2}{{{L^2}} \over {\left( {{m_1}{r_1}^2 + {m_2}{r_2}^2} \right)}}
=n2h28π2(m1r12+m2r22)= {{{n^2}{h^2}} \over {8{\pi ^2}\left( {{m_1}{r_1}^2 + {m_2}{r_2}^2} \right)}}
E=(m1+m2)n2h28π2r2m1m2E = {{\left( {{m_1} + {m_2}} \right){n^2}{h^2}} \over {8{\pi ^2}{r^2}{m_1}{m_2}}}
[\left[ {\,\,} \right.

as

r1=m2rm1+m2;r2=m2rm1+m2]\left. {\,\,\,{r_1} = {{{m_2}r} \over {{m_1} + {m_2}}};\,{r_2} = {{{m_2}r} \over {{m_1} + {m_2}}}\,\,} \right]
Q50
The radiation corresponding to 323 \to 2 transition of hydrogen atom falls on a metal surface to produce photoelectrons. These electrons are made to enter a magnetic field 3×104T.3 \times {10^{ - 4}}\,T. If the radius of the larger circular path followed by these electrons is 10.010.0 mmmm, the work function of the metal is close to:
A 1.81.8 eVeV
B 1.11.1 eVeV
C 0.80.8 eVeV
D 1.61.6 eVeV
Correct Answer
Option B
Solution

Radius of circular path followed by electron is given by,

r=mυqB=2meVeB=1B2meVr = {{m\upsilon } \over {qB}} = {{\sqrt {2meV} } \over {eB}} = {1 \over B}\sqrt {{{2m} \over e}V}
V=B2r2e2m=0.8V\Rightarrow V = {{{B^2}{r^2}e} \over {2m}} = 0.8V

For transition between

33

to

2.2.
E=13.6(1419)E = 13.6\left( {{1 \over 4} - {1 \over 9}} \right)
=13.6×536=1.88eV= {{13.6 \times 5} \over {36}} = 1.88eV

Work function

=1.88eV0.8eV= 1.88eV - 0.8eV
=1.08eV1.1eV= 1.08eV \approx 1.1eV
Ready for a full JEE mock test? Timed · full syllabus · instant results
Take a Mock Test →