Atoms and Nuclei

JEE Physics · 201 questions · Page 6 of 21 · Click an option or "Show Solution" to reveal answer

Q51
Hydrogen (1H1)\left( {{}_1{H^1}} \right), Deuterium (1H2)\left( {{}_1{H^2}} \right), singly ionised Helium (2He4)+{\left( {{}_2H{e^4}} \right)^ + } and doubly ionised lithium (3Li6)++{\left( {{}_3L{i^6}} \right)^{ + + }} all have one electron around the nucleus. Consider an electron transition from n=2n=2 to n=1.n=1. If the wavelengths of emitted radiation are λ1,λ2,λ3{\lambda _1},{\lambda _2},{\lambda _3} and λ4{\lambda _4} respectively then approximately which one of the following is correct?
A 4λ1=2λ2=2λ3=λ44{\lambda _1} = 2{\lambda _2} = 2{\lambda _3} = {\lambda _4}
B λ1=2λ2=2λ3=λ4{\lambda _1} = 2{\lambda _2} = 2{\lambda _3} = {\lambda _4}
C λ1=λ2=4λ3=9λ4{\lambda _1} = {\lambda _2} = 4{\lambda _3} = 9{\lambda _4}
D λ1=2λ2=3λ3=4λ4{\lambda _1} = 2{\lambda _2} = 3{\lambda _3} = 4{\lambda _4}
Correct Answer
Option C
Solution

Wave number

1λ=RZ2[1n121n2]{1 \over \lambda } = R{Z^2}\left[ {{1 \over {n_1^2}} - {1 \over {{n^2}}}} \right]
λ1Z2\Rightarrow \lambda \propto {1 \over {{Z^2}}}

By question

n=1n=1

and

n1=2{n_1} = 2

Then,

λ1=λ2=4λ3=9λ4{\lambda _1} = {\lambda _2} = 4{\lambda _3} = 9{\lambda _4}
Q52
As an electron makes a transition from an excited state to the ground state of a hydrogen - like atom/ion :
A kinetic energy decreases, potential energy increases but total energy remains same
B kinetic energy and total energy decrease but potential energy increases
C its kinetic energy increases but potential energy and total energy decrease
D kinetic energy, potential energy and total energy decrease
Correct Answer
Option C
Solution
U=Kze2r;T.E=k2ze2rU = - K{{z{e^2}} \over r};\,\,T.E = {k \over 2}{{ze^2} \over r}
K.E=k2ze2r.K.E = {k \over 2}{{z{e^2}} \over r}.

Here

rr

decreases

Q53
A He+ ion is in its first excited state. Its ionization energy is :-
A 13.60 eV
B 6.04 eV
C 48.36 eV
D 54.40 eV
Correct Answer
Option A
Solution
T.E.=(13.6)(Z2n2)eVT.E. = - \left( {13.6} \right)\left( {{{{Z^2}} \over {{n^2}}}} \right)eV

z = n = 2 \Rightarrow Ionisation energy = –T.E. = 13.6 eV

Q54
Half-lives of two radioactive elements AA and BB are 2020 minutes and 4040 minutes, respectively. Initially, the samples have equal number of nuclei. After 8080 minutes, the ratio of decayed number of AA and BB nuclei will be:
A 1:41:4
B 5:45:4
C 1:161:16
D 4:14:1
Correct Answer
Option B
Solution

For

At1/2=20{A_{t{{1}/{2}}}} = 20\,\,

min,

t=80t=80

min, number of half lifes

n=4n=4

\therefore Nuclei remaining

=N024.= {{{N_0}} \over {{2^4}}}.

Therefore nuclei decayed

=N0N024= {N_0} - {{{N_0}} \over {{2^4}}}

For

Bt1/2=40{B_{t{{1}/{2}}}} = 40\,\,

min,

t=80t=80

min, number of half lifes

n=4n=4

\therefore Nuclei remaining

=N022.= {{{N_0}} \over {{2^2}}}.

Therefore nuclei decayed

=N0N022= {N_0} - {{{N_0}} \over {{2^2}}}

\therefore Required ratio

=N0N024N0N022= {{{N_0} - {{{N_0}} \over {{2^4}}}} \over {{N_0} - {{{N_0}} \over {{2^2}}}}}
=1116114= {{1 - {1 \over {16}}} \over {1 - {1 \over 4}}}
=1516×43=54= {{15} \over {16}} \times {4 \over 3} = {5 \over 4}
Q55
Imagine that a reactor converts all given mass into energy and that it operates at a power level of 109 watt. The mass of the fuel consumed per hour in the reactor will be : (velocity of light, c is 3×108 m/s)
A 0.96 gm
B 0.8 gm
C 4 × \times 10-2 gm
D 6.6 × \times 10-5 gm
Correct Answer
Option C
Solution

The power can be calculated by the relation

P=EΔt=Δmc2ΔtP = {E \over {\Delta t}} = {{\Delta m{c^2}} \over {\Delta t}}

...... (1) Therefore, from Eq. (1), the mass of the fuel consumed per hour in the reactor is

ΔmΔt=Pc2=109(3×108)2=4×1012{{\Delta m} \over {\Delta t}} = {P \over {{c^2}}} = {{{{10}^9}} \over {{{(3 \times {{10}^8})}^2}}} = 4 \times {10^{ - 12}}

g

Q56
The acceleration of an electron in the first orbit of the hydrogen atom (n = 1) is :
A h2π2m2r3{{{h^2}} \over {{\pi ^2}{m^2}{r^3}}}
B h28π2m2r3{{{h^2}} \over {{8\pi ^2}{m^2}{r^3}}}
C h24π2m2r3{{{h^2}} \over {{4\pi ^2}{m^2}{r^3}}}
D h24πm2r3{{{h^2}} \over {{4\pi }{m^2}{r^3}}}
Correct Answer
Option C
Solution

The speedy of the particle in the orbit of an atom is

v=I22hε0v = {{{I^2}} \over {2h{\varepsilon _0}}}

We have the radius of the first orbit is

r=h2ε0πme2r = {{{h^2}{\varepsilon _0}} \over {\pi m{e^2}}}
ε0=rπme2h2\Rightarrow {\varepsilon _0} = {{r\pi m{e^2}} \over {{h^2}}}

Therefore, the acceleration of an electron in the first orbit of the hydrogen atom (n = 1) is

v2r=I6πm4h2ε03=h24r3π2m2{{{v^2}} \over r} = {{{I^6}\pi m} \over {4{h^2}\varepsilon _0^3}} = {{{h^2}} \over {4{r^3}{\pi ^2}{m^2}}}
Q57
According to Bohr’s theory, the time averaged magnetic field at the centre (i.e. nucleus) of a hydrogen atom due to the motion of electrons in the nth orbit is proportional to : (n = principal quantum number)
A n4{n^{ - 4}}
B n5{n^{ - 5}}
C n-3
D n-2
Correct Answer
Option B
Solution

Magnetic field at the center of neucleus of H-atom B =

μ0I2rn{{{\mu _0}I} \over {2{r_n}}}

Radius of nth orbital, rn =

n2h2ε0mπZe2{{{n^2}{h^2}{\varepsilon _0}} \over {m\pi Z{e^2}}}
\therefore\,\,\,

rn \propto n2 velocity of electron in nth orbital,

υ\upsilon

n =

(e2h2ε0)Zn\left( {{{{e^2}h} \over {2{\varepsilon _0}}}} \right){Z \over n}
\therefore\,\,\,
υ\upsilon

n \propto n-1 I =

qt{q \over t}

=

e2πrnυn{e \over {{{2\pi {r_n}} \over {{\upsilon _n}}}}}

=

eυn2πrn{{e{\upsilon _n}} \over {2\pi {r_n}}}
\therefore\,\,\,

B =

μ0.(eυn2πrn)2rn{{{\mu _0}.\left( {{{e{\upsilon _n}} \over {2\pi {r_n}}}} \right)} \over {2{r_n}}}

=

μ0eυn4πrn2{{{\mu _0}\,e{\upsilon _n}} \over {4\pi r_n^2}}
\therefore\,\,\,

B \propto

υnrn2{{{\upsilon _n}} \over {r_n^2}}

\Rightarrow

\,\,\,

B \propto

n1n4{{{n^{ - 1}}} \over {{n^4}}}

\Rightarrow

\,\,\,

B \propto n -5

Q58
Two radioactive substances A and B have decay constants 5λ\lambda and λ\lambda respectively. At t = 0, a sample has the same number of the two nuclei. The time taken for the ratio of the number of nuclei to become (1e)2{\left( {{1 \over e}} \right)^2} will be :
A 2λ{2 \over \lambda }
B 14λ{1 \over {4\lambda }}
C 12λ{1 \over {2\lambda }}
D 1λ{1 \over {\lambda }}
Correct Answer
Option C
Solution

Nx(at t) = N0e–5λ\lambdat Ny(at t) = N0e–λ\lambdat

NxNy=1e2=e4λt{{{N_x}} \over {{N_y}}} = {1 \over {{e^2}}} = {e^{ - 4\lambda t}}
4λt=2\Rightarrow 4\lambda t = 2
t=24λ=(12λ)\Rightarrow t = {2 \over {4\lambda }} = \left( {{1 \over {2\lambda }}} \right)
Q59
A radioactive nucleus A with a half life T, decays into a nucleus B. At t = 0, there is no nucleus B. At sometime t, the ratio of the number of B to that of A is 0.3. Then, t is given by :
A t=Tlog(1.3)t = {T \over {\log (1.3)}}
B t=Tlog(1.3)t = T\log (1.3)
C t=T2log2log1.3t = {T \over 2}{{\log 2} \over {\log 1.3}}
D t=Tlog1.3log2t = T{{\log 1.3} \over {\log 2}}
Correct Answer
Option D
Solution

Let initially there are total N0 number of nuclei. At time t

NBNA{{{N_B}} \over {{N_A}}}

= 0.3 (given) \Rightarrow

NB{{N_B}}

= 0.3

NA{{N_A}}

N0 = NA + NB = NA + 0.3NA \therefore NA =

N01.3{{{N_0}} \over {1.3}}

As we know Nt = N0 e– λ\lambdat \Rightarrow

N01.3{{{N_0}} \over {1.3}}

= N0 e– λ\lambdat \Rightarrow

11.3{1 \over {1.3}}

= e– λ\lambdat \Rightarrow ln(1.3) = λ\lambdat \Rightarrow t =

ln(1.3)λ{{\ln \left( {1.3} \right)} \over \lambda }

If T is half-life, then λ\lambda =

ln2T{{{{\ln} } 2} \over T}

\Rightarrow t =

ln(1.3)ln2T{{\ln \left( {1.3} \right)} \over {{{\ln 2} \over T}}}

=

ln(1.3)ln2T{{\ln \left( {1.3} \right)} \over {\ln 2}}T
Q60
A solution containing active cobalt 2760Co{^{60}_{27}}Co having activity of 0.80.8 μCi\mu Ci and decay constant λ\lambda is injected in an animal's body. If 1cm31\,c{m^3} of blood is drawn from the animal's body after 1010 hrs of injection, the activity found was 300300 decays per minute What is the volume of blood that is flowing in the body ? (Ci=3.7×1010\left( {\,\,Ci = 3.7 \times {{10}^{10}}\,} \right. decays per second and at t=10t=10 hrs eλt=0.84)\left. {{e^{ - \lambda t}} = 0.84} \right)
A 66 liters
B 77 liters
C 44 liters
D 55 liters
Correct Answer
Option D
Solution

Initial activity, No = 0.8 μ\muCi Activity at time t, N = N0 e-λ\lambdat Activity in 1 cm3 blood after 10 hr, n = 300 decays per minute =

30060dps{{300} \over {60}}\,dps

= 5 dps. Activity in whole blood after to hr = N0 e-λ\lambda×\times10

\therefore\,\,\,\,

Volume of the total blood =

N0e10λn{{{N_0}{e^{ - 10\lambda }}} \over n}

=

0.8×107×3.7×1010×0.845{{0.8 \times {{10}^{ - 7}} \times 3.7 \times {{10}^{10}} \times 0.84} \over 5}

= 4.97 ×\times 103 cm3 = 4.97 litres

\simeq

5 liters.

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