12 TH Last 2 Chapter
12 TH Last 2 Chapter
EXPLANATIONS
2 kS2,
both A and B is/are open. Hence it 7. (b): Given: V= 3 V, R=
A or B or
gate. B 100
a NAND
represents
1.9 eV Voltage gain of the CE amplifier,
3. (b): Given, energy gap =
B - Y
A BC C Output (Y)
0 0 1 |0
010 1 0
B
0 0 1|
Y=(A B+A B)
Also, A or V ==-
A 200
Collector current, I = (20-0)
4x10 y100 =20 mV
or
Ic=5 x 10-3 A 5 mA =
11. (a): Diode D, 22
Input voltage, V, VBE + IpRg =
is reverse biased R
or so, it will block
V,=0+IpRg or 20 I x 500 x
10 10 V
the current and R, 2 2
20
= 40 HA diode D is forward
500 x 103 biased, so it will pass
the current.
Current gain, B= C 5 x 1 0 3 = 125
Hence, equivalent circuit becomes
40x10-6
as shown in
the figure.
Weo N TAIPMI Chapterwise Sotutions y
areve in the i uit ent owing 17. ()
thwaghthe vsistanne W
i4
2S
A
12 V
The potential difference across the resistance R
48N AN is
V SV 05V AV
t 4-8--0then -0-1 By Ohms law,
h-8--othen, -I-0 Thecurrent in the circuit is
AV
AK
10A 010 'A 30 mA
R 100
09643.84
sc (Short creult current)
15. (d)
Here, the p-n junetion diode is
trwand biased. hence it ofters zero resistance. 20. (d): "The barrier potential depends on type
of semiconductor (Por St, V, 0.7 V and for
AN V4N-(6) A =10
AGe,V,0.3 V), amount of doping and also on
RAB ks 1000
the temperature.
16 (b): Here.lnput signal. V, = 20os|15+ 2 21. (c): Voltage gain
and voltag* gain, A, 150 Current gain x Resistanee gain
As A, A,
Transconductance, Sm or R
Outputsignal. \A, Sm
Sune CE amplifier gives a phase ditlerence of ASRt
For tirst case, A, =G, g 0.03 mho,
-I80°) between input and output sigals, p25
G 0.03 Rut
()
For second case, A, Gg 0.02 mho, f20
0.02R, (ii)
Divide (ii) by (), we
get
G
Semiconductor Electronics Materials, Devices and Simple Circuits 331
electrons Region (II) - Active region
22. (a): In n-type semiconductor, Region (11) - Saturation region
carriers and holes are
are majority charge
carriers and pentavalent atoms Using transistor as a switch it is used in cutoff
minority charge region or saturation region.
are dopants.
Using transistor as an amplifier it is used in
23. (a): R A.B active region.
circuit is 31. (a): The truth table ofthe given waveform
The output of the given logic
is as shown in the table.
X = A.B = A.B
Time interval Input A Input B Output C |
0 to t 0
24. (a) , to t2 0
2 k2 2 x 10 2 33. (b):
28. (d): Here, R = =
A
1 k2 1 x 10' 2, B = 100
V=2 V, R, = =
Inputs Output
= 102 V= 10 mV
B C Y=(A+ B) C
Electronic configuration of carbon
29. (c) :
0
(C) is Is 2s 2p. The electronic configuration
0
of silicon (,,Si) is 1s 2s 2ps 3s 3p?
0
Hence, the four electrons of C and Si
bonding
orbit. 0
respectively lie in second and third
30. (b): In the given graph, From the above truth table it is clear that Y = 1,
when A = 1, B = 0 and C = 1
Region () -Cutoff region
332 wbG NEET-AIPMT Chapterwise Solutions Physics
The current through the zener diode is
Al
34. (a): Current gain. 5= I, I - I = (20 15)mA =5 mA
100 2
2
2
:B=_
10V
Output
I-Ic
Now, E _ 1 - _0.04
67. (b): The truth table of OR gate is c 0.96 Ic 0.96 0.96
_ 0.96
B=C_ 24
A BY
0 0 0 Y=A +B
- I c 0.04
75. (a) :
P
Hole Electron
From truth table we can observe that if either of Electron
input is one then output is one. Also if both the
Hole
inputs are one then also output is one.
68. (c): A diode is said to be reverse biased if Depletion layer
p-type semiconductor of p-n junction is at low A p-n junction is shown in the figure. On
potential with respect to n-type semiconductor account of difference in concentration of charge
ofp-n junction. It is so for circuit (c). carriers in the two sections of p-n junction,
69. (b): n reverse biasing, the conduction the electrons from n-region diffuse through
across the p-n junction takes place due to the junction into p-region and the holes from
minority carriers, therefore the size of depletion p-region diffuse into n region.
region (potential barrier) rises. Since the hole is a vacancy of an electron.
70. (b): A n-p-n transistor conducts when when an electron from n region diffuses
emitter-base junction is forward biased while into the p-region, the electron falls into the
collector-base junction is reverse biased. vacancy, i.e., it completes the covalent bond.
71. (d): In full wave rectifier the fundamental Due to migration of charge carriers across
frequency in ripple is twice of input frequency. the junction, the n-region of the junction will
72. (a) Barrier
potential depends upon have its electrons neutralized by holes from
temperature, doping density and forward biasing the p-region, leaving only ionised donor atoms
73. (c):In body-centred cubic (b.c.c.) lattice (positive charges) which are bound and cannot
there are eight atoms at the corners of the cube move. Similarly, the p region of the junction will
and one at the centre as shown in the figure. have ionised acceptor atoms (negative charges)
which are immobile.
The accumulation of electric charges of opposite
polarities in the two regions of the junction gives
rise to an electric field between these regions
is connected across the
as
if a fictitious battery
connected
Junction with its positive terminal
connected
b.c.c. structure to n region and negative terminal
Semiconductor Electronics Materials, Devices and Simple Circuits 335
to p region. Theretore, in a p-n junction high
(b): B 41
potential is at n side and low potential is at p side.
82. (b): P =-_- -11-(0,11,)1-
76. (a): NAND gate is a combination of AND
83. (d): As a p-n junction diode conducts
and NOT gate.
ABY in forward bias and does not conduct in
0 0 0 reverse bias (current is practically zero), thus
A 0
Y 0 undirectional property leads to application of
B
diode in rectifiers.
AND gate
Truth table of AND gate 84. (a): Atomic radius for body centered
ANSWER KEY
EXPLANATIONS
1. (d): Total energy of electron in nh orbit, and its ground state energy, E,= -13.6 eV
-13.622
Charge of muon =charge of electron
eV Mass of muon = 207 x (mass of electron)
E,
n
Kinetic energy of electron in nh orbit, Therefore, when electron is replaced by muon
0.51A
K.E,=3.622
then,first Bohr radius, =
?ev
207
2.56 x 10 m
Potential energy of electron in n orbit, and ground state energy, Ej = -13.6 x 207
PE= -eV
4. (d): Given, 2 = 2.2 x 10 s
-9F =
7
27T,=2x 10 minutes =20 minutes 10. (d): No = Nuclei at time t = 0
b ) : In a Bohr orbit
of the hydrogen atom, N =
Remaining nuclei after 40% decay
Ametik
Su
enengy= (Total energy)
-
=
(1 -
0.4) N, =
0.6 No%
Ainctic energy: Total energy =1:-1| N, =
Remaining nuclei after 85% decay
C)The number of =
(1 - 0.85) N, 0.15 No
radioactive nuclei 'N
=
nucleus
Pih and that of helium nucleus is Binding energy of He
Th 2myh 4x 7.06 MeV 28.24 MeV
The reaction is
Kae 2mie
Piic ATh-Pth | e li+ H2(He)+Q
KHc Pte h
ButPh Pie and mHe mTh Q= 2(BE of He)-(BE of Li)
Th Kue or Kiue Kh
28.24 MeV 39.2 MeV
Thus the helium nucleus has more kinetic =2 x
2 x9.7 x 1o-19
9.1x10-31.6 x10° ms
=
No-x = No N--)
So three half lives would have been passed.
t= nT =3 x 1.4 x 10 years
15. (c): Energy of the photon, E=" = 4.2 x 10 years
Hence, the age of the rock is 4.2 x 10 years.
E=
6.63 x107 x3x10, 18. (): The wavelength of different spectral
975 x10l0
lines of Lyman series is given by
6.63 x10x3x10 1 eV =12.75 eV
975x10x1.6X101 wheren=2,3,4,..
After absorbing a photon of energy 12.75 eV,
where subscript L refers to Lyman.
the electron will reach to third excited state
For longest wavelength, n = 2
of energy -0.85 eV, since energy difference
l and n 4 is 12.75 eV.
corresponding to n = =
--
..()
Number of spectral lines emitted
longest
(n)n-1)_(4)(4-1) The wavelength of different spectral series of
2 Balmer series is given by
-0.85 eV
-1.5l eV
n=
where n =
3, 4,5,.
-3.4 eV
where subscript B reters to Balmer
For longest wavelength, n = 3
- 13.6 eV
Bongs
()
Solutions Physics
30 mbG NEET-AIPMT Chapterwise
4
n= 3, n,
=
R )
36 3 27 3
In second case, n, =
2, n, =
AM931 MeV 20
4 36 7
25. (c): Nuclear radius, R = R,A
(0.02866 931 MeV= 26.7MeV=6.675 MeV
4 constant and A is the mass number
where R, is a
20. (d): Y RAL_(27) 3
Initial number of atoms No 0 Cu (64)!/3 4
Number of atoms after N No-N
time or RcuXRA=x3.6fermi =4.8 fermi
As per question
26. (d): Let after t s amount of the A, and Az
N
7N= Ng - N or 8N =No will become equal in the mixture.
Ng-N 7
N
As N=No
No where n is the number of half-lives
where n is the no. of half lives
A /20
For A, N=Nou
=I(excited stale)
Acording to Rydberg formula Here, n= 1, n, = 5
ingtnconerrvationof linear momentum
31 (b):
stamentum o photon - Momentum of atom
where n is umber of half live
24R 24hR
7 1 O1 1
191A
-(- or m-4
Ar A (3x 10 m/s
At time ofthesample had decayed, 10
9 x 1 0 1 68 / s
-lt2-) x60x60
Ar
60=|
9x 10
kg/s (3600 )
= 4x 10 kg =40 x 10g= 40 mg
l-1)= In2 33. (b): Momentum of emitted photon
hu
In2 In 2 In2 =Pphoton C
In 2 From the law of conservation of linear
Ti/2 momentum, Momentum of recoil nucleus
=
T =
alpha
34. (c):When an
particleHei
emitted, the mass number and the atomic
number of the daughter nucleus decreases by
32 four and two respectively. Whei a beta partile
or Z= 4 or Z = 2
310 mtG NEET-AIPMT Chapterwise Solutions Physics
(B) is emitted. the atomic number of the Number of nuclei of R
daughter nucleus increases by one but the mass 4N M, INo ,9No
2
number remains the same.
= - =
Np =4N
/l
Ng -No[;)
/2
No-No3
el=eA
As Np =
No
5A=lor A= per minute
laking natuual logaritlhms ot both sides ot above 49. (c): ZM, + (A - Z)M, - M(A, Z)
-
B.E
mass defect =
44 TR
3
=(-3.4 + 13.6)
= 10.2 eV
. (ii)
(Ns
- 18se Divide (i) by (ii), we get
emtted here
=AAAg or., A=-5À-À)¥
N3
312 WbG NEET-AIPMT Chapterwise Solutions Physics
C (C)-C" E =-13.6-3.4
22
eV
Kinetic energy of an electron in the first excited
or, 4Ar2
4A
state is
54. (a): In beta nminus (B) decay, a neutron K= -E, = 3.4 eV.
is transtormed into a proton and an electron
59. (c): lonisation potential of hydrogen atom
is emitted with the nucleus along with an
is 13.6 eV.
antineutrino.
Energy required for exciting the hydrogen atom
+c +, where i
is the antineutrino. in the ground state to orbit n is given by
q or, 1-_2V
Ra Re -12
F
BR
Since V, B are constants, or, R = R,e"Ali-12)
charge on the ion
Or, -
mass ot reactant
-13.6 -13.6eV Am = c- a - b
E (Am) x 931 or, E
=
=(c -
a -
b).
AIDmS and Nuclei 313
74. (c)
64. (a): K.E=P.E
75. (d):
is ncgative.
But PE. Volume of atom
Total energy 3 = 105
Volume of nucleus
r(10
E-PE--.4eV.
K.E. =+3.4 eV. 76. (a): Let, f = 0, M, = 10 g
2 (given)
66. (c)
Then from, M = Moe = 10ce
+ (Ep -
E)
-1o-1.356
hc hc
hc 77. (a): Radius offirst orbit, r «
will be minimum.
105.(c)
=8
106.(d): In nuclear fission, the chain reaction
is controlled in such way that only one neutron,
Time for S8 half life = 100 hours.
produced in each fission, causes further fission.
s7. (b): 2dsino = tà : (sino)max = 1 Therefore some moderator is used to slow
ic., a
2
88. (a): E
107.(c): Energy of the ground electronic state
-13.6 eV
ofhydrogen atom E =
92. (a):u E
13.6
n)
13.63.4
(2
ev.
its
93. (a) 94. (a) 95. (a) 108.(b): When a hydrogen atom is in
excited level, then n = 2.
96. (b): Jump to second orbit leads to Balmer
Theretore radius of hydrogen atom in its irst
series. The jump from 4th orbit shall give rise to
excited level (r) * n*r,« (2) = 4 r
second line of Balmer series.
97. (d) 109.(b): Y-ray are most penetrating radiations
98. (b,d): la reduce the mass number by 110.(b): By the law of photo-electric etfect
4units and atomic number by 2 units, while 1ß
=eV or
only increase the atomic number byl unit.
'Number in
-