SOLUTIONS
- (d) : i =
ε
ReRt
1 − L
−
; i =12
6
1
6
V 84103
Ω
−
−
×
−
et
.|1 A| = ( 21.
6A) −^84103
−
×
−
et − ×−
e6 t- (^103) =^1
2
or
6
84 103
t. × −
= ln 2 t = (.0 693)(^84 .)^10
6× −^3
= 0.00097 s = 0.97 ms | 1 ms.- (d) : Vrms =
20
2
V
XL = ZL = (5 × 10–3 H) 2000
rad
s
= 10 :
XC =
1
ωC=
1
()50 10×^6 . 2000
−F rad
s= 10 :
R = RR + RL R = 6 : + 4 : = 10 :
Z = ()XXLC−+^22 R
= () 10 ΩΩ−+ 10 22 () 10 Ω = 10 :
Irms =V
Z
rms =^20
210V
()Ω
= ()^2 A = 1.4 A
Vvoltmeter = Irms ()XXLC−+RL
22= () 21 A. () 01 ΩΩ−+ 0422 ()Ω
= 42 V = 5.6 V
- (d) : I =
V
R
=
220 100
20
sin( πt) I = 11 sin (100pt)
Here peak value = 11 AIt happens for the rst time when (100pt 1 ) =π
2
t 1 =1
200
se rms value of I =11
2
.
It happens when (100pt 2 ) =3
4
πt 2 =^3
400(t 2 – t 1 ) =3
400
–
1
200
=
1
400
s = 2.5 × 10 –3 s.- (a) : For terminal velocity net force on the rod must
be zero
BIlm==gieI×
×,.., =..
.02 98.
06 198
3ANow if e is the emf induced in the rod,
e × I = P = P 1 + P 2So, e=+
=
(. .)
(./)
.
076120
983
06 V
Now as this e is generated due to motion of rod with
terminal velocity in the magnetic eld, i.e.,eBvl ve
TTBl===
×
so = ms−06
06 1
1 1
.
.
Power dissipated across a conductor PV
R
=
2i.e., RV
P
=
2e resistance are in parallel combination so,
V 1 = V 2 = eSo, Re(^1) P
2
1
062
076
== = 047
(.)
.
. Ω
And, R e(^2) P
2
2
062
12
== = 03
(.)
.
. Ω.
- (b) :
di
dt= 10^3 A s–1? Induced emf across inductance, |e| = Ldi
dt
|e| = (5 × 10–3) (10^3 ) V = 5 V
Since , the current is decreasing , the polarity of this
emf would be so as to increase the existing current.
e circuit can be redrawn as shown in the gure.1 W 15V 5 mH BA I15VNow, VA – 5 + 15 + 5 = VB
? VA – VB = –15 V or VB – VA = 15 V- (d) : B =
μ 0 2
2 2232iR
()RX+ /B =μ 0 2
232232iR
()RR+ /=μ 0 2
24232iR
()R /=μμ 0 2
30
22 16iR
Ri
.. R=
φ = NBA cos 45° =^2
161
2
μ 0 i 2
Raφμ
=^0282ia
RA 1 W 15 V 5 mH BI