Solutions for Tutorial-7
Q 1. Solution:
(a) For positive pulse of vi :
The diode would be ON and vo = 2V + 0.7 V = 1.3 V
The capacitor charges to 10 V + 2 V 0.7 V = 11.3 V
For negative pulse of vi :
The diode would be OFF and vo = 10 V 11.3 V = 21.3 V
(b) In the positive swing of applied voltage, the diode gets short-circuited being forward
biased. Thus the charging time constant would be almost zero.
In the negative swing of applied voltage, the diode gets open-circuited being reverse
bias. Thus the discharging time constant is = RC = (56 k)(0.1F) = 5.6 ms
In positive cycle, the very low time constant ensures that the capacitor gets charged
quickly to the applied voltage and also keeps the diode ON. As the diode is assumed to
have only fixed voltage drop with no resistance, the output voltage remains constant.
For the negative cycle, note that the half period of the applied signal happens to much
smaller than the effective time constant .
T=
1
T
= 1 ms,
= 0.5 ms << = 5.6 ms
f
2
So the capacitor does not get enough time to discharge appreciably before the input
signal switches its polarity, thus the output voltage remains unchanged.
Q2. Solution:
(a) I E =
I
VE
2.1 V
3.09 mA
=
= 3.09 mA , assuming I C I E , = C =
= 154.5
RE 0.68 k
IB
20 A
(b) VCC = VR + VCE + VE = (2.7 k )(3.09 mA ) + 7.3 V + 2.1 V = 17.74 V
C
(c) R B =
VR
IB
VCC VBE VE 17.74 V 0.7 V 2.1 V 14.94 V
=
=
= 747 k
IB
20 A
20 A
Q3. Solution:
c
c
a
NI
(a)
Figure 1(a)
+
Magnetic equivalent circuits for Q1
NI
eq
The equivalent magnetic circuit can be drawn as shown in the figures.
a)
(b)
The reluctances are computed as follows:
2
For the center core:
For the right/left path:
5 10
H-1 = 0.332 105
7
4
2400 4 10 5 10
15 102
H-1 = 0.995 105
a = b =
2400 4 107 5 10 4
c =
H-1
H-1
eq = c + (a // b) = 0.8295 105 H-1
Therefore, Inductance
Since Bmax is 2T,
L = N2/eq = 4002/(0.995105) = 1.93 H
max = 2510-4 = NImax/eq
Imax = 2510-40.8295 105/400 =0.207 A
Wf = (1/2) Imax2L = 0.50.20721.93 = 0.041 J
b)With the airgaps,
g =
0.5 10 2
= 79.577 105 H 1
4 107 5 104
0.5
0.
For the center core:
c =
-1
5 102
= 0.332 105 H
7
4
2400 4 10 5 10
Figure 1(b)
For the left/right path: a = b =
0.5 102
14.5 102
H-1 = 80.54 105 H-1
+
7
4
4 10 5 10
2400 4 107 5 10 4
eq = c + (a // b) = 40.602 105 H-1
L = N2/eq = 4002/(40.602 105) = 0.0394 H
Maximum B occurs in the central limb,
max=BmaxA = 2510-4 = NImax/eq
Imax = 2510-440.602 105/400 =10.15 A
Wf = (1/2) Imax2L = 0.510.1520.0394 = 2.03 J
Flux in the air gap = (1/2) max= (1/2)2510-4 = 510-4Wb
Energy stored in the two air gaps
Wg= 2(1/2)gmax2g = [(510-4]279.577105 = 1.989 J
Q4. Solution:
Let the two operating conditions be specified by
V1,f1, Bm1andV2, f2, Bm2
Then,
V1 = Kf1Bm1,
and
f2Bm2/f1Bm1 = V2/V1
For hysteresis loss, Ph1 = KhBm11.6f1,
V2 = Kf2Bm2,
Bm2 = (V2 /V1) (f1 / f2) Bm1 = (220/110) (60/50) 0.8 = 1.92 T
Ph2 = KhBm21.6f2
Ph2 = (Bm2/Bm1)1.6 (f2/f1) Ph1 = (1.92/0.8)1.6 (50/60) 200 = 676.4 W