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ELG4135 − Final 2004 / ELG4535 − final 2004
This document is the solution to the
ELG4135 final 2004.
Ce document est la solution à l'examen
final ELG4535 2004.
- Q1
-
Using these values:
Gain = ( 6V − Vofs ) / ( 2V − Vofs )
Gain = ( 1V − Vofs ) / ( 1.9V − Vofs )
Thus:
( 6V − Vofs ) / ( 2V − Vofs ) =
( 1V − Vofs ) / ( 1.9V − Vofs )
( 6V − Vofs ) × ( 1.9V − Vofs ) =
( 1V − Vofs ) × ( 2V − Vofs )
11.4V² −(7.9V)Vofs + Vofs² =
2V² − (3V) Vofs + Vofs²
9.4V² = (4.9V) Vofs
Vofs = 9.4V²/4.9V = 1.92V
Gain = ( 6V − 1.92V ) / ( 2V − 1.92V )
= 50
-
(1 + R23/(R22||R21) ) = Gain = 50
500k/(50−1) = 10.2k = R22||R21
9V×R21/(R21+R22) = 1.92V
R21 = 1.92V/9V × (R21+R22) = 0.21 × (R21+R22)
R21 = 0.21 / (1−0.21) R22 = 0.27 R22
Thus,
10.2k = 1/( 1/R22 + 1/(.27 R22) )
R22/10.2k = (1 + 1/.27) = 4.69
R22= 4.69×10.2k = 47.8k
R21= 0.27×R22 = 12.9k
-
3dB point for op amp gain is fT/ GFBN.
Freq = 2.0MHz / (1 + 50) = = 39 kHz
-
Neglect V− since IB=0.
V+ of inner ideal op-amp is
2V − 50n×500k = 1.995V
→Approach #1
Vo2 = (1.995V - 1.92V)×50 + 1.92 = 5.75V
→Approach #2 Vo2 = 6V for Vi2 = 2V.
Thus Vo2 = 6V + (−0.005V)×50 = 5.75V
- Q2
- The Schmitt trigger comparator is better in
a case where there is significant noise. Because it
has two thresholds, it will only trigger once for
a noise level below the difference in thresholds.
- Q3
-
VT = 9V×20k/(20k+20k) = 4.5V
-
V+ begins at 4.5V. After Vo4
makes a transition from 8V to 1V,
V+ = 4.5V − (8V − 1V) = −2.5V;
V+ then returns to 4.5V as an exponential
with time constant (τ) = 100n×(20k||20k) = 1ms
-
At t=0, V+ = 4.5V;
Vi4 < V+, so Vo4 = L+.
All signals are constant until t=10ms
At t=10ms, Vi4 > V+;
Vo4 switches to L−.
V+ changes by L+−L−,
thus immediately after t=10ms,
V+= 4.5 − (8V−1V) = −2.5V.
V+ then exponentially recovers to 4.5V.
At that point V−=0V.
When V+ > V−,
Vo4 returns to L+.
-
At t=10ms,
transition of Vo4 to L−
Calculate transition time of Vo4 to L+:
T= τ ln (
(Vt=∞ − Vt=0) /
(Vt=∞ − Vt=T) )
T= 1ms × ln( (4.5V−( −2.5V) )
(4.5V−0V) ) = 0.44 ms
At t=10.44ms,
transition of Vo4 to L+
- Q4
-
ε = √(10Amax/10−1) = 0.35
A(ω) = 40dB = 10 log( 1 +
0.35²(ω/ωp)2N )
(f/fp)2×3 =
(1040/10−1)/(.35²) = 8.2×104
(f/fp)=
( 8.2×104 )1/6
= 6.59
fs = fp×6.59 = 65.9Hz
-
(s − p1)(s − p2)
= s² + (ω0/Q)s
+ ω0²
= (s + 2π (2+j9)(s + 2π (2−j9)
= s² + 25.1s + 3356
ω0 = √(3356) = 57.9 rad/s
Q = ω0/25.1 = 2.31
-
Low pass RLC filter has T(s) =
1/LC / ( s² + s/CR + 1/LC )
1/CR = 25.1
C= 1/100Ω/25.1 = 0.4mF
1/LC = 3356
L= 1/0.4mF/3356 = 0.75H
-
It would be cheaper to build an active filter. The
values of 0.75H and 0.4mF are very large and
expensive compared to a component such as
an Antoniou inductor replacement.
- Q5
-
VBE,Q62 = ILR61
R61 = 0.6V / 10mA = 60Ω
-
→Approach #1:
When Vi6 is large, then VE,Q61
= 9V - VCE,sat = 8.8V
8.8V = (R61 + RL)×10mA
RL= 8.8V / 10mA − 60Ω = 820 Ω
→Approach #2:
Maximum Vi6 is from Monostable is L+ = 8V.
Thus VE,61= 8V - 0.6V = 7.4V
7.4V = (R61 + RL)×10mA
RL= 7.4V / 10mA − 60Ω = 680 Ω
Last Updated:
$Date: 2005-01-03 13:44:28 -0500 (Mon, 03 Jan 2005) $
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