Problem 4. The switch of the Circuit shown is closed at time t = 0, and at time t = 0, i (0) = 3A & v(0) = 2V. = (t) = 8e-3t t = 0 452 -ww- 0.5F 2H {/i(1) 192 1Ω + v(t) (a) Derive the second order differential equation of i(t) over t for t≥ 0. (b) Find the natural response of i(t) for t ≥ 0. (c) What is the basic reason why the natural response goes to zero, as time goes to the Brief catalog of the Operational Amplifier circuits
Problem 4. The switch of the Circuit shown is closed at time t = 0, and at time t = 0, i (0) = 3A & v(0) = 2V. = (t) = 8e-3t t = 0 452 -ww- 0.5F 2H {/i(1) 192 1Ω + v(t) (a) Derive the second order differential equation of i(t) over t for t≥ 0. (b) Find the natural response of i(t) for t ≥ 0. (c) What is the basic reason why the natural response goes to zero, as time goes to the Brief catalog of the Operational Amplifier circuits
Introductory Circuit Analysis (13th Edition)
13th Edition
ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
Chapter1: Introduction
Section: Chapter Questions
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Transcribed Image Text:• Problem 4. The switch of the Circuit shown is closed at time t = 0,
and at time t = 0, i(0) = 3A & v(0) = 2V.
is(t) = 8e-3t
■
Vin m
R₁
U10-
(a) Derive the second order differential equation of i(t) over t for t≥ 0.
(b) Find the natural response of i(t) for t≥ 0.
(c) What is the basic reason why the natural response goes to zero, as time goes to the
Brief catalog of the Operational Amplifier circuits
(Based on the ideal operational amplifier)
R₁
U₂0-W
(a) Inverting amplifier
Vout=
R₂
ww
R₁
Rn
Xo
t = 0
ww
R₁
R₁ R₁
492
-ww-
U₂+
R₁
out=R₁ in
Ovout
0.5F
R₁
Rn
(d) Summing amplifier
Vin -
2H {\i(t) 10
R₁2
R₁
Vout
= (1 + R ₁₂)
(b) Noninverting amplifier
R₂K₁
U10-W
+ ART Juin
R₂K₂
U20-W
RJK3
V30-W
R₂/(1-(K₁ + K₂ + K3)):
R(K4-1)
v(t)
Vin
Rp.
(c) Voltage follower (buffer amplifier)
Ovout Vin
Ovout K4(K₁v1 + K₂v2 + K303)
(e) Noninverting summing amplifier

Transcribed Image Text:The complete response is the sum of the natural response and the forced response
X = Xn+Xf
Natural response of a first-order circuit
Natural response of a second-order circuit
CASE
Overdamped
Critically damped
Underdamped
az
S1 =
FORCING FUNCTION
K
Kt
K₁²
K sin cot
Ke at
Forced response of a first-order, or a second-order circuit
+ A₁
NATURAL FREQUENCIES
$1,52 = -α± √√² - 0²
$1,$₂=-α
S1, S2 = -x±j√√/0²-a² -α±jood
dx
dt
d²x
dt²
Solution of the Second-Order Differential Equation
d²x
x(t) = xn(t) + xf (t)
a2
dt²
+ a。x = f(t)
+ A1
dx
dt
"xn(t)" = Aest
Xn(t) = Ke-t/t
+ a。x = 0
-a₁ + √²-4a₂a0
242
-
Xn(t) = A₁e³₁ª + A₂e³₂t
ASSUMED RESPONSE
A
At + B
At² +Bt+C
A sin cot + B cos cot
Ae-at
NATURAL RESPONSE, Xn
Ale+Azer
(A₁+A₂t)e-at
(A, cos coat+A₂ sin coat)e
xn(t) = ?
(a₂s² + a₁s+ao) = 0
-α₁ - √²-4a₂a0
242
NATURAL RESPONSE, Xn
A₁ est + A₂e21
-α1
(A₁+A₂t)e
(A₁ cos wat+A₂ sin wat)ext
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