Theory: Consider an RLC circuit shown below consisting of an inductor with an inductance of L henry (H), a resistor with a resistance of R ohms (12), and a capacitor with a capacitance of C farads (F) driven by a voltage of E(t) volts (V). Given the voltage drop across the resistor is ER= RI, across the inductor is ELL(dI/dt), and across the capacitor is E= Kirchhoff's Law gives 9 C с 1 L +RI +9=E(t) dl dt dq If we differentiate this equation with respect to time and substitute I = a second-order differential equation dt L d²1 dl +R dt² 71 = dt C + dE dt 1 Problem: Now suppose an RLC circuit with a 2 resistor, a 25F capacitor is driven by the voltage E(t) = 0.1t² V. 25 1 100 we obtain Hinductor, and a = D² I and dl dt d² I i. Using differential operator notation, = DI, write the dt² differential equation associated with this circuit in terms of current I, differential operator D, and time t. ii. Find the roots of the auxiliary polynomial of the corresponding homogeneous equation of I. Enter the roots as a list separated by commas. 71, 72= iii. Find the general solution of the corresponding homogeneous equation (complementary solution) for I. Use A and B for the arbitrary constants. In. (t) = iv. Find a particular solution for I. Where needed, round off all your values to at least five decimal places. 1,(t)= v. Find the general solution for I in terms of t and arbitrary contastands A and B. I(t)=

Introductory Circuit Analysis (13th Edition)
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ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
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Theory: Consider an RLC circuit shown below consisting of an inductor with an
inductance of L henry (H), a resistor with a resistance of R ohms (12), and a capacitor
with a capacitance of C farads (F) driven by a voltage of E(t) volts (V).
E
R
ww
Given the voltage drop across the resistor is ER
EL=L(dI/dt), and across the capacitor is E.
=
L
с
L +RI +9=E(t)
dI
dt
d²I
dt²
dq
dt
If we differentiate this equation with respect to time and substitute I = we obtain
a second-order differential equation
RI, across the inductor is
9
Kirchhoff's Law gives
C
dl
+R
dt
+ I=
dE
dt
1
Problem: Now suppose an RLC circuit with a 2 resistor, a
25
25F capacitor is driven by the voltage E(t) = 0.1t² V.
1
100
H inductor, and a
= D² I and
d² I
dI
i. Using differential operator notation,
DI, write the
dt²
dt
differential equation associated with this circuit in terms of current I, differential
operator D. and time t.
ii. Find the roots of the auxiliary polynomial of the corresponding homogeneous
equation of I.
Enter the roots as a list separated by commas.
71, 72=
iii. Find the general solution of the corresponding homogeneous equation
(complementary solution) for I.
Use A and B for the arbitrary constants.
In. (t)=
iv. Find a particular solution for I.
Where needed, round off all your values to at least five decimal places.
I, (t)
v. Find the general solution for I in terms of t and arbitrary contastands A and B.
I(t)=
Transcribed Image Text:Theory: Consider an RLC circuit shown below consisting of an inductor with an inductance of L henry (H), a resistor with a resistance of R ohms (12), and a capacitor with a capacitance of C farads (F) driven by a voltage of E(t) volts (V). E R ww Given the voltage drop across the resistor is ER EL=L(dI/dt), and across the capacitor is E. = L с L +RI +9=E(t) dI dt d²I dt² dq dt If we differentiate this equation with respect to time and substitute I = we obtain a second-order differential equation RI, across the inductor is 9 Kirchhoff's Law gives C dl +R dt + I= dE dt 1 Problem: Now suppose an RLC circuit with a 2 resistor, a 25 25F capacitor is driven by the voltage E(t) = 0.1t² V. 1 100 H inductor, and a = D² I and d² I dI i. Using differential operator notation, DI, write the dt² dt differential equation associated with this circuit in terms of current I, differential operator D. and time t. ii. Find the roots of the auxiliary polynomial of the corresponding homogeneous equation of I. Enter the roots as a list separated by commas. 71, 72= iii. Find the general solution of the corresponding homogeneous equation (complementary solution) for I. Use A and B for the arbitrary constants. In. (t)= iv. Find a particular solution for I. Where needed, round off all your values to at least five decimal places. I, (t) v. Find the general solution for I in terms of t and arbitrary contastands A and B. I(t)=
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