Natural response of a RLC underdamped circuit?

In summary, the book writes that because the constants A1 and A2 are arbitrary, we substitute (A1+A2) and j(A1-A2) with new constants B1 and B2. These constants must be complex conjugates, which means that B1 and B2 must be real numbers. However, because the imaginary portion of the equation is just replaced with a real number, the math becomes vn=e−αt(B1cos(ωdt)+B2sin(ωdt)). Substituting this real number for the imaginary one in the equation results in the natural response v_{n} = e^{-\alpha t}(B_{1}cos(\omega_{d
  • #1
silentwf
37
0
Not really sure whether this question belongs here or not (if it doesn't, help move?).
So I was reading my electronic circuits textbook and am at the section of underdamped RLC unforced response, and the book mentions the natural response as
[itex]v_{n} = e^{-\alpha\cdot t}(A_{1}\cdot e^{j\omega_{d}t}+A_{2}e^{-j\omega_{d}t})[/itex]
And then after expanding the equation via Euler's formula, the textbook writes
[itex]v_{n} = e^{-\alpha t}((A_{1}+A_{2})cos(\omega_{d}t)+j(A_{1}-A_{2})sin(\omega_{d}t))[/itex]
The two steps above i understand, however, the book then writes "Because the unknown constants A1 and A2 remain arbitrary, we replace (A1+A2) and j(A1-A2) with new arbitrary (yet unknown) constants B1 and B2. A1 and A2 must be complex conjugates so that B1 and B2 are real numbers, Therefore, [the above equation] becomes
[itex]v_{n} = e^{-\alpha t}(B_{1}cos(\omega_{d}t)+B_{2}sin(\omega_{d}t))[/itex]"

This is where I don't understand. Why (or how) can the imaginary portion of the equation be simply substituted for a real number?

(Book I'm using: Introduction to Electronic Circuits 8th edition (International Student Version), by Richard C. Dorf, James A. Svoboda Page 380)
 
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  • #2
There's a missing j on the sin(). B2 can be real but the sun and cos terms must differ by a factor of j one way or another.
 
  • #3
silentwf said:
Not really sure whether this question belongs here or not (if it doesn't, help move?).
So I was reading my electronic circuits textbook and am at the section of underdamped RLC unforced response, and the book mentions the natural response as
[itex]v_{n} = e^{-\alpha t}(A_{1} e^{j\omega_{d}t}+A_{2}e^{-j\omega_{d}t})[/itex]

The math is often written like that, but you need to remember that physically it means
[itex]v_{n} = \Re\left[e^{-\alpha t}(A_{1} e^{j\omega_{d}t}+A_{2}e^{-j\omega_{d}t})\right][/itex] where [itex]\Re[/itex] mean "the real part of".

the book then writes "Because the unknown constants A1 and A2 remain arbitrary, we replace (A1+A2) and j(A1-A2) with new arbitrary (yet unknown) constants B1 and B2. A1 and A2 must be complex conjugates so that B1 and B2 are real numbers.
...
This is where I don't understand.

To be honest, I don't understand that "explanation" either, and I don't know why the book thinks [itex]A_1[/itex] and [itex]A_2[/itex] are complex conjugates. It doesn't matter if they are or not.

If you multiply out the real and imaginary parts of
[itex]A_{1} e^{j\omega_{d}t}+A_{2}e^{-j\omega_{d}t}[/itex],
where [itex]A_1[/itex] and [itex]A_2[/itex] are complex, and using [itex]e^{jz} = \cos z + j \sin z[/itex],
you will see that it the real part is of the form [itex]B_1 \cos \omega_d t + B_2 \sin \omega_d t[/itex] where [itex]B_1[/itex] and [itex]B_2[/itex] are real constants.

(I think Antiphon is wrong about the missing j.)
 
  • #4
vn=e−αt((A1+A2)cos(ωdt)+j(A1−A2)sin(ωdt))
The two steps above i understand, however, the book then writes "Because the unknown constants A1 and A2 remain arbitrary, we replace (A1+A2) and j(A1-A2) with new arbitrary (yet unknown) constants B1 and B2. A1 and A2 must be complex conjugates so that B1 and B2 are real numbers, Therefore, [the above equation] becomes
vn=e−αt(B1cos(ωdt)+B2sin(ωdt))"

i think it's a simple algebraic manipulation...
Dorf's controls book was known (among us struggling undergrads anyway) for brushing by details when i took that course in 1968... present day reviews of it on 'net say same thing.

let's see here

what Dorf says we need is two real numbers B1 and B2
such that:
B1 = A1 + A2
and :
B2 = j(A1-A2)

okay

so
B1 = A1 + A2
and
B2/j = A1 - A2

add the two above eq's and get
B1 + B2/j = 2A1;
or A1 = (B1 +B2/j) /2;;;

subtract them and get
B1 - B2/j = 2A2
or A2 = (B1 - B2/j)/2

now multiply B2/j term in both those eq's by j/j , giving jB2/j^2, and change the resulting j^2's underneath B2 to minus one's which just flips sign of jB2

now you have
A1 = (B1 - jB2)/2
A2 = (B1 + jB2)/2

observe A1 and A2 are complex conjugates so Dorf is happy
and i suppose B could be real
but I'm not smart enough to know if that's the answer.

could it be that simple? would any old integer work?

probably that's what Aleph was saying...

old jim
 
Last edited:
  • #5
Thanks for the replies,
I asked a friend too, and he said it was just simple algebraic manipulation, so jim_hardy would be correct.

I really did wish that the authors explain these things more clearly.
 

Related to Natural response of a RLC underdamped circuit?

1. What is the definition of a RLC underdamped circuit?

A RLC underdamped circuit is an electrical circuit that contains a resistor (R), inductor (L), and capacitor (C) in a series or parallel configuration. It is considered underdamped when the circuit's natural response displays oscillations before reaching a steady state.

2. How does an underdamped circuit differ from overdamped and critically damped circuits?

An underdamped circuit differs from overdamped and critically damped circuits in that it displays oscillations in its natural response. In contrast, an overdamped circuit has a slow natural response without oscillation, and a critically damped circuit has a fast natural response without oscillation.

3. What is the time constant of an underdamped circuit?

The time constant, denoted by the symbol τ, is a measure of how quickly the natural response of an underdamped circuit decays to zero. It is calculated by taking the reciprocal of the damping coefficient (ζ) multiplied by the angular frequency (ω) of the circuit, or τ = 1/(ζω).

4. How do you calculate the damping ratio of an underdamped circuit?

The damping ratio, denoted by the symbol ζ, is a measure of the rate at which the oscillations in the natural response of an underdamped circuit decay. It is calculated by dividing the resistance (R) of the circuit by two times the square root of the inductance (L) divided by the capacitance (C), or ζ = R/[2√(L/C)].

5. How does the initial conditions of a circuit affect its natural response?

The initial conditions, such as the initial voltage and current in the circuit, can affect the amplitude and phase of the natural response in an underdamped circuit. These initial conditions are taken into account when solving for the natural response using the circuit's differential equation.

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