Solving Complex Algebra Homework w/ Equation & Solution

  • Thread starter Thread starter ChasW.
  • Start date Start date
  • Tags Tags
    Algebra Complex
Click For Summary
SUMMARY

The forum discussion centers on solving a complex algebra equation related to impedance matching in RF Circuit Design. The equation presented is {R_T+jX_T \over 1+jB_C(R_T+jX_T)}+jX_L = R_A-jX_A, with the book's solution for R_T being R_T=R_A(1-B_CX_T)+(X_A+X_L)B_CR_T. Participants discuss the process of separating real and imaginary components, emphasizing the importance of equating these parts to derive accurate solutions for R_T and X_T. The conversation highlights common pitfalls in handling complex numbers and the necessity of careful algebraic manipulation.

PREREQUISITES
  • Understanding of complex numbers and their properties
  • Familiarity with impedance matching concepts in RF Circuit Design
  • Proficiency in algebraic manipulation of equations
  • Knowledge of real and imaginary component separation techniques
NEXT STEPS
  • Study complex number equality and its implications in algebraic equations
  • Learn about impedance matching techniques in RF Circuit Design
  • Practice algebraic simplification of complex equations
  • Explore the use of software tools for solving complex algebra problems
USEFUL FOR

Electrical engineers, RF circuit designers, and students studying complex algebra and impedance matching techniques will benefit from this discussion.

ChasW.
Gold Member
Messages
18
Reaction score
0

Homework Statement



I am following along in a book which provides the equation below.
I have also included the book's stated solution.

Homework Equations



The Equation:
{R_T+jX_T \over 1+jB_C(R_T+jX_T)}+jX_L = R_A-jX_A
The Book's Solution:
R_T=R_A(1-B_CX_T)+(X_A+X_L)B_CR_T

The Attempt at a Solution



When attempting to solve for RT, so far I have:
{R_T+jX_T \over 1+jB_CR_T-B_CX_T} = R_A-jX_A-jX_L
R_T=(R_A-jX_A-jX_L)(1+jB_CR_T-B_CX_T)-jX_T
R_T=<br /> R_A+R_AjB_CR_T-R_AB_CX_T<br /> -jX_A+X_AB_CR_T+jX_AB_CX_T<br /> -jX_L+X_LB_CR_T+jX_LB_CX_T -jX_T
I then begin to simplify:
R_T=<br /> R_A(1+jB_CR_T-B_CX_T)<br /> +X_A(-j+B_CR_T+jB_CX_T)<br /> +X_L(-j+B_CR_T+jB_CX_T) -jX_T
R_T=<br /> R_A(1+jB_CR_T-B_CX_T)<br /> +(X_A+X_L)(-j+B_CR_T+jB_CX_T) -jX_T
I seem to be having some issue identifying further simplification.
Any assistance would be appreciated.
Charles
 
Physics news on Phys.org
Could you give more context? It appears that at some point only the real part was retained.
 
  • Like
Likes   Reactions: 1 person
DrClaude said:
Could you give more context? It appears that at some point only the real part was retained.

You are exactly correct. The greater context is a series of equations describing an impedance match using a series inductor and parallel capacitor from RF Circuit Design Theory and Applications where RT is the real part. The example starts off as expressing impedances as real and imaginary components and then separating the two: RT and XT.

The book's stated XT solution is:
X_T=R_TR_AB_C-(1-B_CX_T)(X_A+X_L)
Perhaps my confusion resides with solving for the real-only part. If all that was done was discarding the imaginary parts in the RT equation, then I might be ok.

My reason for wanting to clearly understand the equation and its transformations is to be able to perform the same approach but as applied to other topologies such as series capacitor and parallel inductor.

The way the equations RT and XT are used is described as:
In the RT equation, solve for XL and substitute those results into the XT equation, solve the remaining quadratic equation (plus side version) to obtain BC and then substitute BC into linear XT equation to solve for XL.
 
Last edited:
You need to equate the real and imaginary parts of the complex equation separately.
I mean the real left-hand side equals the real right-hand side and same for the imaginary (if needed).
You can do some simplifications first, as you did. But in the end equate the two parts separately.
 
  • Like
Likes   Reactions: 1 person
nasu said:
You need to equate the real and imaginary parts of the complex equation separately.
I mean the real left-hand side equals the real right-hand side and same for the imaginary (if needed).
You can do some simplifications first, as you did. But in the end equate the two parts separately.
Ok so after the simplifications that I did, does equating to the real part simply mean to drop all of the remaining imaginary components to arrive at the form of RT that the book author did? Or perhaps to reword my question, does taking the real part of RT at the point where I simplified to, mean discarding all remaining imaginary values? I guess what I was expecting was some mathematical step beyond my final simplification or more methodical means for taking the real part of the lengthy expression.
 
It's not really "discarding". You just use the general meaning of two complex numbers being equal.
If you have z1=a1+b1*i and z2=a2+b2*i (where a1,a2,b1,b2 are pure real), the equality z1=z2 implies
a1=a2
and
b1=b2.

Here z1 and z2 are the two sides of your equation.
 
nasu said:
It's not really "discarding". You just use the general meaning of two complex numbers being equal.
If you have z1=a1+b1*i and z2=a2+b2*i (where a1,a2,b1,b2 are pure real), the equality z1=z2 implies
a1=a2
and
b1=b2.

Here z1 and z2 are the two sides of your equation.
Ok I get the basic example you've given as it demonstrates the equality of the real and imaginary parts of two different complex numbers given z1=z2. I am still working towards properly applying that to the separation of the real and imaginary components in the larger expressions.

So for separating out the imaginary side which the book states to be:
X_T=R_TR_AB_C-(1-B_CX_T)(X_A+X_L)
which comes from:
{R_T+jX_T \over 1+jB_C(R_T+jX_T)}+jX_L = R_A-jX_A
I can take it as far as:
{R_T+jX_T \over 1+jB_CR_T-B_CX_T} = R_A-jX_A-jX_L
jX_T=(R_A-jX_A-jX_L)(1+jB_CR_T-B_CX_T)-R_T
jX_T=R_A+R_AjB_CR_T-R_AB_CX_T<br /> -jX_A+X_AB_CR_T+jX_AB_CX_T<br /> -jX_L+X_LB_CR_T+jX_LB_CX_T-R_T
jX_T=R_A(1+jB_CR_T-B_CX_T)+X_A(-j+B_CR_T+jB_CX_T)+X_L(-j+B_CR_T+jB_CX_T)-R_T
jX_T=R_A(1+jB_CR_T-B_CX_T)+(X_A+X_L)(-j+B_CR_T+jB_CX_T)-R_T
What is the next step towards separating out XT?
 
You need to work more on the right side.
Collect all the terms with j. This will be the imaginary part of the left hand side. (Im)
Collect all terms without j. This will be the real part. (Re)

The way you wrote it so far, you have only imaginary part on the left side.
So after you do the above, you will have
XT=Im
and
0=Re.

Solve the two equations for whatever you want to find.
 
nasu said:
You need to work more on the right side.
Collect all the terms with j. This will be the imaginary part of the left hand side. (Im)
Collect all terms without j. This will be the real part. (Re)

The way you wrote it so far, you have only imaginary part on the left side.
So after you do the above, you will have
XT=Im
and
0=Re.

Solve the two equations for whatever you want to find.

When I solve for XT I get:
X_T={R_T+jX_T \over R_A(-jB_C^2R_T)+(X_A+X_L)(jB_C-B_C^2R_T)}
which doesn't seem to be much better than the last attempt.
Perhaps you would be willing to show me the transformation to XT=Im as you have described?
 
  • #10
ChasW. said:
When I solve for XT I get:
X_T={R_T+jX_T \over R_A(-jB_C^2R_T)+(X_A+X_L)(jB_C-B_C^2R_T)}
You're mixing real and imaginary again.

Consider
$$
\begin{align}
\frac{A + j B}{C + j D} &= F + jG \\
A + j B &= (C + j D)(F + jG) \\
A + j B &= CF + j CG + j DF - DG \\
A + j B &= (CF - DG) + j (CG + DF)
\end{align}
$$
Look at that last line. It means that ##A = CF - DG## and ##B = CG + DF##. You need to do something similar with your equation.
 
  • Like
Likes   Reactions: 1 person
  • #11
DrClaude said:
You're mixing real and imaginary again.

Consider
$$
\begin{align}
\frac{A + j B}{C + j D} &= F + jG \\
A + j B &= (C + j D)(F + jG) \\
A + j B &= CF + j CG + j DF - DG \\
A + j B &= (CF - DG) + j (CG + DF)
\end{align}
$$
Look at that last line. It means that ##A = CF - DG## and ##B = CG + DF##. You need to do something similar with your equation.
I think this helped.

Starting from
R_T+jX_T=R_A(1+jB_CR_T-B_CX_T)+(X_A+X_L)(-j+B_CR_T+jB_CX_T)
Using what you've provided I can see that
R_T=R_A(1-B_CX_T)+(X_A+X_L)(B_CR_T)
which also brings me closer with XT
X_T=R_AB_CR_T+(X_A+X_L)(-1+B_CX_T)
If I can just find the sign error now. For XT, the book has
X_T=R_TR_AB_C-(1-B_CX_T)(X_A+X_L)
... or is that actually not an error, but rather adding the opposite? Mental fatigue has bested me :)

Thank you both.
Charles
 
Last edited:
  • #12
ChasW. said:
X_T=R_AB_CR_T+(X_A+X_L)(-1+B_CX_T)
If I can just find the sign error now. For XT, the book has
X_T=R_TR_AB_C-(1-B_CX_T)(X_A+X_L)
... or is that actually not an error, but rather adding the opposite? Mental fatigue has bested me :)
When your brain has rested, I'm sure you'll see that
(-1+B_CX_T) (X_A+X_L) = -(1-B_CX_T) (X_A+X_L)
 
  • Like
Likes   Reactions: 1 person
  • #13
It's not an error. They are the same.
Take the "-" outside the parenthesis and you get the result in the book.
 
  • Like
Likes   Reactions: 1 person
  • #14
Sounds right
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
8
Views
2K
Replies
6
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K