Determining total impedance, Voltage V2 and current IL of circuit

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Discussion Overview

The discussion revolves around determining the total impedance (ZT), voltage (V2), and current (IL) in a given electrical circuit. Participants explore calculations related to parallel branch impedances, addressing both theoretical and practical aspects of circuit analysis.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a method for calculating total impedance in parallel branches but expresses uncertainty about the results, particularly regarding the angle of the impedance.
  • Several participants challenge the calculations, noting that the combined impedance of purely reactive components should yield a purely imaginary result, questioning the correctness of the initial results.
  • There is a discussion about the arithmetic involved in combining reactive components, with some participants suggesting that the angle should be +90° or -90° depending on the position on the imaginary axis.
  • Another participant proposes using rectangular form for complex values to simplify calculations, while others request clarification on the calculations being performed.
  • One participant attempts to clarify their calculations for the first parallel branch, expressing their results in terms of rectangular coordinates and arriving at a purely imaginary impedance.
  • A new problem regarding Thevenin's equivalent circuit is introduced, with a participant expressing difficulty in finding the Thevenin resistance and receiving guidance to start a new thread for that topic.
  • There is a question about whether V2 equals the source voltage E, with participants discussing the relationship between V2 and the current source in the circuit.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the calculations for the total impedance, as multiple viewpoints and corrections are presented. The discussion remains unresolved regarding the accuracy of the initial impedance calculations and the implications for V2 and IL.

Contextual Notes

Some calculations depend on the correct interpretation of reactive components and their angles. There are unresolved mathematical steps and assumptions regarding the configuration of the circuit elements.

johnsy1312
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I am asked to find the total impendance ZT, voltage V2 and IL for the circuit attached

I am not sure if i am correct, but this is how i approached this problem:

So i first found the total impendance in the first parallel branch and then the second
Z=\frac{1}{\frac{1}{4<-90^o}+\frac{1}{6<90^o}}=2.4<0^o

Then i found impendance for 2nd parallel branch:
Z=\frac{1}{\frac{1}{6.8&lt;0^o}+\frac{1}{6.8&lt;0^o}+\frac{1}{8&lt;90^o}}=8.69<66.97^o

So, ZT= 8.69&lt;66.97^o+2&lt;0^o+2.4&lt;0^o = 13.09&lt;66.97^o

Finding V2: Knowing I=4mA&lt;0^o, Z_T=13.09&lt;66.97^o

E=4&lt;0^o*13.09&lt;66.97^o=52.36V&lt;66.97^o

Therefore V_2=52.36V&lt;66.97^o

Finding I_L
I_L = \frac{V_L}{Z_L}=\frac{52.36&lt;66.97^o}{8&lt;90^o}=5.76&lt;23.03^o mA
 

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Redo your calculations for the parallel branch impedances. The formulas look good but your results do not look right. For example, for the first parallel group you have two purely reactive components (inductor and capacitor) in parallel. The resulting combined impedance should be purely imaginary, yet you've come up with purely real result (angle 0°). So something's going awry with your calculations.
 
gneill said:
Redo your calculations for the parallel branch impedances. The formulas look good but your results do not look right. For example, for the first parallel group you have two purely reactive components (inductor and capacitor) in parallel. The resulting combined impedance should be purely imaginary, yet you've come up with purely real result (angle 0°). So something's going awry with your calculations.

When you add the two reactive components together, the angle becomes 90, since the inductor is 6kohm<90 and capacitor is 4kohm<-90?
 
johnsy1312 said:
When you add the two reactive components together, the angle becomes 90, since the inductor is 6kohm<90 and capacitor is 4kohm<-90?

Are you asking, concluding, or guessing? Why not show your calculation steps?

For the first parallel combination both components are reactive (so their impedances have only imaginary components). Carrying out the arithmetic should be fairly straightforward.
 
gneill said:
Are you asking, concluding, or guessing? Why not show your calculation steps?

For the first parallel combination both components are reactive (so their impedances have only imaginary components). Carrying out the arithmetic should be fairly straightforward.

So with what your saying would the total impedance for the first branch be Z=(6-4)j, how do we obtain an angle from that when they are both on the same axis? Isn't the angle between them 0?
 
johnsy1312 said:
So with what your saying would the total impedance for the first branch be Z=(6-4)j, how do we obtain an angle from that when they are both on the same axis? Isn't the angle between them 0?

You had the right formula for parallel impedance in your first post. Just plug in the rectangular form of the impedances for the two components and carry through the math to arrive at a single value.

Note that the angle is specified with respect to the positive real axis. If the result lies along the imaginary axis then the angle must be either +90° or -90°.
 
gneill said:
You had the right formula for parallel impedance in your first post.

So Z=\frac{1}{\frac{1}{6kohm&lt;90^o}+\frac{1}{4kohm&lt;-90^o}}?
 
johnsy1312 said:
So Z=\frac{1}{\frac{1}{6kohm&lt;90^o}+\frac{1}{4kohm&lt;-90^o}}?

Sure. Do the math. You might find that using rectangular form for the complex values will be convenient.
 
z=\frac{12}{(2+3)j}<br /> =12*(\frac{1}{(2+3)j})
 
  • #10
johnsy1312 said:
z=\frac{12}{(2+3)j}<br /> =12*(\frac{1}{(2+3)j})

Can you explain what the above is all about? The numbers don't seem to correspond to any given in the problem statement. What are you calculating?
 
  • #11
Disregard previous post:

Correct me if i am wrong.

6kohm&lt;90^o=(6sin(90^o)+6cos(90^o))j<br /> =6j
4kohm&lt;-90^o=(4sin(-90^o)+4cos(-90^o))j<br /> =-4j

Therefore:

Z= \frac{1}{\frac{1}{6j}-\frac{1}{4j}}<br /> =-12j
 
Last edited:
  • #12
johnsy1312 said:
Disregard previous post:

Correct me if i am wrong.

6kohm&lt;90^o=(6sin(90^o)+6cos(90^o))j<br /> =6j
4kohm&lt;-90^o=(4sin(-90^o)+4cos(-90^o))j<br /> =-4j

Therefore:

Z= \frac{1}{\frac{1}{6j}-\frac{1}{4j}}<br /> =-12j

That's better! Note that the units of the result are kΩ.

Can you do the same for the second parallel grouping?
 
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  • #13
Thanks!

I also have this other problem which i cannot see to get right and i have attempted it 100 times :/

I have to determine the Thevenin's equivalent circuit for the circuit attached.
I am stuck on the first and essential part, finding the thevenin's resistance.

Answer should be 10ohms, my attempt:

R_2||4 = \frac{5*16}{5+16} = 3.81ohms

R_1,3,5 = 20 + 12 + 2 = 34ohms

R_th= \frac{34*3.81}{3.81+34} = 3.42ohms
 

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  • #14
You should start a new thread for a new problem. Please do so.

One hint: R2 and R4 are not in parallel.
 
  • #15
I did :)
They look like they are in parallel though :/
 
  • #16
For this circuit, does V2=E?
 
  • #17
johnsy1312 said:
For this circuit, does V2=E?

In general I won't confirm or refute unsubstantiated guesses. What logic lead you to your conclusion?
 
  • #18
The parallel the branch that V2 is on seems like it is parallel to the origin source, otherwise called the current source in this case.
 
  • #19
johnsy123 said:
The parallel the branch that V2 is on seems like it is parallel to the origin source, otherwise called the current source in this case.

Sketch the "reduced" circuit, replacing the simplified parallel combinations with boxes and label them with their reduced impedances. How does the circuit look? Where does V2 appear?
 

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