Problems about Zin in complex circuit analysis

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e0ne199
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1. Homework Statement

scr1.png

the problem is my answer for question (a) is not the same as the answer provided by the question, i get 2.81 - j4.49 Ω while the answer demands 2.81 + j4.49 Ω

Homework Equations


simplifying the circuit, details can be seen below

The Attempt at a Solution


XL1=jωL1=j*20e-3*1000=j20Ω
XL2=jωL2=j*5e-3*1000=j5Ω
XC1=1/(-jωC1)=1/(j*100e-6*1000)=-j10Ω
XC2=1/(-jωC2)=1/(j*200e-6*1000)=-j5Ω

solving Zpar1:
Zpar1 = XL1 * XC1 /(XL1 + XC1)
Zpar1 = -j10Ω * j20Ω /(-j10Ω + j20Ω) = -j20Ω

solving Zser1:
Zser1 = -j20Ω - j5Ω = -j25Ω

solving Zin:
Zin = 1/((1/10)+(1/(j5))-(1/(j25))) = 2.81 - j4.49 Ω
 

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e0ne199 said:
Zin = 1/((1/10)+(1/(j5))-(1/(j25))) = 2.81 - j4.49 Ω
I believe that you are making some arithmetical mistake in evaluating the above expression. When I type the same thing into Mathcad I see:

upload_2018-11-26_14-58-24.png
 

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gneill said:
I believe that you are making some arithmetical mistake in evaluating the above expression. When I type the same thing into Mathcad I see:

View attachment 234677
i don't know if mathcad can give result like that because i calculated using ti-89 emulator and got result like what i posted above... you can see the screenshot on my attachmet
Screenshot_20181127-103405.jpeg
 

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does the use of i or j symbol affect the calculation?
 
What you've just shown me is :

upload_2018-11-26_21-45-9.png


Not the same.
 

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gneill said:
What you've just shown me is :

View attachment 234700

Not the same.
ok i think i have the solution... i did not input the equation into my calculator properly, i have achieved the same result after adding more bracket symbol into my equation... thanks for the guidance
 
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The answers provided for questions (a) and (b) in problem 10.9 are easily arrived at, however the answer given for question (c) doesn't make sense to me. Can someone clarify?
 
The part (c) result matches what I came up with.

You have a delta configuration to start, with the capacitance from a to b across the top.
The left leg of the delta is an L-R combination. The right leg is an L-C combo.

For the L-R combo, I got a value of 2 + j4. For the L-C combo, I got a value of -j20.

Keep in mind that the L-R part and the L-C part are in series with each other and this series (L-R + L-C) is in parallel with the capacitance.

As I said, the results agree with what is shown for part (c).
 
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I confirm the answer for (c). I took the 10Ω resistor in parallel with the j5Ω inductor as Zleft. Then took -j10Ω cap in parallel with the j20Ω inductor as Zright.
Then Zleft in series with Zright.
Then that result in parallel with the -j5Ω cap.
 
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upload_2019-1-25_19-2-38.png
 

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All the required impedances can be obtained in one go using a little linear algebra. Choose the bottom node (g) of the circuit to be the reference node. Label the other two nodes 1 and 2.

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Write the admittance matrix (Y) by inspection.
Invert the Y matrix to obtain the impedance (Z) matrix. Two of the elements of the Z matrix are directly the impedances Z(ag) (shown in red) and Z(bg) (shown in magenta). The impedance Z(ab) is the sum of Z(ag) and Z(bg) minus the two transfer impedances:

GetZ.png
 

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By the way, it is easier-in my opinion-to use Excel complex:
Define Name:
ZR=COMPLEX(10,0)
ZLa=COMPLEX(0,5)
ZLb=COMPLEX(0,20)
ZCa=COMPLEX(0,-5)
ZCb=COMPLEX(0,-10)
Z1=ZLa*ZR/(ZLa+ZR)=IMDIV(IMPRODUCT(ZLa,ZR),IMSUM(ZLa,ZR))
Z2=ZLb*ZCb/(ZLb+ZCb)=IMDIV(IMPRODUCT(ZLb,ZCb),IMSUM(ZLb,ZCb))
ZA=IMSUM(Z1,Z2); ZB=IMSUM(Z2,ZCa);ZC=IMSUM(Z1,ZCa)
Zab=ZA*ZCa/(ZA+ZCa)=IMDIV(IMPRODUCT(ZCa,ZA),IMSUM(ZCa,ZA))
Zag=Z1*ZB/(Z1+ZB)=IMDIV(IMPRODUCT(Z1,ZB),IMSUM(Z1,ZB)
Zbg=Z2*ZC/(ZC+Z2)=IMDIV(IMPRODUCT(Z2,ZC),IMSUM(Z2,ZC))

upload_2019-1-28_8-29-5.png
 

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Wow! @Babadag that was kind of impressive. I do remember using Excel to attempt complex number mathematics, but found other methods.

If you are familiar with Python, it easily handles complex numbers.
note that Python uses the letter j after a number to indicate the imaginary component.
Code:
# Here is a simple function in Python, using a lambda function.
# it will calculate the parallel equivalent of two impedances.
#
zpar2 = (lambda x,y: x*y /(x+y))
print(zpar2(1,2j))
# here is the output
(0.8+0.4j)

R is another popular interpreted programming language, which is also available for free.
It also handles complex and imaginary (using the traditional i )
Code:
# R code for parallel impedances.
par2 <- function(a,b) { return (a*b / (a+b))}
par2(1,1i)
# here is the output
[1] 0.5+0.5i

Note these are simple calculations. I didn't put in any handling for when the denominator to be zero.
 
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Thank you very much, scottdave! It is very interesting, indeed.