Engineering Phasor Circuit Analysis Homework: Understanding Incorrect Answers | MacLaddy

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The discussion centers on a student's confusion regarding the correct application of Kirchhoff's Voltage Law (KVL) in phasor circuit analysis. The student initially arrived at an answer for a circuit problem but was informed by the instructor that a negative sign should be included in the final expression due to the direction of voltage sources. Clarification was provided that when summing potential drops around a loop, a voltage rise is treated as negative, while drops are positive. The conversation also touches on the implications of alternating current sources and their phase relationships, emphasizing the importance of understanding polarity in circuit analysis. Ultimately, the student gains a clearer understanding of KVL and its application in their coursework.
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Homework Statement



Hello folks. I had a recent midterm where I got a problem wrong, but I'm not sure I understand why. I am hoping someone here can shed some light. Please see the attached circuit diagram.

Homework Equations



Phasor notation stuff... I am correct on all except one sign. Please see below.

The Attempt at a Solution



Using superposition, and considering the sources as Case 1, and Case 2, as noted in the image.

Case 1:

12cos(2000t)=12\angle{0^\circ}
cap= -40j
Ind= 10j

Using KVL

-12\angle{0^\circ}+(-40j)I_1+30I_1+10jI_1=0
I_1=0.28\angle{45^\circ}
I_1=0.28cos(2000t+45^\circ)

Case 2:

18cos(4000t)=18\angle{0^\circ}
cap= -20j
Ind= 20j

Using KVL

-18\angle{0^\circ}+(-20j)I_2+20jI_2+30I_2=0
I_1=0.6\angle{0^\circ}
I_1=0.6cos(4000t)

Final answer

i(t)=0.28cos(2000t+45^\circ)+0.6cos(4000t)

However, my instructor says that the answer above should have a negative sign instead of a positive. Like this...

i(t)=0.28cos(2000t+45^\circ)-0.6cos(4000t)

He explained that he is following KVL by using the sign directions that are drawn on the diagram. This seems wrong to me, as that would make every element in the second equation positive.

18\angle{0^\circ}+(-20j)I_2+20jI_2+30I_2=0

But shouldn't the power source always have a different sign than the other elements? If I apply KVL to the above it would indicate that either everything is applying voltage to the element, or everything is removing it.

Any hints on where my thinking is incorrect?

Thanks,
MacLaddy
 

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When you are summing potential drops around a loop, then a potential rise due to a voltage source is written as a negative value, and a potential drop as a positive value.

In your case for the second source you are going clockwise around the loop and when you go through the 18 V source you do it from + to -, so it's a potential drop. It gets treated like any other drop, which is to say, it is summed as a positive quantity.
 
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gneill said:
When you are summing potential drops around a loop, then a potential rise due to a voltage source is written as a negative value, and a potential drop as a positive value.

In your case for the second source you are going clockwise around the loop and when you go through the 18 V source you do it from + to -, so it's a potential drop. It gets treated like any other drop, which is to say, it is summed as a positive quantity.

Thanks gneill. I suppose I'm convinced, especially since you echo my professors sentiments. It just seems unlikely that a polarity direction could be assigned to a current that is alternating. Perhaps this is more of an academic problem than a real life one? At least now I know for sure when the final comes rolling around.

Mac
 
MacLaddy said:
Thanks gneill. I suppose I'm convinced, especially since you echo my professors sentiments. It just seems unlikely that a polarity direction could be assigned to a current that is alternating. Perhaps this is more of an academic problem than a real life one? At least now I know for sure when the final comes rolling around.

Mac
Consider an AC source with a function of time given by ##v1(t) = A sin(\omega t)##. At time t = 0 the value is increasing in the positive direction. Another source ##v2(t) = -A sin(\omega t)## would be decreasing. So the sources are in fact 180° out of phase. The polarity of the symbol used in the schematic tells you the relative orientation of the sources' basic phase angles.
 
Last edited:
gneill said:
Consider an AC source with a function of time given by ##v1(t) = A sin(\omega t)##. At time t = 0 the value is increasing in the positive direction. Another source ##v2(t) -A sin(\omega t)## would be decreasing. So the sources are in fact 180° out of phase. The polarity of the symbol used in the schematic tells you the relative orientation of the sources' basic phase angles.

Thank you, that I do understand. But aren't the sources above out of phase--have different frequencies? Truly, it doesn't matter too much. I'm a mechanical guy taking an electrical class. I believe I understand well enough now for my purposes.

Mac
 
MacLaddy said:
Thank you, that I do understand. But aren't the sources above out of phase--have different frequencies?
Their relative phases will change over time due to having different fundamental frequencies, yes. It's not always the case though, and relative phase matters a great deal in many cases.
 
A.sin(ωt) and -A.sin(ωt)
have the same peak amplitude, A
have opposite phase, meaning they differ by 180°

The pair could be written, equivalently, as A.sin(ωt) and A.sin(ωt - 180°)
because the minus sign for amplitude is, basically, a shorthand way of showing a 180° phase shift
 

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