Initial and final values for second order circuits

Click For Summary

Discussion Overview

The discussion revolves around understanding initial and final values in second-order circuits, particularly focusing on the behavior of capacitors and inductors in steady-state DC conditions. Participants are exploring concepts related to voltage across capacitors, current through inductors, and the implications of circuit configurations at specific time instances.

Discussion Character

  • Homework-related
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question how the voltage across an open capacitor can be defined, specifically regarding a voltage of -20V.
  • There is a discussion about the inductor current being zero in steady-state DC due to the absence of a voltage source, with some participants confirming this understanding.
  • One participant proposes using KVL (Kirchhoff's Voltage Law) to derive the voltage across the capacitor, leading to confusion about the negative sign in the voltage measurement.
  • Another participant explains that the reference point for voltage measurements is determined by the placement of the voltmeter leads, which influences the perceived voltage across the capacitor.
  • There is a query regarding the concept of a "direct short" at t=0+ when a capacitor is in series with a voltage source, with participants discussing the implications of this configuration.
  • Some participants express confusion about the relationship between voltage across the resistor and capacitor in a specific circuit scenario, questioning whether the voltage across the resistor should be zero.

Areas of Agreement / Disagreement

Participants generally agree on some foundational concepts, such as the behavior of capacitors and inductors in steady-state DC. However, there are multiple competing views and unresolved questions regarding specific voltage measurements and circuit behaviors, indicating that the discussion remains unresolved.

Contextual Notes

Limitations include potential misunderstandings about voltage references, the implications of circuit configurations at specific time instances, and the application of KVL in analyzing circuit behavior. These aspects remain open to interpretation and further clarification.

sugz
Messages
110
Reaction score
0

Homework Statement



I am attempting to understand this example shown below:

example.PNG


Homework Equations



During stead state DC, the capacitor is an open circuit and the inductor is short circuited.

The Attempt at a Solution


[/B]
The questions I have are really related to the concepts as I don't seem to understand it well enough even after reading through the chapter many times.
1- How is Vc equal to -20V? Since Vc is an open circuit, how would there be a voltage across it?
2- My understanding is that the inductor current (iL) is zero because there is no voltage source in the circuit during steady state DC. Please confirm if my understanding is correct.
3- I have read through the book many times and I don't seem to understand how this is determined. If someone can provide a detailed explanation, I would really appreciate it!
 
Physics news on Phys.org
sugz said:
1- How is Vc equal to -20V? Since Vc is an open circuit, how would there be a voltage across it?
2- My understanding is that the inductor current (iL) is zero because there is no voltage source in the circuit during steady state DC. Please confirm if my understanding is correct.

For (1) consider the circuit as drawn here with a voltmeter placed across the "open" capacitor position:

Fig1.png


The voltmeter leads are placed in such a way as to read the capacitor voltage as it is defined on the diagram. Essentially this makes the "-" lead of the capacitor the reference point for the reading. Now note the path marked out in blue: This comprises a single node since it's all connected by conductor. What is the potential of this node with respect to the voltmeter's reference point? So what will the voltmeter read?

For (2) you are correct in this case. The capacitor is "open" so no current can flow from the 20 V source, and the current supply is zero so no current from there. With no sources of current there can be no current in the circuit.
 
gneill said:
For (1) consider the circuit as drawn here with a voltmeter placed across the "open" capacitor position:

View attachment 89506

The voltmeter leads are placed in such a way as to read the capacitor voltage as it is defined on the diagram. Essentially this makes the "-" lead of the capacitor the reference point for the reading. Now note the path marked out in blue: This comprises a single node since it's all connected by conductor. What is the potential of this node with respect to the voltmeter's reference point? So what will the voltmeter read?

For (2) you are correct in this case. The capacitor is "open" so no current can flow from the 20 V source, and the current supply is zero so no current from there. With no sources of current there can be no current in the circuit.
gneill said:
For (1) consider the circuit as drawn here with a voltmeter placed across the "open" capacitor position:

View attachment 89506

The voltmeter leads are placed in such a way as to read the capacitor voltage as it is defined on the diagram. Essentially this makes the "-" lead of the capacitor the reference point for the reading. Now note the path marked out in blue: This comprises a single node since it's all connected by conductor. What is the potential of this node with respect to the voltmeter's reference point? So what will the voltmeter read?

For (2) you are correct in this case. The capacitor is "open" so no current can flow from the 20 V source, and the current supply is zero so no current from there. With no sources of current there can be no current in the circuit.
Dear gneill, that was a very clear explanation. From what I understand, the "-" lead is connected to the positive side of the voltage, which would make that point +20V. The "+" lead is connected to the single node, which is at a lower voltage. Therefore, the potential of this node with respect to the voltmeter's reference point is 20V. I was a little confused at where the negative sign comes from? I understand that I am able to get -20V if I perform KVL around the third loop (-10-Vc+40*iL=0, where iL equals 0 and therefore Vc=-10V). Is there another way of doing this?
 
Last edited:
sugz said:
Dear gneill, that was a very clear explanation. From what I understand, the "-" lead is connected to the positive side of the voltage, which would make that point +20V.
No, from the point of view of the meter, wherever the "-" lead is is the 0 V reference (for the meter).
The "+" lead is connected to the single node, which is at a lower voltage. Therefore, the potential of this node with respect to the voltmeter's reference point is 20V. I was a little confused at where the negative sign comes from?
Do a "KVL walk" from the meter's "-" lead down through the voltage supply to the blue node. What's the potential of the blue node with respect to the lead?
 
  • Like
Likes   Reactions: sugz
gneill said:
No, from the point of view of the meter, wherever the "-" lead is is the 0 V reference (for the meter).

Do a "KVL walk" from the meter's "-" lead down through the voltage supply to the blue node. What's the potential of the blue node with respect to the lead?
Thank you very much! I understand this now!
 
gneill said:
For (1) consider the circuit as drawn here with a voltmeter placed across the "open" capacitor position:

View attachment 89506

The voltmeter leads are placed in such a way as to read the capacitor voltage as it is defined on the diagram. Essentially this makes the "-" lead of the capacitor the reference point for the reading. Now note the path marked out in blue: This comprises a single node since it's all connected by conductor. What is the potential of this node with respect to the voltmeter's reference point? So what will the voltmeter read?

For (2) you are correct in this case. The capacitor is "open" so no current can flow from the 20 V source, and the current supply is zero so no current from there. With no sources of current there can be no current in the circuit.
I am attempting to solve another problem, which carries over the same concepts. The question I have is related to part (a) where the solution suggests "Since it is in series with the +10V source, together they represent a direct short at t=0+. This means that the entire 2A from the current source flows through the capacitor and not the resistor". Can you please explain this? I am confused about the direct short at t=0+.
 

Attachments

  • question 3.PNG
    question 3.PNG
    19.7 KB · Views: 509
  • question 3 q.PNG
    question 3 q.PNG
    5.3 KB · Views: 510
At the instant t = 0+, the capacitor has a potential difference of -10 V. It's in series with the 10 V voltage source. Together they add up to 0 V. For that instant, the two components can be replaced with single zero volt voltage supply. A zero volt voltage supply is, for all intents and purposes, equivalent to a short circuit (a zero resistance path).
 
  • Like
Likes   Reactions: sugz
gneill said:
At the instant t = 0+, the capacitor has a potential difference of -10 V. It's in series with the 10 V voltage source. Together they add up to 0 V. For that instant, the two components can be replaced with single zero volt voltage supply. A zero volt voltage supply is, for all intents and purposes, equivalent to a short circuit (a zero resistance path).
Oh right! That makes sense! Thanks a lot, once again!
 
gneill said:
At the instant t = 0+, the capacitor has a potential difference of -10 V. It's in series with the 10 V voltage source. Together they add up to 0 V. For that instant, the two components can be replaced with single zero volt voltage supply. A zero volt voltage supply is, for all intents and purposes, equivalent to a short circuit (a zero resistance path).
Hi,
I know this is a little late but I have been attempting to figure this out myself but had no success. In part (b) of that question, it is indicated that vR=vC+10. However, shouldn't vR=0 since all of the 2A goes to the short circuit (capacitor current)? This would make dvR/dt=0?
 
  • #10
sugz said:
Hi,
I know this is a little late but I have been attempting to figure this out myself but had no success. In part (b) of that question, it is indicated that vR=vC+10. However, shouldn't vR=0 since all of the 2A goes to the short circuit (capacitor current)? This would make dvR/dt=0?
Perhaps we're not looking at the same circuit? The one I see in the problem statement has a 3 A supply. When it turns on at time zero its current will be divided between the 2 Ω and 4 Ω resistors essentially instantaneously since, as you say, the capacitor looks like a short circuit to an instantaneous change. I'd expect that VR (or the point labelled "a" on the circuit shown as figure (b)) to pop up from zero to +4 V. From there I suppose there will be some "ringing" in the LC tank circuit which will also be seen on VR, I guess as a damped sinewave.

Maybe this could be made more obvious if you replaced the current source and 2 Ω resistor with their Thevenin equivalent? You'd then have that node "a" in the middle of a voltage divider.
Fig4.png
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
4K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 18 ·
Replies
18
Views
4K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 7 ·
Replies
7
Views
4K
  • · Replies 8 ·
Replies
8
Views
3K