Circuit analysis - series capacitors

In summary, the conversation discusses a problem involving two capacitors of different values in series attached to a DC source. The original poster is unsure if they have solved the problem correctly and asks for help in solving it individually. Other posters discuss the concept of time constant and how it applies to this problem, as well as the importance of considering the entire circuit and not just individual components when solving problems. They also touch on the concept of Thevenin equivalents and how they can be used to simplify circuits.
  • #1
Steve13579
12
0
I am hoping that general physics is the correct location for this problem, but if I am wrong please say so. I have a problem where two capacitors of different value are in series and are attached to a DC source.

Homework Statement


IiX24S5.png

Image is a bit blurry but that is how our professor scanned it. This is practice he said we should do, and I solved it for V total but not individually.

relevant formulas: C(dv/dt) tou=RC

attempt at solution:
at t=0; v=0
at t=∞; v=12

(v-12)/100k + c(dv/dt) = 0
(dv/dt) + 5v = 60
than solving the differential equation I get
v = c1e-5t + 12
solving for c1 I got the final solution
v(t) = -12e-5t + 12

How would I go about solving individually? And did I even get the correct solution? It is logical for t=0 being 0v and at t=∞ getting 12v

Thanks,
Steve
 
Last edited:
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  • #2
I figured it out, sort of.
You set up:
C(dv/dt) + (v-4)/(100k) = 0 and
C(dv/dt) + (v-8)/(100k) = 0
where C = 2uF
The part I still don't understand is why capacitance is the same for both equations but voltage is not.
 
  • #3
I'm working on this problem as well. It turns out that problem you posted comes out of the textbook that my professor wrote , funny enough. You should use voltage division to find the voltages at t=infinity

I'm stuck how how the time constant is the same both of the capacitors, isn't it just R*C but C is different?
 
  • #4
Maylis said:
I'm working on this problem as well. It turns out that problem you posted comes out of the textbook that my professor wrote , funny enough. You should use voltage division to find the voltages at t=infinity

I'm stuck how how the time constant is the same both of the capacitors, isn't it just R*C but C is different?

Some questions to ask yourself:
How do capacitors in series "add"? What capacitance does the rest of the circuit "see" that determines the time constant? In a series circuit can there be different currents in different components? Can current be flowing in one part of a series circuit but not in another?
 
  • #5
The phrase ''what capacitance does the rest of the circuit see'' is just too vague for me to be able to make anything useful out of it. Anything related to sight and I don't know, I can't see any circuit components vision. I thought that the time constant is the thevenin resistance times the capacitance. It is actually the thevenin capacitance times the thevenin resistance?

The way I understand the time constant conceptually, its the time required for the capacitor to reach ~63% of its max charge. If the capacitance is different, then it stands to reason that time to reach that 63% is different, no?

What if I kept the capacitors separate instead of combining them? Then one capacitor ''sees'' the other one and vice versa.

This is part of why I have issues with these problems. I drew up another one to contrast this problem, where the time constant is different for each inductor. To me, the problems look different and I cannot make the connection why in this problem in the time constant is different, but in the original problem they are the same. I think they should be solved in a similar manner. I am missing something fundamental I think that is underlying the concept regarding thevenin equivalents but not discussed in great enough detail in the book to know it without discovering it myself or having outside help. I definitely haven't discovered it myself.

For the problem I posted, I don't see what inductance and resistance each inductor ''sees''
 

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  • #6
Maylis said:
The phrase ''what capacitance does the rest of the circuit see'' is just too vague for me to be able to make anything useful out of it. Anything related to sight and I don't know, I can't see any circuit components vision. I thought that the time constant is the thevenin resistance times the capacitance. It is actually the thevenin capacitance times the thevenin resistance?
"Thevenin Capacitance" doesn't have an official definition that I'm aware of, but I think I understand what you're driving at. A first order circuit (one containing just one type of reactive component) will have resistance and capacitance, or resistance and inductance. Reducing the circuit to a simple equivalent circuit of a lumped resistance and lumped reactance ill tell you how the whole thing will behave in terms of time.

If the circuit is simple enough that inductances or capacitances can be combined and reduced using the usual rules for parallel or serial components then that's the way to go. When things are complicated by having resistances in the way so that such simple combinations are not viable then one can resort to performing a circuit analysis (by whatever method) in the Laplace domain to derive the differential equation or transfer function as desired.

The way I understand the time constant conceptually, its the time required for the capacitor to reach ~63% of its max charge. If the capacitance is different, then it stands to reason that time to reach that 63% is different, no?
Yes, if the net capacitance is changed then the time constant will change. The net capacitance does not change for a fixed circuit. A given first order circuit can have only one time constant that applies to all voltage and current dynamics in the circuit.

What if I kept the capacitors separate instead of combining them? Then one capacitor ''sees'' the other one and vice versa.
The net capacitance of the fully reduced circuit model will still be the same. Overall circuit behavior depends on the actions of all components working in combination. Cutting out a component changes the circuit. If you cut out a component and reduce what's left, then tack the component back on, you must then reduce the new circuit again. You'll end up with the same equivalent model.

This is part of why I have issues with these problems. I drew up another one to contrast this problem, where the time constant is different for each inductor. To me, the problems look different and I cannot make the connection why in this problem in the time constant is different, but in the original problem they are the same. I think they should be solved in a similar manner. I am missing something fundamental I think that is underlying the concept regarding thevenin equivalents but not discussed in great enough detail in the book to know it without discovering it myself or having outside help. I definitely haven't discovered it myself

Your example is a bit misleading because the short circuit created by the switch at t = 0 effectively isolates the two inductive branches into separate circuits. The short circuit will not allow any current from one branch to flow through the other branch, and the short permits no potential difference from one branch to affect the other. Short circuits and fixed voltage sources can effectively isolate loops from interacting with each other.
 
  • #7
Thanks for the lengthy response. I was walking on the quad about 10 mins and your argument about the current clicked in my head. So the current stops in both capacitors at the same time. Hence the time constants must be equal.

I also took a look at my inductor circuit and I see what you are saying. My professor loves putting short circuits in exam problems to make complicated circuits at first site reduce to something more manageable as long as you notice the short circuit
 
  • #8
Maylis said:
Thanks for the lengthy response. I was walking on the quad about 10 mins and your argument about the current clicked in my head. So the current stops in both capacitors at the same time. Hence the time constants must be equal.
Yup :smile:

I also took a look at my inductor circuit and I see what you are saying. My professor loves putting short circuits in exam problems to make complicated circuits at first site reduce to something more manageable as long as you notice the short circuit

Yes, it's one of those sneaky tricks that one has to beware of, or perhaps more constructively, be ready to take advantage of :smile:
 
  • #9
Thanks guys! My exam actually had two series capacitors, but it wanted voltage on one after a given time knowing current. I used C calculated from both capacitors and found overall voltage using 1/C integral i(x)dt, than used a ratio between the two capacitors. Is there a more direct root? And charge is same on both capacitors right, despite different capacitance values?
 
  • #10
Steve13579 said:
Thanks guys! My exam actually had two series capacitors, but it wanted voltage on one after a given time knowing current. I used C calculated from both capacitors and found overall voltage using 1/C integral i(x)dt, than used a ratio between the two capacitors. Is there a more direct root? And charge is same on both capacitors right, despite different capacitance values?

If you know the current with respect to time for the particular capacitor you can directly perform the integration to find its charge and hence voltage.
 

Related to Circuit analysis - series capacitors

What is a series capacitor?

A series capacitor is a type of electronic component that is used in circuits to store and release electrical energy. It is made up of two conductive plates separated by a non-conductive material, known as a dielectric. When connected in series, capacitors allow the flow of alternating current (AC) while blocking direct current (DC).

How does a series capacitor affect a circuit?

A series capacitor affects a circuit by introducing a capacitive reactance, which is a type of opposition to the flow of AC. This reactance can change the overall impedance of the circuit, which can affect the flow of current and voltage. In other words, a series capacitor can change the behavior of a circuit by altering its electrical properties.

What is the formula for calculating the total capacitance of series capacitors?

The formula for calculating the total capacitance of series capacitors is: 1/C = 1/C1 + 1/C2 + 1/C3 + ... 1/Cn, where C is the total capacitance and C1, C2, C3, etc. are the individual capacitance values of each capacitor in the series. This formula takes into account the fact that capacitors in series add up to a smaller total capacitance than if they were connected in parallel.

How can series capacitors be used in practical applications?

Series capacitors have a variety of practical uses in electronic circuits. They can be used to filter out unwanted frequencies, store energy, and stabilize voltage levels. They are also commonly used in power supplies, audio equipment, and signal processing circuits.

What are some common problems that can occur with series capacitors?

One common problem with series capacitors is the occurrence of voltage drops across individual capacitors due to leakage or breakdown. This can lead to a decrease in the overall capacitance of the circuit. Additionally, series capacitors can introduce phase shifts in the AC signal, which can affect the accuracy of the circuit's output. It is important to carefully select and properly connect series capacitors to avoid these issues.

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