Solving RLC Circuit Problem 1: I1, I2, & I3 Calculations

In summary, when the switch is first closed, I1, I2, and I3 are all zero. After 5 time constants, I1 will be .037A, I2 will be .01258A, and I3 will be .025A.
  • #1
tommoturbo
33
0
1. (See attachment) Q1 a, Determine I1,I2and I3 after 5 time constants
b, when the switch is first closed ie t=0
c,when the switch re opens




2. I total=I1-(i1+I2)

i=I[1-e --RL/L




3. i havnt practiced any circuits with resitance in series and parallel just looking for a way forwerd on how to write the equations down for each one
with the circuit initially closed i imagine its basic kirchhoffs laws to calculate I1,2 and 3 but these will be very small as almost all of the supply voltage is going to the inductor but after 5 time constants at 63.2% steady state the current values will increase


any help appreciated

regards Ian
 

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  • #2
go to this site.
http://knowhowstuff.blogspot.com/search/label/Physics%20Q%20and%20A

there is the answer
 
  • #3
Been awhile since circuits for me. I'm going to assume that you are working with simple differential equations and not something more advanced like Laplace transforms, etc. I think I would sum up the voltage of each loop. The sum of voltage around each loop is set to zero. That will give you 2 equations for I1, I2, I3. The third equation is I1=I2 + I3, the current entering the top node has to equal the two currents leaving it. One of these three equations will be a first order differential equation (DE) in I3. Use the other two equations to eliminate I1 and I2 from this DE and then solve the DE. You'll need an initial condition to solve for the constant of integration. The propery of inductors to oppose sudden changes in current should lead you to the proper initial condition to use for I3 at time zero. Once that is solved for I3, you can use the other two equations to get I1 and I2. The start plugging in your times of zero to get part b, e^(+/-5) to get part a. I assume that part c is meant that after a long time the switch is opened so that the currents have reached steady state.
 
  • #4
Thankyou very much for the replies
Uskalu

As i am only learning, the method i used to calculate the currents for I1 I2 I3
was a very long method giving similar results ie

I2=I1x(R1/R1+R3)
I2=.037(100/300)=12.3mA (.0123A) etc

now the part i don't understand on your working out
is the equation you used to calc the voltage across R2, R2=200x30/800
i don't know where the 30 and 800 come in (as i am only a novice at this)
i got 7.5v as well doing it the long way

also the time constant

when the switch is closed is the time constant

tor=L/R now is the R always 200ohm in this equation for each one of the I1,I2 and I3

as i get it ro be 5mS

your equation is eg I3=.025x.819 (not sure of the .819).

when the switch is closed can it be drawn as (5v with two 100ohm resistors in series and the inductor?)

Please forgive my questioning its just my lack of knowledge in this


Best Regards Ian
 
  • #5
I got a different value for the currents at 5 time constants.

I1=0.0375-0.0125*e^(-5)=0.03741
I2=0.0125*(1+e^(-5))=0.01258
I3=0.025*(1-e^(-5))=0.02517

5 time constants is a long time. So the current values should be very close to the final values after the switch has been shut a long time, when the inductor is acting like a short.
 
  • #6
tommoturbo said:
also the time constant

when the switch is closed is the time constant

tor=L/R now is the R always 200ohm in this equation for each one of the I1,I2 and I3

I got time constant of 5 ms too. However, you don't really need to know it. In general, the exponential can be written as
exp(-t/tau)
where tau is the time constant. You are told that time is 5 time constants or t=5*tau. So the exponential terms are
exp(-5*tau/tau) = exp(-5).

Since the I1 and I2 currents can be written in terms of I3 by simple algebra equations, then the same exp(t/tau) will appear in all three current formulas.
 
  • #7
goto this.
http://knowhowstuff.blogspot.com/2009/05/tension-problem.html

i updated it


"when the switch is closed can it be drawn as (5v with two 100ohm resistors in series and the inductor?)"


initially when time=0 current through inductor is zero.
 
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  • #8
Thank you both for you swift and knowledgeable replies
that has made a lot of sense now.
I think it has finally sunk in

Many Thanks

ian
 
  • #9
One last question, part 4 of this question asks to plt all three currents on a time axis wavefrom. starting from 0mS to 80mS however the switch opens at t=50mS.

As I3 is the current through the inductor i have plotted that fine but as part of the other questions
we found that when the switch is first closed t=0 i1 and I2 = .025A so when i start plotting my graph will i start from 25mA for i1 and i2 and then use the formula i=I[1-e-rt/L]

Basically i can do the inductor circuit plotting fine its what's happening in the rest of the circuit from t=0 onwards and t=50 decaying as switch opens



Many thanks Ian
 
  • #10
You should find the currents I1 and I2, in terms of I3 using the circuit laws. You already have I3, so plug that into I1 and I2. However, you can cheat some to get the current equations. Solve the currents when the switch just closes and the inductor is open circuit. You already have those currents. Now solve the circuit for when the switch is closed a long time, the inductor is a short. That gives you the starting currents and the ending currents. The plots for each current should go from the initial value to the final value in an exponential fashion in which you already know the time constant of 5 ms.
 
  • #11
Right i see so my graph will start at 0 from t=0 (as inductor is open circuit)with i3 rising exponentially to 99.3% of max steady state current until switch opens and then decays exponentially.

And at T=0 (instant switch closes I1=37.5mA and i2 = 12.5mA

after a steady state and the switch reopens
I3 will equal I1 + I1 and will be 25mA

will i1 drop straight to 0A
and i2 jump instantly to 25mA?

or do i keep the steady state figure and use the decay exponential equations for them

Thanks again for your help, i tought i had it sussed just try ing to get my head around what happens in the rest of the circuit.

Best Regards Ian
 
  • #12
tommoturbo said:
Right i see so my graph will start at 0 from t=0 (as inductor is open circuit)with i3 rising exponentially to 99.3% of max steady state current until switch opens and then decays exponentially.

Yes, for I3 this is what will happen.

And at T=0 (instant switch closes I1=37.5mA and i2 = 12.5mA

Nope. Those are the final values after the switch has been closed a long time.

after a steady state and the switch reopens
I3 will equal I1 + I1 and will be 25mA

will i1 drop straight to 0A
and i2 jump instantly to 25mA?

I think you meant I3 = I1 + I2, and not that's not correct. You need to make sure to keep the signs right. Both I2 and I3 are leaving the junction. I1 is entering it. So you have to write it as I1 = I2 + I3 (unless you change the picture). With I1=0, you have I2 = - I3.

In ideal cuircuit laws, there is nothing to prevent I1 from suddently changing (step function) from one value to another, like to zero. I1 does not pass through any inductors which prevent that. Same for I2. I2 is allowed to suddenly change. I3 can't change suddenly because of the inductor. The I3 current just before the switch is opened and just after have to be the same.

or do i keep the steady state figure and use the decay exponential equations for them

Answered above. However, don't forget that the change in circuit configuration when the switch is opened will lead to a different time constant when the switch is opened.
 
  • #13
Thanks for all the help Chris I am starting to understand it now, the only time i get to work through it is when I am working nights and my brain usually gets puddled quickly.

one final question

as the time constant for the ciruit when the switch is closed is tor=L/R 1/200=.005s

how do i get the open circuit time constant I am not sure what figures to plug in as the switch is open no current will flow through R2 and the only circuit flow will be reverse emf for the 5 times constants as the the inductor decays.


initially i thought both open circuit and closed had the same value?
but now i realize fom you help that it probably wont, I am not sure how to work the open circuit time constant out

Sorry if I am being simple its just that when i first started working it out and completing it from your replies i went back through my work to check what i had and realized i hadnt initially understood what was being asked in the question.


Regards Ian
 
  • #14
tommoturbo said:
how do i get the open circuit time constant I am not sure what figures to plug in as the switch is open no current will flow through R2 and the only circuit flow will be reverse emf for the 5 times constants as the the inductor decays.

That's the answer. No current flow through R2. So R2 can't effect the circuit operation. However, there is a current through both R1 and R3, so ...

(your have only a single circuit loop with L1, and the resisters in series)
 
  • #15
Thanks for all your help Chris i think i have it sussed now

couldnt have done it without you explanations


Regards Ian
 
  • #16
How did you solve for part c. When the circuit reopened? Specifically for I2.
 
  • #17
Welcome first time poster. Most of the answer has been given above in the discussion. To reiterate, when the switch is opened, no charge can flow in the left hand side of the circuit. There is not a complete path for them to follow. So I1 goes to zero. This means that resister R2 no longer has any effect on the circuit. Suggest you redraw the circuit with just the right hand side since left hand side has no effect after the switch is opened.

Since what is left is a single loop, I2 has to be the same as I3. No charge can just appear from nowhere at that top node point to make I3 and different from I2. Because the arrows are drawn in opposite directions, I2 will be of opposite sign of I3 but same magnitude.

Can you solve the circuit that is left, two resisters in series with the inductor? The two things you need to know is 1) This circuit will have a different time constant than part a and b, because R2 not longer matters. 2) Since I3 is going through the inductor it can't change instantaneously after the switch is opened. It has to have the same current as before the switch is opened. That becomes your new initial condition for solving this second circuit.
 

FAQ: Solving RLC Circuit Problem 1: I1, I2, & I3 Calculations

1. How do I calculate the current in each branch of an RLC circuit?

In order to calculate the current in each branch of an RLC circuit, you will need to use Kirchhoff's laws. First, apply Kirchhoff's current law to each node in the circuit to determine the total current entering and leaving the node. Then, use Kirchhoff's voltage law to determine the voltage drops across each component in the circuit. Finally, use Ohm's law (V=IR) to calculate the current in each branch of the circuit.

2. What values do I need to know in order to solve an RLC circuit problem?

In order to solve an RLC circuit problem, you will need to know the values of the resistors, inductors, and capacitors in the circuit, as well as the voltage and frequency of the power source. Additionally, you may need to know the values of any initial conditions, such as the initial charge on a capacitor or the initial current through an inductor.

3. How do I determine the phase angle in an RLC circuit?

The phase angle in an RLC circuit can be determined by calculating the impedance of each component and then using the formula tan⁡θ=XL−XC/R, where XL and XC are the inductive and capacitive reactances, respectively, and R is the resistance. This will give you the phase angle between the voltage and current in the circuit.

4. Can I use the same method to solve RLC circuits with AC and DC sources?

No, the method for solving RLC circuits with AC sources is different from the method used for DC sources. With AC sources, you will need to use complex numbers and phasor diagrams to represent the voltages and currents in the circuit. However, the basic principles of Kirchhoff's laws and Ohm's law still apply.

5. What is the purpose of solving RLC circuit problems?

The purpose of solving RLC circuit problems is to analyze and understand the behavior of electrical circuits with resistors, inductors, and capacitors. This can help in designing and troubleshooting electronic circuits and systems, as well as in predicting the behavior of AC and DC power sources in different applications.

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