- #1
freshbox said:Hi guys, I want to ask if I can use the voltage divider rule to solve for part (ii).
Thanks!
freshbox said:Total capcitance of two capacitors in series:
Ct=C1xC2/C1+C2 is also the same as 1/Ct=1/C1+1/C2
Is the any difference between them? How come there are 2 type of ways to find the total C.
freshbox said:Ok, thank you. Can I ask if the above diagram capacitors are being replaced by inductor, can I still use the voltage divider rule to solve?
Thanks.
The DC resistance of an ideal inductor is zero. While capacitors behave as open circuits and can charge up to present a potential difference, inductors behave as short circuits and just conduct more and more current. I = (V/L)t.freshbox said:No, why?
Does the voltage divider rule for inductor exist? Because I can't find the formula in my book but I did some googling and found a formula for it.
freshbox said:Is the VDR for capacitor the same as Inductor?
Shouldn't the result be in volts if it's a voltage? Where are the units for your C5?freshbox said:Ok. I can't get the answer for part (iii.)
My working:
V3=CtE/C5 = 2.42x10-6x25/14=4.321uC
That provided answer looks suspiciously large. 0.733J is a lot of energy for a small capacitor to hold... check the given units.Wc=1/2CV2
=1/2x8x10-6x(4.321x10-6)2
=7.468x10-17J
Ans is:0.733J
*I combined C3 and C4 together to form C5. From there, i tried to find the voltage across the new C5 reason being voltage for C3 and C4 is the same in parallel. My new V3 is also equal to the V across C3 and C4.
After getting the new voltage "C5", I sub the values inside the formula including the 8uf (C4) but i cannot get the answer.
freshbox said:7.468x10-17J is my answer
0.733J is the book answer.
So if ignore the rounding off errors am I'm right?
Yes, that's closer to what I found: 74.32 μJ.freshbox said:My bad. 74.6uJ. I'm sorry can you help me take a look at another question...
My working:
250x10-3=5002x1800x4∏x10-7xA / 200x10-3
50000x10-6=5002x1800x4∏x10-7xA
A=50000x10-6[/SUP / 5002x1800x4∏x10-7
A=0.000008841x101
freshbox said:law of indices division = minus
-6/-7 = -6 - -7 = 1
This what I'm thinking..
freshbox said:Sorry, going back to post #12. Is there something wrong with my concept+answer?
I missed out C1 earlier on and i use VDR on C2 and C34 instead. I thought VDR only apply for 2 capacitors and how can i use it if i have 3 capacitors at that time?
I notice that you are rounding intermediate results as you go along and not keeping enough guard digits to prevent rounding errors from entering your later calculated values. You apply two different (but correct) methods to find a given value and end up with different numbers in the significant figures. This is rounding/truncation errors biting you.freshbox said:So if what i said in post #20 is correct, redoing everything...
The method in post #12 was fine, but you made some errors in applying it, such as using '14' for the value of C5 when it should have had units of microfarads included.Since Ct=2.42uF (2.414 μF)
Q=VC
Q=25x2.42=60.5uC (60.345 μC)
Qt=Q1=Q2 (Series Circuit)
V2=8.64v (8.621 V)
Finding Voltage across C1, naming it as V1
Q=VC
60.5uC=V x 5uF
V1=12.1V (12.069 V)
V2+V1=8.64+12.1
= 20.74V (20.690 V)
Et-20.74=4.26V (4.310 V)
4.26V is the voltage across C3 and C4
Subbing all the values into the energy stored in C formula, the answer i got is 72.59uJ (74.316 μJ then rounded to 74.32 μJ for "final answer"). So can I say post #12 working+concept = wrong while this is the correct one.
Please help me take a look, thank you.
PS: Just curious, is part (ii) still doable using the VDR method?
Sorry, I don't follow your question, but it is true that most problems can be solved via several approaches.freshbox said:Thank you gneill for your explanation so far. So can I say that post #12/23 question has a couple of ways to solve it?
It means that the currents and voltages settle into a steady state after which no further changes in their values take place unless the circuit is disturbed in some fashion (like a switch being thrown).I would like to ask you a question relating to the picture below:
"currents and voltages have reached their final values" -> Does it have another meaning as current and voltage = @ max value. ?
freshbox said:Is 5 time constant = steady state/final values? Because I know that at 5 time constant, for capacitor: v is max/i is 0. Inductor: v is 0/I is max. So for this case, is Vc=35v (max value) ?
It applies when there is only one TYPE of energy storing device (inductor or capacitor) in a circuit. There can be multiple capacitors or multiple inductors, but not a mix of both.freshbox said:Do you mean that the 5 time constants concept is only applicable when the circuit only have 1 inductor or 1 capacitor by itself. So for this question, because there is a mixture of inductor and capactor, the 5 time constants concept cannot be apply here?
Thanks.
freshbox said:So the question says that it has reached its final value, does it mean that it is at 5 time constant?
The problem statement says to assume that the currents and voltages have reached their final values. There are no constraints placed on how long you are allowed to wait to ensure that this happens. So just assume that enough time has passed regardless of how long it might be (and you do not care about the specific amount of time!); once a circuit reaches steady state it will no longer change no matter how much more time passes.freshbox said:Do you mean that it can happen at any time? Why does it not matter? Is it because this circuit has 2 type of device?
A series parallel capacitive circuit is a type of electrical circuit that contains both series and parallel connections of capacitors. This means that some capacitors are connected in a series, while others are connected in parallel.
In a series parallel capacitive circuit, the capacitors connected in series have the same amount of charge on each plate, but the total voltage is divided among them. The capacitors connected in parallel have the same voltage across them, but the total charge is divided among them.
One advantage of using a series parallel capacitive circuit is that it allows for the combination of different capacitor values to achieve a desired capacitance. It also allows for a more compact circuit design and can handle higher voltages and currents compared to a single capacitor.
A limitation of a series parallel capacitive circuit is that it can be more complex to analyze and design compared to a simple series or parallel circuit. It also has a limited frequency response, meaning it may not be suitable for high frequency applications.
To calculate the total capacitance in a series parallel capacitive circuit, you can use the formula: 1/Ctotal = 1/C1 + 1/C2 + 1/C3 + ... where C1, C2, C3, etc. are the individual capacitances of the capacitors connected in parallel. You can then use this total capacitance value in other equations to analyze the circuit.