Electrical, calculate capacitances

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In summary, the problem involves a d.c. supply of 200V and two capacitors, A and B, connected in series with a p.d. of 120V across A. When a 3μF capacitor is connected in parallel with B, the p.d. across A increases to 140V. Using the equations C=Q/V and the rules for calculating total capacitance in parallel and series connections, the values of the two unknown capacitors (Ca and Cb) can be determined. By equating the charges and voltages in the two scenarios, it is found that Ca=3.6μF and Cb=5.4μF.
  • #1
bsbs
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1. Homework Statement

d.c supply 200V
capacitors A and B connected in series
p.d across A is 120V

p.d. across A, increased to 140V when a 3μF capacitor is connected in parallel with B.

attached diagram for better understanding.

Find capacitance of A and B.

2. Homework Equations

C=Q/V
Capacitance total in parallel connection = sum of 'n' numbers of capacitors
Capacitance total in series connection for this case is = 1/Ct = 1/A + 1/(B+3)

3. The Attempt at a Solution

Need help, really don't know where to start with 2 unknown capacitors value.
 
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  • #2
With capacitors in series, charge on the plates of each capacitor is equal. In case 1, denote the charge Q₁ and write the equations relating Q₁, CA, CB, and the voltages.
 
  • #3
NascentOxygen said:
With capacitors in series, charge on the plates of each capacitor is equal. In case 1, denote the charge Q₁ and write the equations relating Q₁, CA, CB, and the voltages.

thanks, i am getting some headway now.

(Qa) = (Ca) x 120
=120μC if assume (Qa) is 1μF

120μC = (Cb) x 80
(Cb) = 1.5

thus, if (Ca)=1, (Cb)=1.5

the ratio is correct now, next hint please, on getting the correct answer.
Now, with the voltage across (Ca) increased to 140V after putting the 3μF in parallel with (Cb)
 
Last edited:
  • #4
bsbs said:
thanks, i am getting some headway now.

(Qa) = (Ca) x 120
=120μC if assume (Qa) is 1μF
Well, we don't make such assumptions! You keep CA as CA and allow the algebra to sort out things (hopefully, eventually it will cancel out).
Now, with the voltage across (Ca) increased to 140V after putting the 3μF in parallel with (Cb)
You repeat the same idea, except now one of the series capacitors has the value (CB + 3*10⁻⁶)
 
  • #5
NascentOxygen said:
Well, we don't make such assumptions! You keep CA as CA and allow the algebra to sort out things (hopefully, eventually it will cancel out).

You repeat the same idea, except now one of the series capacitors has the value (CB + 3*10⁻⁶)

unsolved, but thanks anyway.
 
  • #6
bsbs said:
unsolved, but thanks anyway.

It's exactly the same thing.

You found the first scenario already:

Q = Ca*120
Q = Cb*80

The charges on each capacitor are the same because they are in series.

So:

120 Ca = 80 Cb


The second scenario is the same.

Q = Ca * 140
Q = Ceq * 60

where Ceq is the equivalent capacitance for Cb in parallel with 3uF


This leads to two equations and two unknowns that you can solve for Ca and Cb.

===

You need to be careful with charge redistribution problems. Here you start with a live circuit from scenario A that charges capacitor B to 80 volts. Then an uncharged 3uF cap is added in parallel with B that causes instant charge redistribution. But since you know the voltages across all capacitors it is easy to determine the charges on them.

If voltages are unknown, you sometimes have to follow how the charge redistributes itself across the capacitors in the second connected scenario. This is done by assuming some unknown charge dQ moves from a plate of one capacitor to others and you follow how the charge moves to other capacitors by honouring series and parallel relationships. In parallel connected capacitors, the charge shares such that the voltage across the caps are equal. In series connected capacitors, the same charge magnitude moves onto the second capacitor's plates.

You will run into problems of this nature in the future.
 
  • #7
aralbrec said:
If voltages are unknown, you sometimes have to follow how the charge redistributes itself across the capacitors in the second connected scenario. This is done by assuming some unknown charge dQ moves from a plate of one capacitor to others and you follow how the charge moves to other capacitors by honouring series and parallel relationships. In parallel connected capacitors, the charge shares such that the voltage across the caps are equal. In series connected capacitors, the same charge magnitude moves onto the second capacitor's plates.

You will run into problems of this nature in the future.

Thanks, you are great help, finally solved, valuable piece of info for charge re-distribution

Ca=8cb/12....eqn 1
Ca=18+6Cb/14...eqn 2
eqn1=eqn2

therefore, Cb = 5.4μF

therefore, 120 Ca = 80 x 5.4

Ca = 3.6μF
 

FAQ: Electrical, calculate capacitances

1. What is capacitance?

Capacitance is the measure of an object's ability to store electrical charge. It is represented by the letter C and is measured in units of Farads (F).

2. How do you calculate capacitance?

The capacitance of an object can be calculated by dividing the electric charge on the object by the potential difference across it. This can be represented by the equation C = Q/V, where C is capacitance, Q is charge, and V is potential difference.

3. What factors affect capacitance?

The capacitance of an object is affected by several factors, including the distance between the two conductors, the surface area of the conductors, and the type of material between the conductors.

4. What are some real-life applications of capacitance?

Capacitance has many real-life applications, including in electronic circuits, power transmission, and energy storage devices such as capacitors. It is also used in touchscreens, sensors, and medical equipment.

5. How is capacitance related to electric fields?

Capacitance is directly related to electric fields. The electric field between two charged conductors is directly proportional to the potential difference and inversely proportional to the distance between them. This relationship is described by the equation E = V/d, where E is electric field, V is potential difference, and d is distance.

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