JIT HW 25-9 Conductors are commonly used as places to store charge You can’t just “create” some positive charge somewhere, you have to have corresponding.

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Presentation transcript:

JIT HW 25-9

Conductors are commonly used as places to store charge You can’t just “create” some positive charge somewhere, you have to have corresponding negative charge somewhere else Definition of a capacitor: Two conductors, one of which stores charge +Q, and the other of which stores charge –Q. Capacitors  V ab +Q+Q –Q–Q Can we relate the charge Q that develops to the voltage difference  V? Gauss’s Law tells us the electric field between the conductors Integration tells us the potential difference Ch 26

The relationship between voltage difference and charge is always linear This allows us to define capacitance Capacitance has units of Coulomb/Volt Also known as a Farad, abbreviated F A Farad is a very large amount of capacitance Let’s work it out for concentric conducting spheres: Capacitance What’s the capacitance of the Earth, if we put the “other part” of the charge at infinity?

A “more typical” geometry is two large, closely spaced, parallel conducting plates Area A, separation d. Parallel Plate Capacitors Let’s find the capacitance: Charge will all accumulate on the inner surface Let +  and –  be the charges on each surface As we already showed using Gauss’s law, this means there will be an electric field given by If you integrate the electric field over the distance d, you get the potential difference A d To get a large capacitance, make the area large and the spacing small Circuit symbol for a capacitor:

JIT Ans d

Warmup 78

Solve on board

JIT Quick Quiz 26.2 Ans a (increase)

Capacitors in Parallel 2 V 3  F 6  F When we close the switch, how much charge flows from the battery? A) 36  CB) 4  CC) 18  C D) 8  CE) 10  C The voltage difference across each capacitor will be 2 V. When capacitors are connected like this at both ends, we say they are connected in parallel The combined capacitors act like a single capacitor with capacitance:

Capacitors in Series VV C1C1 Charge flows to the left side of the first capacitor Since capacitors have balanced charge, the right side must have the equal and opposite charge The only place it can get this charge is the left side of the right capacitor The charges on the second capacitor are also balanced C2C2 When we close the switch, which capacitor gets more charge Q on it? A) The one with the bigger capacitance B) The one with the smaller capacitance C) They get the same amount of charge D) Insufficient information +Q -Q +Q -Q V1V1 The voltage difference on each capacitor is not the same, since only one end is connected. But the charge is the same. The two voltages differences can be added together V2V2

Warmup 78

Series and Parallel When two circuit elements are connected at one end, and nothing else is connected there, they are said to be in series When two circuit elements are connected at both ends, they are said to be in parallel C1C1 C2C2 C1C1 C2C2 These formulas work for more than two circuit elements as well. C1C1 C2C2 C3C3 C4C4 C5C5

JIT Quick Quiz 26.3 Ans a

Ans B Ans A,B Ans C

Sample Problems 60  F What is the capacitance of the structure shown at left? A) 180  FB) 120  FC) 30  F D) 20  FE) none of the above They are connected end-to-end, so they are in series Now add a wire across the middle. The two ends of the middle capacitor are at the same potential; therefore, there is no charge on this capacitor You might as well ignore it

Complicated Capacitor Circuits 4 The capacitance of the capacitors in pF below is marked. What is the effective capacitance of all the capacitors shown? For complex combinations of capacitors, you can replace small structures by equivalent capacitors, eventually simplifying everything 10 V Capacitors 1 and 5 are connected at both ends- therefore they are parallel 6 Capacitors 3 and 6 are connected at just one end – therefore they are series 2 All three capacitors are now connected at both ends – they are all in parallel

Solve on board

Warmup09

Energy in a capacitor Suppose you have a capacitor with charge q already on it, and you try to add a small additional charge dq to it, where dq is small. How much energy would this take? The side with +q has a higher potential Moving the charge there takes energy The small change in energy is: +q –q dq Now, imagine we start with zero charge and build it up gradually to q = Q It makes sense to say an uncharged capacitor has U = 0

Energy in a capacitor (2) 20 V 1  F2  F 20 V 1  F2  F For each of the two circuits, which capacitor gets more energy in it? A) The 1  F capacitor in each circuit B) The 2  F capacitor in each circuit C)The 1  F capacitor in the top circuit, the 2  F capacitor in the bottom circuit D) The 2  F capacitor in the top circuit, the 1  F capacitor in the bottom circuit E) They are equal in each circuit Capacitors in parallel have the same voltage difference  V The larger capacitor has more energy Capacitors in series have the same charge Q The smaller capacitor has more energy

Ans A

Energy density in a capacitor Suppose you have a parallel plate capacitor with area A, separation d, and charged to voltage  V. (1) What’s the energy divided by the volume between the plates? (2) Write this in terms of the electric field magnitude A d Energy density is energy over volume We can associate the energy with the electric field itself This formula can be shown to be completely generalizable It has nothing in particular to do with capacitors

JIT Ans b

Solve on Board

Warmup09

Dielectrics in Capacitors What should I put between the metal plates of a capacitor? Goal – make the capacitance large The closer you put the plates together, the bigger the capacitance It’s hard to put things close together – unless you put something between them When they get charged, they are also very attracted to each other Placing an insulating material – a dielectric – allows you to place them very close together The charges in the dielectric will also shift This partly cancels the electric field Small field means smaller potential difference C = Q/  V, so C gets bigger too ––––––––––––––––––––––––

Choosing a dielectric What makes a good dielectric? Have a high dielectric constant  The combination  0 is also called , the permittivity Must be a good insulator Otherwise charge will slowly bleed away Have a high dielectric strength The maximum electric field at which the insulator suddenly (catastrophically) becomes a conductor There is a corresponding breakdown voltage where the capacitor fails

JIT Ans a

Consider isolated capacitor Consider isolated capacitor after charging Ans B Ans A

What are capacitors good for? They store energy The energy stored is not extremely large, and it tends to leak away over time Gasoline or fuel cells are better for this purpose They can release their energy very quickly Camera flashes, defibrillators, research uses They resist changes in voltage Power supplies for electronic devices, etc. They can be used for timing, frequency filtering, etc. In conjunction with other parts