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Department of Physics and Applied Physics 95.144, Summer 2015, Lecture 9 Course website: http://faculty.uml.edu/Andriy_Danylov/Teaching/PhysicsII Lecture Capture: http://echo360.uml.edu/danylov201415/physics2spring.html Lecture 9 Chapter 29 Capacitors and more 07.17.2015 Physics II 95.144

L9 Ch29 Su15

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Page 1: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Course website:http://faculty.uml.edu/Andriy_Danylov/Teaching/PhysicsII

Lecture Capture: http://echo360.uml.edu/danylov201415/physics2spring.html

Lecture 9

Chapter 29

Capacitors and more

07.17.2015Physics II

95.144

Page 2: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

The Geometry of Potential and Field

Page 3: L9 Ch29 Su15

Which set of equipotential surfaces matches this electric field?

A)

B)

C)

ConcepTest 1 El. Potential/Area

D)

E)

F)

E

Page 4: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Potential of a Conductor

i

f

sdEVVVf

iif

0V if VV

A conductor in electrostatic equilibrium is at the same potential.

constV

Page 5: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

The Electric Battery

A battery transforms chemical energy into electrical energy.

Chemical reactions within the cell create a potential difference between the terminals by slowly dissolving them.

Atom of Zn gets dissolved leaving two electrons behind

Two electrons get attracted by the ion of Zn leaving behind positively charged electrode

Page 6: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Capacitor

Page 7: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Capacitor stores energy

You can store potential energy by pulling a bow, stretching a spring, etc.

A capacitor is a system that stores potential energy in a form of an electric field.

Page 8: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Capacitance (definition)

The ratio of the charge Q to the potential difference VC is called the capacitance C:

The SI unit of capacitance is the farad:

VC

Page 9: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Parallel-plate capacitor

In its simplest form, a capacitor consists of a pair of parallel metal plates separated by air/insulating material.

Page 10: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Parallel-plate capacitorLet’s find capacitance of a parallel-plate capacitor

Capacitance is a purely geometric property of two electrodes because it depends only on their surface area and spacing.

E

d

Aarea

+Q–Q

The electric field between the plates is ‐ surface

charge density

(Eq.28.26)The potential difference between plates:

We need to find Q and ΔV:

≝ = 

This gives the capacitance:

Page 11: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Parallel-plate capacitor

We can increase capacitance by increasing area A (by making “a roll of metal and insulator”

Page 12: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Parallel-plate capacitor/keyboard

Capacitors are important elements in electric circuits. They come in a variety of sizes and shapes.

The keys on most computer keyboards are capacitor switches. Pressing the key pushes two capacitor plates closer together, increasing their capacitance.

Page 13: L9 Ch29 Su15

What is the capacitance of these two electrodes?

A) 8 nF

B) 4 nF

C) 2 nF

D) 1 nF

E) Some other value

ConcepTest 2 Capacitance

Page 14: L9 Ch29 Su15

Since the battery stays connected, the potential difference must remain constant!

+Q –Q

dAC 0

A parallel-plate capacitor initially has a voltage of 400 Vand stays connected to the battery. If the plate spacing is now doubled, what happens?

A) the voltage decreases

B) the voltage increases

C) the charge decreases

D) the charge increases

E) both voltage and charge change

ConcepTest 3 Varying Capacitance I

Follow-up: How do you increase the charge?

Since , when the spacing d is doubled, the capacitance C is halved.

And since , that means the charge must decrease.

Q = C∆V

400 V

Page 15: L9 Ch29 Su15

Once the battery is disconnected, Q has to

remain constant, since no charge can flow

either to or from the battery.

A parallel-plate capacitor initially has a potential difference of 400 V and is then disconnected from the charging battery. If the plate spacing is now doubled (without changing Q), what is the new value of the voltage?

A) 100 V

B) 200 V

C) 400 V

D) 800 V

E) 1600 V

+Q –Q

dAC 0

ConcepTest 4 Varying Capacitance II

Since , when the spacing d is

doubled, the capacitance C is halved. And since , that means the voltage must double

400 VQ = CV

Page 16: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

CapacitorsIn Series

and Parallel

Page 17: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Combinations of Capacitors In practice, two or more capacitors are sometimes joined together. The circuit diagrams below illustrate two basic combinations:

parallel capacitors and series capacitors.

The equivalent capacitance is the capacitance of the single capacitor that can replace a set of connected capacitors without changing the operation of the circuit

Page 18: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Capacitors in ParallelConsider three capacitors connected in parallel.

QRea

l cir

cuit

Equ

ival

ent c

ircu

it

ΔV

, ΔV

, ΔV

, ΔV

Q ΔV

Ceq

Capacitors in parallel have the same potential difference, ΔV

Q is a total charge drawn from the battery + +

Since ≝;;;

We have replaced 3 capacitors with a “equivalent” capacitor.

+ +

+ +

Conservation of charge

Ceq is inserted without changing the operation of the circuit, so Q and ΔV are same as in the real circuit

Equivalent capacitance of capacitors in parallel.

=

Page 19: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

+ +

Capacitors in SeriesConsider three capacitors connected in series.

QRea

l cir

cuit

Equ

ival

ent c

ircu

it

+Q

Q ΔV

Ceq

Capacitors in series have the same charge, Q.

+ +

Since ≝

Ceq is inserted without changing the operation of the circuit, so Q and ΔV are same as in the real circuit

Equivalent capacitance of capacitors in series.

C1 C2 C3

+ -

-Q +Q -Q +Q -Q

ΔV

ΔV1 ΔV2 ΔV3

Page 20: L9 Ch29 Su15

The 2 equal capacitors in series add up as inverses, giving 1/2C. These are parallel to the first one, which add up directly. Thus, the total equivalent capacitance is 3/2C.

ConcepTest 5 Equivalent Capacitor I

o

o

C CCCeq

A) Ceq = 3/2CB) Ceq = 2/3CC) Ceq = 3CD) Ceq = 1/3CE) Ceq = 1/2C

What is the equivalent capacitance,

Ceq , of the combination below?

in series

o

o In parallelC2

in series

In parallel2

32

Page 21: L9 Ch29 Su15

Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

What you should read

Chapter 29 (Knight)

Sections 29.4 29.5

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Department of Physics and Applied Physics95.144, Summer 2015, Lecture 9

Thank youSee you tomorrow