Physics II Chapter 26Department of Physics and Applied Physics Today we are going to discuss:...

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PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Lecture 10

Chapter 26

Capacitance

Physics II

My Capacitance is limited

Course website:https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Today we are going to discuss:

Chapter 26:

Section 26.2 The Geometry of Potential and Field Section 26.3 A Conductor in Electrostatic equilibrium Section 26.5 Capacitance and Capacitors

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Connecting Potential and Field (Review)

sdEVVVf

iif

We can find the potential difference between two points if we know the electric field.

dxdVEx

dydVEy

dzdVEz

Atwhichpointistheelectricfieldstronger?

A) AtxAB) AtxBC) Thefieldisthesamestrengthatboth

D)There’snotenoughinformationtotell

|E| = slope of potential graph

dxdVEx

At XA a slope is larger

ConcepTest E from the electric potential

Anelectronisreleasedfromrestatx=2minthepotentialshown.Whatdoestheelectrondorightafterbeingreleased?

A) Stayatx 2m

B)Movetotheright( x)atsteadyspeed

C)Movetotherightwithincreasingspeed

D)Movetotheleft(x)atsteadyspeed

E)Movetotheleftwithincreasingspeed

1) Slope of V negative => Ex is positive (field to the right).2) Electron is negative => force to the left.

3) Force to the left => acceleration to the left.

xEqxF

dxdVEx

maFx

a

ConcepTest My Favorite question

qEFx

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

The Geometry of Potential and Field

Let s be along an equipotential line, dsdVEs

where V=const. So dV=0. dsdVEs

0

0So, it is impossible to have an electric field along equipotential lines,

linesialequipotentE

equipotential lines

Whichsetofequipotentialsurfacesmatchesthiselectricfield?

A)

B)

C)

D)

E)

F)

E

ConcepTest Geometry E and V

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Potential of a Conductor

i

f

sdEVVVf

iif

0V if VV

Aconductorinelectrostaticequilibriumisatthesamepotential.

constV

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

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

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

CapacitorstoresenergyAcapacitorisasystemthatstorespotentialenergyinaformofanelectricfield.

Ugh!It’s just energy

Capacitor

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

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

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Parallel-plate capacitor

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

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Parallel-plate capacitor

Let’sfindcapacitanceofaparallel‐platecapacitor

Capacitanceisapurelygeometricpropertyoftwoelectrodesbecauseitdependsonlyontheirsurfaceareaandspacing.

E

d

Aarea

+Q–Q

Theelectricfieldbetweentheplatesisη ‐ surfacechargedensity

(Eq.25.26)Thepotentialdifferencebetweenplates:

WeneedtofindQandΔV:

≝ = 

Thisgivesthecapacitance:

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Parallel-plate capacitor

WecanincreasecapacitancebyincreasingareaAbymaking“arollofmetalandinsulator”

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Parallel-plate capacitor/keyboard

Capacitorsareimportantelementsinelectriccircuits.Theycomeinavarietyofsizesandshapes.

Thekeysonmostcomputerkeyboardsarecapacitorswitches.Pressingthekeypushestwocapacitorplatesclosertogether,increasingtheircapacitance.

Whatisthecapacitanceofthesetwoelectrodes?

A) 8 nF

B) 4 nF

C) 2 nF

D) 1 nF

E) Some other value

ConcepTest Capacitance

Sincethebatterystaysconnected,thepotential

differencemustremainconstant!+Q –Q

Aparallel‐platecapacitorinitiallyhasavoltageof400V andstaysconnectedtothebattery.Iftheplatespacingisnowdoubled, whathappens?

A)thevoltagedecreases

B)thevoltageincreases

C)thechargedecreases

D)thechargeincreases

E)bothvoltageandchargechange

ConcepTest Varying Capacitance I

Follow-up: How do you increase the charge?

Since,whenthespacingd isdoubled,

thecapacitanceC ishalved.Andsince,thatmeans

thechargemustdecrease.

Q =CΔV

400 V

Oncethebatteryisdisconnected,Q hastoremain

constant,sincenochargecanfloweithertoor

fromthebattery.

Aparallel‐platecapacitorinitiallyhasapotentialdifferenceof400V andisthendisconnectedfromthechargingbattery.Iftheplatespacingisnowdoubled,whatisthenewvalueofthevoltage?

A)100V

B)200V

C)400V

D)800V

E)1600V

+Q –Q

ConcepTest Varying Capacitance II

Since,whenthespacingd isdoubled,

thecapacitanceC ishalved.Andsince ,thatmeansthevoltagemustdouble

400 VQ =CΔV≝

PHYS.1440Lecture10 A.DanylovDepartmentofPhysicsandAppliedPhysics

Thank you