chapter 22 current and resistance. current conservation of current batteries resistance and...

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Chapter 22 Current and Resistance

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Page 2: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

• Current

• Conservation of current

• Batteries

• Resistance and resistivity

• Simple circuits

Chapter 22Current and Resistance

Topics:

Sample question:

How can the measurement of an electric current passed through a person’s body allow a determination of the percentage body fat?

Slide 22-1

Page 3: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

How can we control the flow of electric charges?

• Study the basic properties of current • Understand how our investigations of

static electricity relates to current.

Page 4: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Charged Parallel Plate Capacitor

• Connect the plates with a metal wire and the capacitor becomes discharged (neutral)

• The capacitor is discharged by a current in the connecting wire.

Page 5: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Properties of a Current

Slide 22-8

Indicators of Current in the Wire• Current is the motion of charges• Charges flow not current• Current is the flow

Page 6: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Charge Carriers

• Charge carriers are the charges that move in a current

• The charge carriers in metals are electrons.

Page 7: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Conduction Electrons in a Metal

Page 8: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Charge Carriers

• Insulator – does not have such free charges and cannot carry current

• Semiconductor – intermediate case – few charge carriers which can be either positive or negative ions

• Examples of ionic solutions as charge carriers – seawater, blood, intercellular fluids

Page 9: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Creating a Current

• We use an electric field to “push” on the electrons in in a conductor similarly to pushing a book on a table to give it kinetic energy

• When we apply an electric field the field exerts a force on the electrons and they begin to move.

Page 10: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Motion of electrons

• Kinetic energy of collisions in converted to thermal energy

• The metal gets warmer

Page 11: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Sustaining the current

• You must continue the push or the electrons will stop moving

• Maintain an electric field• Drift Velocity - Electron’s average motion

is opposite the field• If the field goes to zero then the drift

velocity goes to zero.• A current is a motion of charges sustained

by an internal electric field

Page 12: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Where does the electric field come from in a current carrying wire?

• A potential difference creates a current in the wire.

• Electric potential energy Uelec is energy stored in a system of charged particles due to their electrical interactions.

• The energy transfer Δ Uelec

• The potential is measured in volts

Page 13: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Creating Potential

• Electrons are bumped and pushed along• The E field has some strength in N/C• This is similar to the strength of a

gravitational field in N/kg. (9.8N/kg)• Think about gravitational potential energy

being mgh and electrical potential energy being qEd

Page 14: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Creating Potential

• Uelec = qEd energy stored in a particle• Ug = mgh energy stored by height• E d = J/C =ΔV energy independent of

charge• gh =J/kg• We care about the change in potential• Protons go from high to low potential• Electrons got from low to high potential

Page 15: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Creating Potential

• In reality the electrons are moving• A battery adds energy • Think about an energy elevator.• A 1.5 V battery is like a charge escalator • The battery reenergizes the particle• The volt is the unit of potential• Voltage is the difference in potential• A particle uses all of its potential in a circuit

Page 16: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Simple Circuits

The current is determined by the potential difference and the resistance of the wire:

Slide 22-13

I =∆Vchem

R_____

Page 17: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Batteries

The potential difference between the terminals of a battery, often called the terminal voltage, is the

battery’s emf.

Slide 22-12

∆Vbat = = Wchem

q____

Page 18: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Difference in Potential creates current

Page 19: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Capacitor

• The potential difference across the capacitor depends on the capacitor’s charge.

• The potential difference (and the current) steadily falls as the capacitor discharges

• When the capacitor is fully discharged there is no longer a potential difference and the current ceases

Page 20: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Conservation of Current• Add a lightbulb

between two capacitors

• How does the current at A compare to current at B/

• They are the same

Page 21: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Conservation of Current

• The number of electrons is not changed by the lightbulb

• The lightbulb cannot

destroy electrons• The lightbulb can’t store

electrons• It does use energy

Page 22: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Law of Conservation of Current

• The current is the same at all points in a current carrying wire

Page 23: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Definition of a Current

Slide 22-9

Page 24: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Current

• Current is a rate• The current direction in a wire is from

higher potential to lower potential (in the direction of the electric field)

• Unit is ampere • 1ampere = 1 coulomb per second = 1C/s

Page 25: Chapter 22 Current and Resistance. Current Conservation of current Batteries Resistance and resistivity Simple circuits Chapter 22 Current and Resistance

Conservation of Current

Slide 22-10