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Current and Resistance Tuesday, July 19, 2011

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Page 1: Current

Current and Resistance

Tuesday, July 19, 2011

Page 2: Current

Current

Convention : Current depicts flow of positive (+) charges

Tuesday, July 19, 2011

Page 3: Current

Current

+

Area

Convention : Current depicts flow of positive (+) charges

Tuesday, July 19, 2011

Page 4: Current

Current

+

Area

Ammeter(measures current)

Convention : Current depicts flow of positive (+) charges

Tuesday, July 19, 2011

Page 5: Current

Current

+

Area

Ammeter(measures current)

+

+

Convention : Current depicts flow of positive (+) charges

Tuesday, July 19, 2011

Page 6: Current

Current

+

Area

Ammeter(measures current)

+

+

Convention : Current depicts flow of positive (+) charges

Tuesday, July 19, 2011

Page 7: Current

Current

A measure of how much charge passes through an amount of time

Ammeter(measures current)

++

+

Tuesday, July 19, 2011

Page 8: Current

Current

++

+

Count how many charges flow through

Tuesday, July 19, 2011

Page 9: Current

Current

++

+

Expand surface to a volumeCount how many charges flow through

Tuesday, July 19, 2011

Page 10: Current

Current

++

+

Expand surface to a volume

Area = A

Count how many charges flow through

Tuesday, July 19, 2011

Page 11: Current

Current

++

+

Expand surface to a volume

Area = A length = Δx

Count how many charges flow through

Tuesday, July 19, 2011

Page 12: Current

Current

++

+

Expand surface to a volume

Total volumeV = (A)(Δx)

length = ΔxArea = A

Count how many charges flow through

Tuesday, July 19, 2011

Page 13: Current

Current

++

+

Expand surface to a volume

Total volumeV = (A)(Δx)

length = ΔxArea = A

Number of charges = (charge density or charge per volume)*(volume)Number of charges = (n) * (AΔx)

Count how many charges flow through

Tuesday, July 19, 2011

Page 14: Current

Current

++

+

Expand surface to a volume

Total volumeV = (A)(Δx)

length = ΔxArea = A

Number of charges = (n) * (AΔx)

Total amount of charge = (number of charges)*(charge)ΔQ = (n A Δx)*(q)

Count how many charges flow through

Number of charges = (charge density or charge per volume)*(volume)

Tuesday, July 19, 2011

Page 15: Current

Current

++

+ Total volumeV = (A)(Δx)

length = ΔxArea = A

ΔQ = (n A Δx)*(q)

Tuesday, July 19, 2011

Page 16: Current

Current

++

+ Total volumeV = (A)(Δx)

length = Δx = vd ΔtArea = A

ΔQ = (n A Δx)*(q)but charges have drift velocity vd = Δx/Δt

Tuesday, July 19, 2011

Page 17: Current

Current

++

+ Total volumeV = (A)(Δx)

Area = A

ΔQ = (n A vd Δt)*(q)

but charges have drift velocity vd = Δx/Δt

length = Δx = vd Δt

ΔQ = (n A Δx)*(q)

Tuesday, July 19, 2011

Page 18: Current

Current

++

+ Total volumeV = (A)(Δx)

Area = A

ΔQ/Δt = (n A vd)*(q)

I = n q vd A

but charges have drift velocity vd = Δx/Δt

length = Δx = vd Δt

ΔQ = (n A vd Δt)*(q)

ΔQ = (n A Δx)*(q)

Tuesday, July 19, 2011

Page 19: Current

Current

This is the reason why large wires are needed to support large currents

Tuesday, July 19, 2011

Page 20: Current

Current

This is the reason why large wires are needed to support large currents

Tuesday, July 19, 2011

Page 21: Current

Resistance

Current density (J)current per area

Tuesday, July 19, 2011

Page 22: Current

Resistance

Current density (J)current per area

Direction of current (flow of positive charges) is same with direction of electric field

Tuesday, July 19, 2011

Page 23: Current

Resistance

Current density (J)current per area

Direction of current (flow of positive charges) is same with direction of electric field

conductivity

Tuesday, July 19, 2011

Page 24: Current

Resistance

Current density (J)current per area

Direction of current (flow of positive charges) is same with direction of electric field

conductivity (material property)

resistivity (material property)

Tuesday, July 19, 2011

Page 25: Current

Resistance

Current density (J)current per area

Direction of current (flow of positive charges) is same with direction of electric field

conductivity

resistivity

Current is proportional to conductivity but inversely proportional to resistivity!

Tuesday, July 19, 2011

Page 26: Current

Resistance

Current is proportional to conductivity but inversely proportional to resistivity!

Tuesday, July 19, 2011

Page 27: Current

Resistance

Current is proportional to conductivity but inversely proportional to resistivity!Current is proportional to the electric potential(specifically potential difference)

Tuesday, July 19, 2011

Page 28: Current

Resistance

Current is proportional to conductivity but inversely proportional to resistivity!Current is proportional to the electric potential(specifically potential difference)

Ohm’s LawResistancePotential difference

current

Tuesday, July 19, 2011

Page 29: Current

Resistance

Current is proportional to conductivity but inversely proportional to resistivity!Current is proportional to the electric potential(specifically potential difference)

Ohm’s Law

a much better form than ΔV = I R

ResistancePotential difference

current

Tuesday, July 19, 2011

Page 30: Current

Resistance

Current is proportional to conductivity but inversely proportional to resistivity!Current is proportional to the electric potential(specifically potential difference)

Ohm’s LawResistancePotential difference

current

a much better form than ΔV = I R

Increasing ΔV increases IIncreasing R decreases I

Tuesday, July 19, 2011

Page 31: Current

Resistance

Current is proportional to conductivity but inversely proportional to resistivity!Current is proportional to the electric potential(specifically potential difference)

Ohm’s LawResistancePotential difference

current

a much better form than ΔV = I R

Increasing ΔV increases IIncreasing R decreases I

ΔV = I R Increasing R does not increase ΔVCurrent (I) is increased because ΔV is increased

Tuesday, July 19, 2011

Page 32: Current

Resistance

Tuesday, July 19, 2011

Page 33: Current

Resistance

Important points:

same with capacitance, resistance does not depend on ΔV and I

Resistance depends on material property resistivity ρ, length of wire l and cross sectional area A

direction of the current I is same as direction of electric field

conventional current is flowing positive (+) charges though in reality electrons flow

Tuesday, July 19, 2011

Page 34: Current

Recent Equations

I =∆V

R

R =ρl

A

→J = σ

→E =

→E

ρ

→J =

→I

A

→J = nq

→v dA

Tuesday, July 19, 2011

Page 35: Current

Exercise

Rank from lowest to highest amount of current

Derive the equation R = ρL/Afrom V = IR, J = E/ρ = I/A, V = EL

Tuesday, July 19, 2011

Page 36: Current

Resistance and Temperature

∆T = T − T0

T0 is usually taken to be 25 °C

ρ = ρ0(1 + α∆T )

R =ρl

A

T ↑ ρ ↑

Tuesday, July 19, 2011

Page 37: Current

Power

P =∆U

∆t

P =∆(q∆V )

∆t

P =(∆q)(∆V )

∆t

P =∆q

∆t∆V

P = I∆V

Tuesday, July 19, 2011

Page 38: Current

Power

P = I∆V

I =∆V

R

P =V 2

RP = I2R

Tuesday, July 19, 2011

Page 39: Current

End of Chapter Exercises

An aluminum wire having a cross-sectional area of 4.00 x 10-6 m2 carries a current of 5.00 A. Find the drift speed of the electrons in the wire. The density of aluminum is 2700 kg/m3. Assume that one conduction electron is supplied by each atom.Molar mass of Al is 27 g/mol.

The electron beam emerging from a certain high-energy electron accelerator has a circular cross section of radius 1.00 mm. (a) The beam current is 8.00 µA. Find the current density in the beam, assuming that it is uniform throughout. (b) The speed of the electrons is so close to the speed of light that their speed can be taken as c = 3.00 x 108 m/s with negligible error. Find the electron density in the beam. (c) How long does it take for Avogadroʼs number of electrons to emerge from the accelerator?

Three wires A, B, C and D are made of the same material but of different lengths and radii. Wire A has length L but has radius R. Wire B has length 2L but with radius ½R. Wire C has length ½L but with radius 2R. Wire D has length ½L but with radius ½R.

Rank with increasing resistance

A 0.900-V potential difference is maintained across a 1.50-m length of tungsten wire that has a cross-sectional area of 0.600 mm2. What is the current in the wire?resistivity of tungsten is 5.6 x 10-8 Ω-m

Tuesday, July 19, 2011