unit 4 day 8 – ampere’s law & magnetic fields thru solenoids & toroids

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Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids Definition of Current Ampere’s Law Magnetic Field Inside & Outside a Current Carrying Conductor Magnetic Field of a Solenoid Magnetic Field of a Toroid

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Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids. Definition of Current Ampere’s Law Magnetic Field Inside & Outside a Current Carrying Conductor Magnetic Field of a Solenoid Magnetic Field of a Toroid. Definition of Current. - PowerPoint PPT Presentation

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Page 1: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

• Definition of Current

• Ampere’s Law

• Magnetic Field Inside & Outside a Current Carrying Conductor

• Magnetic Field of a Solenoid

• Magnetic Field of a Toroid

Page 2: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Definition of Current• The unit of current, Ampere, is defined in terms of the

magnetic field it produces

μ0 was originally measured experimentally

• To define μ0, a standard was created using two parallel wires, each with a current of I = 1.0 A, separated by a distance d = 1.0 m

AmTwhere

r

IB

70

0

104

2

Page 3: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Definition of Current

• The force between the wires per unit length is:

using μ0 = 4π x 10-7 T·m/A exactly

• Therefore, 1A, by definition, is the current flowing in each of 2 long parallel wires, resulting in a magnetic force of 2.0 x 10-7N/m

• Then, 1C = 1A·s, and the values of k & ε0 were then obtained experimentally

mN

d

II

l

F 7210 100.22

Page 4: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Ampere’s Law• Remembering that the magnetic field in a long, straight

current carrying conductor is:

• This equation is only valid for long straight wires. In general the relationship between current in a wire of any shape, and its magnetic field around it was derived by Andre Marie Ampere.

• For any arbitrary closed path around a current enclosed by the area of the closed path:

r

IB

20

enclIldB 0

Page 5: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Ampere’s Law

• Where the integrand is taken around any closed loop, and Iencl is the current passing through the area enclosed by the closed path

• For a straight conductor:

enclIldB 0

r

IB

rBdlBdlBI

2

2

0

0

Page 6: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Magnetic Field Inside & Outside a Current Carrying Conductor

• Outside the conductor, the magnetic field is an inverse law:

• Inside the conductor, the magnetic field is linear because the current is uniformly distributed

r

IB

IrBdlB

Rr

encl

2

2

0

0

20

2

2

0

0

2

2

2

2

R

IrB

R

rIrB

IdlB

R

rII

Rr

encl

encl

Page 7: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Magnetic Field Inside & Outside a Current Carrying Conductor

20

2 R

IrB

r

IB

20

Page 8: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Magnetic Field of a Solenoid• A solenoid is a long coil of wire made

of many (N) loops, each producing a magnetic field

• Inside the solenoid, the magnetic field is parallel to the long axis

• Outside the solenoid, the magnetic field is zero

• The magnetic field on-axis is:

l

NIB 0

Page 9: Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids

Magnetic Field of a Toroid• The magnetic field is confined to

being inside the ring only

• The magnetic field is not uniformly distributed inside the ring; it is largest along the inner edge of the ring, and smallest at the outer edge of the ring

• Outside the ring the magnetic field is zero

• The magnetic field is all inside the coil, made of N loops of wire

r

NIB

20