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Feb 15 2002 Electricity and Magnetism • Electric field continued

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Page 1: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Electricity and Magnetism

• Electric field continued

Page 2: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Electric Field

• New concept – Electric Field E• Charge Q gives rise to a Vector Field

• E is defined by strength and direction of force on small test charge q

Page 3: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Electric Field

• For a single charge

• Visualize using Field Lines– Cartoon!– Strength -> Density of Lines– Direction -> Direction of Lines

• away from positive charges

+Q

Page 4: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Electric Field

• Field can be used to accelerate charged particles

F = Q E-> Particle Accelerators

Page 5: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

The Electric Field

• Electric Field also exists is test charge q is not present

• We can say:The charge Q gives rise to a property of space itself – the Electric Field

-> In-Class Demo...

Page 6: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Electric Field Demo

• Use a Van-der-Graaf Generator• Much more powerful than rubbing glass rods• Not really dangerous (I’ve been told) – but

potentially painful• Creates large electric fields• Really big ones were used in Particle

Accelerators (still in use in some labs)

Page 7: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Page 8: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Torque τ = p x Ep = Q l Dipolemoment

Page 9: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Does Dipole feel a net Force?

No Yes

Page 10: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Superposition Principle

• Field of many charges is Vector Sum of individual fields

Page 11: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Example: Superposition principle for 3 charges

x

y

+L

-L

+

+

+

0

Q1

Q2

Q3

x0

E1

E2

E3r1

r2

r3)

Page 12: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Example: Superposition principle for continouscharge distribution

x

y

+L

-L

0 x0

Total Charge Q = 2 λ L

dE

dQ = λ dy

r

Page 13: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

Example: Superposition principle for continouscharge distribution

x

y

+L

-L

0 x0

Total Charge Q = 2 λ L

dE

dQ = λ dy

r

Page 14: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

More on Fields and Field Lines

• What’s wrong with this picture?• Magnitude and direction of field have to be

unique at each point!• Field lines can’t cross!

E

Page 15: Electricity and Magnetism - MIT OpenCourseWare...Electricity and Magnetism • Electric field continued Feb 15 2002 Electric Field • New concept – Electric Field E • Charge Q

Feb 15 2002

More on Fields and Field Lines

• Very close to surface of charged object• Field lines perpendicular to surface (if we go

close enough)! • Symmetry left and right (like an infinite plane)

+ + ++++ + + +