coulomb ’ s law, e fields

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COULOMB’S LAW, E FIELDS

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COULOMB ’ S LAW, E FIELDS. Class Activities Coulomb ’ s Law. Class Activities: Charge Distibutions. Two charges +Q and -Q are fixed a distance r apart. The direction of the force on a test charge -q at A is…. Up Down Left Right Some other direction, or F =0. - PowerPoint PPT Presentation

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Page 1: COULOMB ’ S LAW, E FIELDS

COULOMB’S LAW, E FIELDS

Page 2: COULOMB ’ S LAW, E FIELDS

Class ActivitiesCoulomb’s Law

Page 3: COULOMB ’ S LAW, E FIELDS

Class Activities: Charge Distibutions

Page 4: COULOMB ’ S LAW, E FIELDS

Two charges +Q and -Q are fixed a distance r apart. The direction of the force on a test charge -q at A is…

A.UpB.DownC.LeftD.RightE.Some other direction,

or F =0

Page 5: COULOMB ’ S LAW, E FIELDS

Two charges +q and -q are on the y-axis, symmetric about the origin. Point A is an empty point in space on the x-axis. The direction of the E field at A is…A.UpB.DownC.LeftD.RightE.Some other direction, or E = 0, or ambiguous

2.3

+q

x

y

-q

A

Page 6: COULOMB ’ S LAW, E FIELDS

How is the vector related to r1 and r2?

r2

r1

2.1b

Page 7: COULOMB ’ S LAW, E FIELDS

Coulomb's law:

In the fig, q1 and q2 are 2 m apart. Which arrow can represent ?

q1 q2

A

B C

D) More than one (or NONE) of the aboveE) You can't decide until you know if q1 and q2 are the same or opposite signed charges

Page 8: COULOMB ’ S LAW, E FIELDS

What is ("from 1 to the point r") here?

+qr1=(x1,y1) -q

r=(x,y)

2.2

Page 9: COULOMB ’ S LAW, E FIELDS

Only click when you are DONE with page 1 (Part 1 i-iii)

Is the answer to part 1- iiiA) A sum?B) An integral over dy?C) An integral over something else?

Page 10: COULOMB ’ S LAW, E FIELDS

Tutorial 1, part 2- Script rOnly after you finish Part 2, what is in part 2-iv ?

E) None of these!

Page 11: COULOMB ’ S LAW, E FIELDS

5 charges, q, are arranged in a regular pentagon, as shown. What is the E field at the center?

A) ZeroB) Non-zeroC) Really need trig and a calculator to

decide

q

q

qq

q

2.5

Page 12: COULOMB ’ S LAW, E FIELDS

1 of the 5 charges has been removed, as shown. What’s the E field at the center?

q

qq

q

A) +(kq/a2) jB) -(kq/a2) jC) 0D) Something entirely different!E) This is a nasty problem which I need more

time to solve

+x

+ya

2.6

Page 13: COULOMB ’ S LAW, E FIELDS

To find the E- field at P=(x,y,z) from a thin line (uniform linear charge density ):

What is ?

A) X B) y'

C) D)

E) Something completely different!!

P=(x,0,0)x

y

dl'r'

r

2.10

Page 14: COULOMB ’ S LAW, E FIELDS

P=(x,0,0)x

y

dl'r'=(0,y',0)

r

2.11

Page 15: COULOMB ’ S LAW, E FIELDS

,so

P=(x,0,0)x

y

dl'r'=(0,y',0)

r

2.11

Page 16: COULOMB ’ S LAW, E FIELDS

To find the E- field at P from a thin ring (radius R, uniform linear charge density ):

what is ?

P=(0,0,z)

R xy dl'

B

E) NONE of the arrows shown correctly represents

A CD

2.12

Page 17: COULOMB ’ S LAW, E FIELDS

To find the E- field at P from a thin ring (radius a, uniform linear charge density ):

what is ?A)

B) a

C) D) z

E) Something completely different!!

P=(0,0,z)

a x

y dl'

2.13

Page 18: COULOMB ’ S LAW, E FIELDS

Griffiths p. 63 finds E a distance z from a line segment with charge density :

What is the approx. form for E, if z>>L?

A) 0 B) 1 C) 1/z D) 1/z^2 E) None of these is remotely correct.

x

(0,0,z)

-L +L

2.16

Page 19: COULOMB ’ S LAW, E FIELDS

Griffiths p. 63 finds E a distance z from a line segment with charge density :

What is the approx. form for E, if z<<L?

A) 0 B) 1 C) 1/z D) 1/z^2 E) None of these is remotely correct.

x

(0,0,z)

-L +L

2.16

Page 20: COULOMB ’ S LAW, E FIELDS

D) None of these

To find E at P from a negatively charged sphere (radius R, uniform volume charge density ) using

what is (given the small volume element shown)? P=(x,y,z)

x

yz(x’,y’,z’)

R A

BC

2.14

Page 21: COULOMB ’ S LAW, E FIELDS

A)

B)

C)

D) E) None of these

P=(X,Y,Z)

X,Y,Z

(X x)2

(Y y)2

(Z z)2

dxdydz

X,Y,Z (X x)2 (Y y)2 (Z z)2 3/2

dxdydz

X x,Y y,Z z

(X x)2

(Y y)2

(Z z)2

dxdydz

X x,Y y,Z z (X x)2 (Y y)2 (Z z)2 3/2

dxdydz

140

(....?)

x

yz(x,y,z)

R

2.15

dq

Page 22: COULOMB ’ S LAW, E FIELDS

A)

B)

C)

D) E) None of these

P=(X,Y,Z)

X,Y,Z

(X x)2

(Y y)2

(Z z)2

dxdydz

X,Y,Z (X x)2 (Y y)2 (Z z)2 3/2

dxdydz

X x,Y y,Z z

(X x)2

(Y y)2

(Z z)2

dxdydz

X x,Y y,Z z (X x)2 (Y y)2 (Z z)2 3/2

dxdydz

140

(....?)

x

yz(x,y,z)

R

2.15