week 4 - physics courses...for path #3, you are moving in a direction perpendicular to the field...

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Page 1: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

week 4

Page 2: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by
Page 3: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by
Page 4: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by
Page 5: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Which requires the most

work, to move a positive

charge from P to points 1, 2,

3 or 4 ? All points are the

same distance from P.

1) P → 1

2) P → 2

3) P → 3

4) P → 4

5) all require the same amount of work

P1

2

3

4

Page 6: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

For path #1, you have to push the positive charge against the E field, which is hard to do. By contrast, path #4 is the easiest, since the field does all the work.

Which requires the most

work, to move a positive

charge from P to points 1, 2,

3 or 4 ? All points are the

same distance from P.

1) P → 1

2) P → 2

3) P → 3

4) P → 4

5) all require the same amount of work

P1

2

3

4

Page 7: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Which requires zero work, to

move a positive charge from

P to points 1, 2, 3 or 4? All

points are the same distance

from P.

1) P → 1

2) P → 2

3) P → 3

4) P → 4

5) all require the same amount of work

P1

2

3

4

Page 8: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by definition).

1) P → 1

2) P → 2

3) P → 3

4) P → 4

5) all require the same amount of work

P1

2

3

4

Follow-up: Which path requires the least work?

Which requires zero work, to

move a positive charge from

P to points 1, 2, 3 or 4? All

points are the same distance

from P.

Page 9: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

The positive charge is the end view

of a positively charged glass rod. A

negatively charged particle moves in

a circular arc around the glass rod.

Is the work done on the charged

particle by the rod’s electric field

positive, negative or zero?

1. Positive

2. Negative

3. Zero

Page 10: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

The positive charge is the end view

of a positively charged glass rod. A

negatively charged particle moves in

a circular arc around the glass rod.

Is the work done on the charged

particle by the rod’s electric field

positive, negative or zero?

1. Positive

2. Negative

3. Zero

Page 11: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

When a positive charge moves in the direction of the electric field,

1. the field does positive work on it and the potential energy increases

2. the field does positive work on it and the potential energy decreases

3. the field does negative work on it and the potential energy increases

4. the field does negative work on it and the potential energy decreases

Page 12: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

When a positive charge moves in the direction of the electric field,

1. the field does positive work on it and the potential energy increases

2. the field does positive work on it and the potential energy decreases

3. the field does negative work on it and the potential energy increases

4. the field does negative work on it and the potential energy decreases

The work done by the field is

dW = qE ⋅dr In this case the vectors E and dr are parallel and the charge is positive so dW >0The change in potential energy is the negtive of the work done by the field, so

ΔU = - W <0

Page 13: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

When a negative charge moves in the direction of the electric field,

1. the field does positive work on it and the potential energy increases

2. the field does positive work on it and the potential energy decreases

3. the field does negative work on it and the potential energy increases

4. the field does negative work on it and the potential energy decreases

Page 14: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

When a negative charge moves in the direction of the electric field,

1. the field does positive work on it and the potential energy increases

2. the field does positive work on it and the potential energy decreases

3. the field does negative work on it and the potential energy increases

4. the field does negative work on it and the potential energy decreases

The work done by the field is

dW = qE ⋅dr In this case the vectors E and dr are parallel and the charge is negative so dW <0The change in potential energy is the negtive of the work done by the field, so

ΔU = - W >0

Page 15: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) proton

2) electron

3) both feel the same force

4) neither – there is no force

5) they feel the same magnitude force but opposite direction

A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the electron from the negative side. Which feels the larger electric force?

electron

proton

electron

proton+

-

Page 16: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) proton

2) electron

3) both feel the same force

4) neither – there is no force

5) they feel the same magnitude force but opposite direction

Since F = qE and the proton and electron

have the same charge in magnitude, they

both experience the same force. However,

the forces point in opposite directions

because the proton and electron are

oppositely charged.

A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the electron from the negative side. Which feels the larger electric force?

electron

proton

electron

proton+

-

Page 17: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) proton

2) electron

3) both feel the same acceleration

4) neither – there is no acceleration

5) they feel the same magnitude acceleration but opposite direction

A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the electron from the negative side. Which has the larger acceleration?

electron

proton

electron

proton+

-

Page 18: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) proton

2) electron

3) both feel the same acceleration

4) neither – there is no acceleration

5) they feel the same magnitude acceleration but opposite direction

Since F = ma and the electron is much less

massive than the proton, then the electron

experiences the larger acceleration.

A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the electron from the negative side. Which has the larger acceleration?

electron

proton

electron

proton+

-

Page 19: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) proton

2) electron

3) both acquire the same KE

4) neither – there is no change of KE

5) they both acquire the same KE but with opposite signs

A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the electron from the negative side. When it strikes the opposite plate, which one has more KE?

electron

proton

electron

proton+

-

Page 20: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) proton

2) electron

3) both acquire the same KE

4) neither – there is no change of KE

5) they both acquire the same KE but with opposite signs

Since PE = qV and the proton and electron

have the same charge in magnitude, they

both have the same electric potential energy

initially. Because energy is conserved, they

both must have the same kinetic energy after

they reach the opposite plate.

A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the electron from the negative side. When it strikes the opposite plate, which one has more KE?

electron

proton

electron

proton+

-

Page 21: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Here is a simple problem we already know how to solve using forces and F=ma.But let’s solve it using conservation of energy:

The electric field strength is 50,000 N/C inside a parallel plate capacitor with a 2.0 mm spacing. A proton is released form rest at the positive plate. What is the proton’s speed when it reaches the negative plate?

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Ans: 1.38 x 105 m/s

Page 22: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Rank in order, from largest to smallest, the potential energies Ua to Ud of these four pairs of charges. Each + symbol represents the same amount of charge.

• 1. Ua = Ub = Uc = Ud

• 2. Ud = Ub > Uc = Ua

• 3. Ud > Ub = Uc > Ua

• 4. Ub > Ua > Ud > Uc

• 5. Ud > Ub = Uc > Ua

Page 23: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Rank in order, from largest to smallest, the potential energies Ua to Ud of these four pairs of charges. Each + symbol represents the same amount of charge.

• 1. Ua = Ub = Uc = Ud

• 2. Ud = Ub > Uc = Ua

• 3. Ud > Ub = Uc > Ua

• 4. Ub > Ua > Ud > Uc

• 5. Ud > Ub = Uc > Ua

Ua = kq2

rUb = k

2q2

rUc = k

(2q)q2r

= kq2

rUd = k

(2q)(2q)2r

= 2kq2

r

Page 24: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

The electric potential energy of two point charges approaches zero as the two point charges move farther away from each other.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential energy of the system of three charges is

1. positive

2. negative

3. zero

4. not enough information given to decide

Page 25: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

The electric potential energy of two point charges approaches zero as the two point charges move farther away from each other.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential energy of the system of three charges is

1. positive

2. negative

3. zero

4. not enough information given to decide

If the length of the side of the triangle is d, then

U = k ( q*q/d + q(-q)/d +q(-q)/d ) = - kq2/d < 0

Page 26: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Which group of charges took more work to bring together from a very large initial distance apart?

1

+1

+1

+1

d d

d

2+1+2

d

3 Both took the same amount of work

Page 27: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

The work needed to assemble a collection of charges is the same as the total PE of those charges:

Which group of charges took more work to bring together from a very large initial distance apart?

1

+1

+1

+1

d d

d

2+1+2

d

3 Both took the same amount of work

For case 1: only 1 pair

For case 2: there are 3 pairsadded over

all pairs

Page 28: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

These four 1.0 g spheres are released simultaneously and allowed to move away from each other. What is the speed of each sphere when they are very far apart?

Ans (if needed, see next page): 0.49 m/s

Page 29: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

These four 1.0 g spheres are released simultaneously and allowed to move away from each other. What is the speed of each sphere when they are very far apart?

1 2

3 4

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6 69 <.H <H !A& ;K.L@ <H !M H.;:!CP)' '$ $' ! ' . ! !

!

Final energy is pure kinetic energy:

!"#$%#! &'()*+! "#$%&'!()!*+#)$%,$-.!/0$!*01%&$-!)20$%$)!1%$!2+(#3!*01%&$).!

,-./0*-1)+! 45$1)$! %$6$%! 3+! 7(&8%$! 49:.;<.! =1>$5! 30$! )20$%$)! <?! 9?! @?! 1#-! ;! (#! 1! *5+*AB()$!C1##$%?! B(30! 30$!

)20$%$!(#!30$!822$%!5$63D01#-!*+%#$%!>$(#&!)20$%$!<.!

2'*3)+! /0$!3+315!2+3$#3(15!$#$%&'!+6!30$!6+8%!)20$%$)!>$6+%$!30$'!1%$!155+B$-!3+!C+,$!()!

!"!!!E!<9!"!!9@!"!!@;!"!!;<F!"!E!<@!"!!9;F!

G55!30$!*01%&$)!1%$!(-$#3(*15?!#<9!!!#9@!!!#@;!!!#;<!!!<.H!*C?!1#-! <@ 9; 9.H !*C.# #! ! !/0$!(#(3(15!2+3$#3(15!$#$%&'!()!

: : : :I

(

H H

< <H <H !JFE<H <H !JF < <H <H !JFE<H <H !JF; 9 ;K.L@ <H !M; H.H<H!C ; H.H<;<;!C

!$ $# #

$ $ $ $$% & % &' ' ' '

! " ! '( ) ( )* + * +

!

N(#*$!155!*01%&$)!1%$!13!%$)3?!%"!!!H!M.!G)!30$!)20$%$)!1%$!155+B$-!3+!C+,$!1B1'!6%+C!+#$!1#+30$%!1#-!30$'!1%$!61%!121%3?!!6!!!H!M.!/0$!6(#15!A(#$3(*!$#$%&'!()!

9 @ 9<6 6 69;E F 9E<.H <H !A&F,% &'

$! ! ' !

7%+C!30$!$#$%&'!*+#)$%,13(+#!$O813(+#!!6!"!%6!!!!(("(%(?!

, -@ 9 I

6 69 <.H <H !A& ;K.L@ <H !M H.;:!CP)' '$ $' ! ' . ! !

!

!"#$%#! &'()*+! "#$%&'!()!*+#)$%,$-.!/0$!*01%&$-!)20$%$)!1%$!2+(#3!*01%&$).!

,-./0*-1)+! 45$1)$! %$6$%! 3+! 7(&8%$! 49:.;<.! =1>$5! 30$! )20$%$)! <?! 9?! @?! 1#-! ;! (#! 1! *5+*AB()$!C1##$%?! B(30! 30$!

)20$%$!(#!30$!822$%!5$63D01#-!*+%#$%!>$(#&!)20$%$!<.!

2'*3)+! /0$!3+315!2+3$#3(15!$#$%&'!+6!30$!6+8%!)20$%$)!>$6+%$!30$'!1%$!155+B$-!3+!C+,$!()!

!"!!!E!<9!"!!9@!"!!@;!"!!;<F!"!E!<@!"!!9;F!

G55!30$!*01%&$)!1%$!(-$#3(*15?!#<9!!!#9@!!!#@;!!!#;<!!!<.H!*C?!1#-! <@ 9; 9.H !*C.# #! ! !/0$!(#(3(15!2+3$#3(15!$#$%&'!()!

: : : :I

(

H H

< <H <H !JFE<H <H !JF < <H <H !JFE<H <H !JF; 9 ;K.L@ <H !M; H.H<H!C ; H.H<;<;!C

!$ $# #

$ $ $ $$% & % &' ' ' '

! " ! '( ) ( )* + * +

!

N(#*$!155!*01%&$)!1%$!13!%$)3?!%"!!!H!M.!G)!30$!)20$%$)!1%$!155+B$-!3+!C+,$!1B1'!6%+C!+#$!1#+30$%!1#-!30$'!1%$!61%!121%3?!!6!!!H!M.!/0$!6(#15!A(#$3(*!$#$%&'!()!

9 @ 9<6 6 69;E F 9E<.H <H !A&F,% &'

$! ! ' !

7%+C!30$!$#$%&'!*+#)$%,13(+#!$O813(+#!!6!"!%6!!!!(("(%(?!

, -@ 9 I

6 69 <.H <H !A& ;K.L@ <H !M H.;:!CP)' '$ $' ! ' . ! !

!

Use conservation of energy:!"#$%#! &'()*+! "#$%&'!()!*+#)$%,$-.!/0$!*01%&$-!)20$%$)!1%$!2+(#3!*01%&$).!

,-./0*-1)+! 45$1)$! %$6$%! 3+! 7(&8%$! 49:.;<.! =1>$5! 30$! )20$%$)! <?! 9?! @?! 1#-! ;! (#! 1! *5+*AB()$!C1##$%?! B(30! 30$!

)20$%$!(#!30$!822$%!5$63D01#-!*+%#$%!>$(#&!)20$%$!<.!

2'*3)+! /0$!3+315!2+3$#3(15!$#$%&'!+6!30$!6+8%!)20$%$)!>$6+%$!30$'!1%$!155+B$-!3+!C+,$!()!

!"!!!E!<9!"!!9@!"!!@;!"!!;<F!"!E!<@!"!!9;F!

G55!30$!*01%&$)!1%$!(-$#3(*15?!#<9!!!#9@!!!#@;!!!#;<!!!<.H!*C?!1#-! <@ 9; 9.H !*C.# #! ! !/0$!(#(3(15!2+3$#3(15!$#$%&'!()!

: : : :I

(

H H

< <H <H !JFE<H <H !JF < <H <H !JFE<H <H !JF; 9 ;K.L@ <H !M; H.H<H!C ; H.H<;<;!C

!$ $# #

$ $ $ $$% & % &' ' ' '

! " ! '( ) ( )* + * +

!

N(#*$!155!*01%&$)!1%$!13!%$)3?!%"!!!H!M.!G)!30$!)20$%$)!1%$!155+B$-!3+!C+,$!1B1'!6%+C!+#$!1#+30$%!1#-!30$'!1%$!61%!121%3?!!6!!!H!M.!/0$!6(#15!A(#$3(*!$#$%&'!()!

9 @ 9<6 6 69;E F 9E<.H <H !A&F,% &'

$! ! ' !

7%+C!30$!$#$%&'!*+#)$%,13(+#!$O813(+#!!6!"!%6!!!!(("(%(?!

, -@ 9 I

6 69 <.H <H !A& ;K.L@ <H !M H.;:!CP)' '$ $' ! ' . ! !

!

Page 30: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

A proton is released from

rest at point B, where the

potential is 0 V.

Afterward, the proton

1. moves toward A with an increasing speed.

2. moves toward A with a steady speed.

3. remains at rest at B.

4. moves toward C with a steady speed.

5. moves toward C with an increasing speed.

Page 31: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

A proton is released from

rest at point B, where the

potential is 0 V.

Afterward, the proton

1. moves toward A with an increasing speed.

2. moves toward A with a steady speed.

3. remains at rest at B.

4. moves toward C with a steady speed.

5. moves toward C with an increasing speed.

Page 32: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Rank in order, from largest to

smallest, the potentials Va to

Ve at the points a to e.

1. Va = Vb = Vc = Vd = Ve

2. Va = Vb > Vc > Vd = Ve

3. Vd = Ve > Vc > Va = Vb

4. Vb = Vc = Ve > Va = Vd

5. Va = Vb = Vd = Ve > Vc

Page 33: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Rank in order, from largest to

smallest, the potentials Va to

Ve at the points a to e.

1. Va = Vb = Vc = Vd = Ve

2. Va = Vb > Vc > Vd = Ve

3. Vd = Ve > Vc > Va = Vb

4. Vb = Vc = Ve > Va = Vd

5. Va = Vb = Vd = Ve > Vc

Page 34: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

An AA battery is connected to a parallel plate capacitor having 4.0-cm-diameter plates spaced 2.0 mm apart. How much charge does the battery supply to each plate?

Ans: 8.3 x 10-12 C

Page 35: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) V > 0

2) V = 0

3) V < 0

What is the electric potential at point A?

A B

Page 36: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Since Q2 (which is positive) is closer

to point A than Q1 (which is negative)

and since the total potential is equal to V1 + V2, then the total potential is

positive.

1) V > 0

2) V = 0

3) V < 0

What is the electric potential at point A?

A B

Page 37: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) V > 0

2) V = 0

3) V < 0

What is the electric potential at point B?

A B

Page 38: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Since Q2 and Q1 are equidistant

from point B, and since they have equal and opposite charges, then the total potential is zero.

1) V > 0

2) V = 0

3) V < 0

What is the electric potential at point B?

Follow-up: What is the potential at the origin of the x-y axes?

A B

Page 39: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Consider a point P in

space where the electric

potential is zero. Which

statement is correct?

1. a point charge placed at P would feel no electric force

2. the electric field at points around P is directed toward P

3. the electric field at points around P is directed away from P

4. none of the above

5. not enough information given to decide

Page 40: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Consider a point P in

space where the electric

potential is zero. Which

statement is correct?

1. a point charge placed at P would feel no electric force

2. the electric field at points around P is directed toward P

3. the electric field at points around P is directed away from P

4. none of the above

5. not enough information given to decide

The value of the electric potential at any one point in space is arbitrary. Only differences in electric potential have physical significance.

Page 41: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

The electric potential due to a point charge approaches zero as you move farther away from the charge.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential at the center of the triangle is

1. positive

2. negative

3. zero

4. not enough information given to decide

Page 42: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

The electric potential due to a point charge approaches zero as you move farther away from the charge.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential at the center of the triangle is

1. positive

2. negative

3. zero

4. not enough information given to decide

If the distance from any charge tothe center of the triangle is d, then

V = k ( q/d + q/d -q/d ) = kq/d > 0

Page 43: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Four point charges are

arranged at the corners

of a square. Find the

electric field E and the

potential V at the center

of the square.

1) E = 0 V = 0

2) E = 0 V ≠ 0

3) E ≠ 0 V ≠ 0

4) E ≠ 0 V = 0

5) E = V regardless of the value

-Q

-Q +Q

+Q

Page 44: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

1) E = 0 V = 0

2) E = 0 V ≠ 0

3) E ≠ 0 V ≠ 0

4) E ≠ 0 V = 0

5) E = V regardless of the value

-Q

-Q +Q

+Q

The potential is zero: the scalar contributions from the two positive charges cancel the two minus charges.

However, the contributions from the electric field add up as vectors, and they do not cancel (so it is non-zero).

Follow-up: What is the direction of the electric field at the center?

Four point charges are

arranged at the corners

of a square. Find the

electric field E and the

potential V at the center

of the square.

Page 45: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Example: electric potential of an electric dipole with dipole moment p a distance r much larger than the separation 2a between the charges, r >> 2a.

r2

!

P

r1r

–q +qa a

~2a co

s !

V (P ) =kq

r1+

k(!q)r2

= kq

!1r1! 1

r2

"

=kq(r2 ! r1)

r1r2

or, for a << r

V (r, !) ! k(2qa) cos !

r2= kp

cos !

r2

Page 46: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

At which point

does V = 0?

1

3

2

4

+Q –Q

5) all of them

Page 47: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

At which point

does V = 0?

1

3

2

4

+Q –Q

5) all of them

All of the points are equidistant from both charges. Since

the charges are equal and opposite, their contributions to

the potential cancel out everywhere along the mid-plane

between the charges.

Follow-up: What is the direction of the electric field at all 4 points?

Page 48: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Equipotential surfaces of a dipole

+–

(show applet if possible)

Page 49: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

4) all of the above 5) none of the above

1)

x

+2µC

-2µC

+1µC

-1µC 2)

x

+2µC

-1µC

+1µC

-2µC 3)

x

+2µC

-1µC

-2µC

+1µC

Which of these configurations gives V = 0 at all points on the x-axis?

Page 50: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Only in case (1), where opposite charges lie

directly across the x-axis from each other, do

the potentials from the two charges above the

x-axis cancel the ones below the x-axis.

Which of these configurations gives V = 0 at all points on the x-axis?

4) all of the above 5) none of the above

1)

x

+2µC

-2µC

+1µC

-1µC 2)

x

+2µC

-1µC

+1µC

-2µC 3)

x

+2µC

-1µC

-2µC

+1µC

Page 51: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Which of these configurations gives V = 0 at all points on the y-axis?

4) all of the above 5) none of the above

1)

x

+2µC

-2µC

+1µC

-1µC 2)

x

+2µC

-1µC

+1µC

-2µC 3)

x

+2µC

-1µC

-2µC

+1µC

Page 52: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Which of these configurations gives V = 0 at all points on the y-axis?

4) all of the above 5) none of the above

1)

x

+2µC

-2µC

+1µC

-1µC 2)

x

+2µC

-1µC

+1µC

-2µC 3)

x

+2µC

-1µC

-2µC

+1µC

Only in case (3), where opposite charges lie

directly across the y-axis from each other, do

the potentials from the two charges above the

y-axis cancel the ones below the y-axis.

Follow-up: Where is V = 0 for configuration #2?

Page 53: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Which two points have the same potential?

1) A and C

2) B and E

3) B and D

4) C and E

5) no pair

A

C

B DEQ

Page 54: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Which two points have the same potential?

1) A and C

2) B and E

3) B and D

4) C and E

5) no pair

A

C

B DEQ

Since the potential of a point charge is:

only points that are at the same distance from charge Q are at the same potential. This is true for points C and E.

They lie on an Equipotential Surface.

Follow-up: Which point has the smallest potential?

Page 55: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Rank in order, from largest to

smallest, the potential differences

∆V12, ∆V13, and ∆V23 between

points 1 and 2, points 1 and 3, and

points 2 and 3. Here the symbol

∆V12 means ∆V12=V1-V2, etc

1. ∆V12 > ∆V13 = ∆V23

2. ∆V13 > ∆V12 > ∆V23

3. ∆V13 > ∆V23 > ∆V12

4. ∆V13 = ∆V23 > ∆V12

5. ∆V23 > ∆V12 > ∆V13

Page 56: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Rank in order, from largest to

smallest, the potential differences

∆V12, ∆V13, and ∆V23 between

points 1 and 2, points 1 and 3, and

points 2 and 3. Here the symbol

∆V12 means ∆V12=V1-V2, etc

1. ∆V12 > ∆V13 = ∆V23

2. ∆V13 > ∆V12 > ∆V23

3. ∆V13 > ∆V23 > ∆V12

4. ∆V13 = ∆V23 > ∆V12

5. ∆V23 > ∆V12 > ∆V13

1 and 2 the same distance from q: V1=V2

3 is farther away

since V = kq/r

potential at 3 issmaller than at 1&2

Page 57: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Example: ring of charge Q , radius a, with uniform charge density, on points along ring’s axis.

dq

x

x2 + a2

aP V =

!dV =

!k dq

r

Continuous charge distribution:

(COB)

V (x) =kQ!

a2 + x2

Page 58: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

A thin rod with charge Q has been bent into a semicircle of radius R. Find an expression for the electric potential at the center.

Ans: V = k Q/R

Page 59: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

Example: disk of charge Q , radius a, with uniform charge density, on points along disk’s axis.

xPr

dr

Sum over concentric rings, usingprevious result for ring of:

radius:

charge:

r

dq = (2!r dr)" = (2!r dr)Q

!a2=

Q

a2dr2

(COB)

V (x) =2kQ

a2

!"x2 + a2 ! |x|

#

Page 60: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

additional problems

Page 61: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

At the back of a TV picture tube, a uniform electric field of 600 kN/C extends over region of 5.0 cm and points towards the back of the tube. (a) Find the potential difference between the back and the front of this field region. (b) How much work would it take to move an ion with charge +2e from the back to the front of the field region? (c)What would happen to an electron released at the back of the field region

(COB)

Ans:(a) 30 kV(b) 9.6 x 10-15 J (or (2e)(30 kV) = 60 keV, see next page)

Page 62: week 4 - Physics Courses...For path #3, you are moving in a direction perpendicular to the field lines. This means you are moving along an equipotential, which requires no work (by

An isolated, infinite charged sheet carries a uniform charge density σ. (a) Find an expression for the potential difference from the sheet to a point a perpendicular distance x from the sheet. (b) What is the potential difference between two points the same distance from the sheet?

(COB)

ANS:

!V0x = ! !x

2"0

EA

E =!

2"0