Transcript Slide 1

Chapter 17 Electrical Energy
and Current
17 – 1 Electric Potential
• Electric potential energy (EPE): the
potential energy associated with an
object’s position in an electric field
• Electrical potential energy is a
component of mechanical energy.
ME = KE + PEgrav + PEelastic + PEelectric
Electrical potential energy can be associated
with a charge in a uniform field.
ΔPEelectric = qEd
magnitude of
change in PE
q = charge
E = electric field
d = displacement from a reference point
Review
• In the case of gravity, the
gravitational field does
work on a mass
• WAB=F d = mgd
• ΔPE = W AB= mgΔh
• In the case of a charge
moving in an electric
field
• As the positive charge
moves from A to B, work
is done
• WAB = F d = q E d
• ΔPE = W AB= q E Δd
Energy and Charge Movements
Direction of
movement
+ charge
- charge
Along E
Loses PE
Gains PE
Opposite E
Gains PE
Loses PE
Electric potential energy for a pair
of point charges
q1q2
PE  kc
r
Note: The reference point for zero potential energy is
usually at 
Example
• What is the potential energy of the charge
configuration shown?
q 3 = 1.0 mc
q 2 = - 2.0 mc
q 1 = 2.0 mc
0.30 m
Given:
q 1 = 2.0 x 10-6 C
q 2 = - 2.0 x 10-6 C
q 3 = 1.0 x 10-6 C
r = 0.30 m (same for all)
k= 9.0 x 109 n•m2/C2
The total potential energy is the algebraic sum
of the mutual potential energies of all pairs of
charges.
• PET = PE12 + PE23 + PE 13
• = k q1q 2 +
kq2q3 + kq1q3
r
r
• = k [(q1q2) + (q2q3 ) +
r
(q1q3)]
r
= [(9.0 x 109 n•m2/C2)/ 0.30] x [(2.0 x 10-6 C)(- 2.0 x 10-6 C)
+ (- 2.0 x 10-6 C)(1.0 x 10-6 C) +(2.0 x 10-6 C)(1.0 x 10-6 C)]
=- 0.12 J
Electric Potential
• Electric potential: the electric potential energy
associated with a charged particle divided by the
charge of the particle
• symbol for electric potential = V
V = PE/q
• SI unit = volt (V)
• 1Volt = 1 Joule/Coulomb
Potential Difference
• Potential Difference equals the work that must
be performed against electric forces to move a
charge between the two points in question,
divided by the charge.
• Potential difference is a change in electric
potential.
PEelectric
V 
q
changein electric potentialenergy
potentialdifference
electric charge
Chapter 17
Potential Difference, continued
• The potential difference in a uniform field varies
with the displacement from a reference point.
∆V = –Ed
Potential difference in a
uniform electric field
E = electric field
d = displacement in the field
Sample Problem
• A proton moves from rest in
an electric field of 8.0104
V/m along the +x axis for 50
cm. Find
• a) the change in in the
electric potential,
• b) the change in the
electrical potential energy,
and
• c) the speed after it has
moved 50 cm.
• a) V = -Ed = -(8.0104 V/m)(0.50 m) = -4.0104 V
b) PE = q V = (1.610-19 C)(-4.0 104 V)
= -6.4 10-15 J
• C) Ei = Ef
• KEi+PEi = KEf + PEf,
since KEi=0
KEf = PEi – PEf = -PE
1/2 mpv2 = -PE
v = 2 PE/m
= 2(6.4x10-15 J)/1.67x10-27 kg)=2.8x106 m/s
Chapter 17Difference,
Potential
point charges
• At right, the electric potential at point A depends on
the charge at point B and the
distance r.
• An electric potential exists at
some point in an electric
field regardless of whether
there is a charge at that
point.
Chapter 17
• The reference point for potential
difference near a point charge is often
at infinity.
• Potential Difference Between a Point at
Infinity and a Point Near a Point Charge
q
V  k c
r
Electric Potential of Multiple Point
Charges- Superposition
• The total electric potential
at point “a” is the
algebraic sum of the
electric potentials due to
the individual charges.
Problem Solving with Electric
Potential (Point Charges)
• Remember that potential is a scalar quantity
– So no components to worry about 
• Use the superposition principle when you have
multiple charges
– Take the algebraic sum
• Keep track of sign
– The potential is positive if the charge is positive and
negative if the charge is negative
• Use the basic equation V = kcq/r
Example: Finding the Electric
Potential at Point P
5.0 mC =
= -2.0 mC
6
5
.
0

10
C
V1  (8.99  10 9 Nm 2 / C 2 )
 1.12  10 4 V,
4.0m
6
(

2
.
0

10
C)
V2  (8.99  10 9 Nm 2 / C 2 )
 3.60  10 3 V
(3.0m) 2  (4.0m) 2
Superposition: Vp=V1+V2
Vp=1.12104 V+(-3.60103 V)
=7.6103 V