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Work You do work when you push an object up a hill The longer the hill the more work you do: more distance The steeper the hill the more work you do: more force The work W done on an object by an agent exerting a constant force is the product of the component of the force in the direction of the displacement and the magnitude of the displacement
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Chapter 18Electrical energy and
Capacitance
Today’s Topics
• Electric Potential Energy• Electric Potential• Electric Equi-potential Lines
Work
• You do work when you push an object up a hill• The longer the hill the more work you do: more
distance• The steeper the hill the more work you do: more
forceThe work W done on an object by an agent exerting a constant force is the product of the component of the force in the direction of the displacement and the magnitude of the displacement
dFW ||
Work done by gravity
dFW cos
m
mg
d
cosF
Energy is capacity to do work
• Gravitational Potential Energy• Kinetic Energy• Energy can be converted into other forms of
energy • When we do work on any object we transfer
energy to it • Energy cannot be created or destroyed
mghUG 2
21 mvK
GU
GUKW
• A person lifts a heavy box of mass m a vertical distance h
• They then move a distance d, carrying the box
• How much work is done?
Quiz
Conversion of Gravitational Potential Energy to Kinetic
Energym
mg
m
v
mghUG 2
21 mvK
ghv
ghv
mghmv
2
221
2
2
Work done on object
h
Electric Potential Energy
EEF Q
+Q
+Q
d
FdW
QEd
QEdU e
v
Electric Potential Energy
• Work done (by electric field) on charged particle is QEd
• Particle has gained Kinetic Energy (QEd)
• Particle must therefore have lost Potential Energy U=-QEd
Electric PotentialThe electric potential energy depends on the charge present
We can define and electric potential V which does not depend on charge by using a “test” charge
EdQU 0
0QUV
Change in potential is change in potential energy for a test charge per unit charge
EdQUV
0
for uniform field
Electric Potential
0QUV
compare with the Electric Field and Coulomb Force
0QFE
If we know the potential field this allows us to calculate changes in potential energy for any charge introduced
VQU EF Q
Electric Potential
Electric Potential is a scalar field
it is defined everywhere
but it does not have any direction
it doesn’t depend on a charge being there
Electric Potential, units
SI Units of Electric Potential
0QUV
EdV
Units are J/C
Alternatively called Volts (V)
We have seen
dVE / Thus E also has units of V/m
Potential in Uniform fieldE
+Q +Q
+Q
A B
C
0|| dFWBC
|||| QEddFWAB
BCABAC WWW
||QEd
||QEdU AC d||
||EdVAC
Electric Potential of a single charge
+
r
E
B
A
Advanced
Equi-potential Lines
Like elevation potential can be displayed as contours
A contour diagram
Like elevation potential requires a zero point, potential V=0 at r=
Like slope & elevation we can obtain the Electric Field from the potential field
rVE
Potential Energy in 3 chargesrQV
041Q2
Q1
Q3
12
1
02212 4
1rQQVQU
12
21
012 4
1rQQU
23
2
13
1
03123312 4
1rQ
rQQUVQUU
231312 UUUU
23
32
13
31
12
21
041
rQQ
rQQ
rQQU
Capacitors
A system of two conductors, each carrying equal charge is known as a capacitor
-
Capacitance of charged sphere
+Q
r=
VQC
definition
R
rQ V
0 41
potential due to isolated charge
Capacitors
-
+ +Q -Q
e.g. 1: two metal spherese.g. 2: two parallel sheets
Each conductor is called a plate
CapacitanceCapacitance…….. is a measure of the amount of charge a capacitor can store (its “capacity”)
Experiments show that the charge in a capacitor is proportional to the electric potential difference (voltage) between the plates.
Units
VQC
Thus SI units of capacitance are:
C/V
This unit is also known as the farad after Michael Faraday
Remember that V is also J/C so unit is also C2J-1
1F=1C/V
Capacitance
The constant of proportionality C is the capacitance which is a property of the conductor
VQ VCQ VQC
Experiments show that the charge in a capacitor is proportional to the electric potential difference (voltage) between the plates.
Capacitance of parallel plates
+Q -Q
IntutivelyThe bigger the plates the more surface area over which the capacitor can store charge C A
E
Moving plates togeth`er Initially E is constant (no charges moving) thus V=Ed decreases charges flows from battery to increase V C 1/d Never Ready+
V
Batteries, Conductors & Potential
Never R
eady
+A battery maintains a fixed potential difference (voltage) between its terminals A conductor
has E=0 within and thus V=Ed=0
VV= 0
Capacitance of parallel plates
+Q -Q
Physically
E
Never Ready+
EdV
VQC
property of conductorV