© John Parkinson 1 2 Electric Field "An electric field is a region in which charged particles...
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Transcript of © John Parkinson 1 2 Electric Field "An electric field is a region in which charged particles...
© John Parkinson
1
2
Electric Field
"An electric field is a region in which charged particles experience a force"
ELECTRIC FIELD
+Q FORCE-QFORCE
Lines of force show the direction of the force felt by a positive charge
3
THE DENSITY OF THE FIELD LINES IS A MEASURE OF THE STRENGTH OF THE FIELD
-+
Field lines start and end on charges
4
This is defined as the force per unit [+ve] charge acting at a point in the field.
ELECTRIC FIELD
STRENGTH E
ELECTRIC FIELD STRENGTH E
Q
FE UNITS = ?N C-1
Hence the force on a charge of Q coulombs in the diagram above is given by :
+Q
F = E Q
IT IS A VECTOR
5
Simply Potential [i.e. the volts] measures the energy of each coulomb of charge.
Electric potential, V
Electric potential is the electrical potential energy per unit charge (ie. per coulomb) at a point in a field.
This is the work done per unit charge in bringing a small positive charge from infinity to the point.
Potential only depends on the charge causing the field and is a scalar
Hence the energy of Q coulombs of charge at a point, where the potential is V
volts is given by W = QV
6
+QA point charge or a
charged sphere produces a radial field
Lines of Equipotential V
These are perpendicular to the field lines
FIELD PATTERNS
At any point the field strength equals the potential gradient
r
VE
7
+Q
Field & Potential due a point charge or charged sphere
At a distance r from the charge
204 r
QE
E is a
vector
r
QV
04 V is a
scalar
8
FIELD PATTERNS Oppositely charged parallel plates produce
a uniform field between the plates
+++++++++++++++++++++++++++++
--------------------------------------------------
Evenly spaced equipotentials – so it’s a uniform field.
Equipotentials
9
V Voltsd metres
The field is uniform
Hence the potential gradient V/r is uniform
Henced
VE
It follows that E has units of N C-1 or V m-1
10
Electric Potential Contours (energy levels)
-Q +Q 0 V
-100 V
200 V
300 V
400 V
100 V
-200 V
-300 V
This is analogous to climbing
[and falling down]
gravity hills
QUESTION How much energy is required to move a +0.5 C charge from A to B?
A
B
The potential difference V = VB – VA = 200 – (- 100) = 300 Volts
W = Q V = 0.5 x 300 = 150 J
11
Motion of Charge Initially Moving Perpendicularly to an Electric Field e.g. an electron in an oscilloscope beam.
- - - - - - - - - -
+ + + + + + + + + + +
Ex
y
--
vH
VH is the initial horizontal velocity and REMAINS CONSTANT - Like a projectile !!
For the vertical motion u = 0, som
Fa
2
2
1tay
For the horizontal motion, x = VH t
222x
mv
qEy
H
Hence which is a PARABOLA
where m = mass of the particle and F = EQ
12
Gravitational Field Electric Field
Inverse Square Law Newton’s Law 2
21
r
MMGF
Inverse Square Law Coulomb’s Law 2
0
21
4 r
QQF
Field Strength g = force per unit mass & is a VECTOR
2r
Gmg
Field Strength E = force per unit charge & is a VECTOR
204 r
QE
Gravity Potential, Scalar & for Radial Field r
GMVg
Electric Potential ,Scalar & for Radial Field r
QV
04
Field strength = Potential Gradient
r
Vg g
Field strength = Potential Gradient
r
VE
Definition of potential Work done in bringing a unit mass from infinity to the point in the field
Definition of potential Work done in bringing a unit charge from infinity to the point in the field
Potential Energy gmV W Potential Energy QV W
Comparing Gravitational and Electric Fields