Chapter 30. Potential and Field

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Chapter 30. Potential and Field
To understand the
production of electricity by
solar cells or batteries, we
must first address the
connection between electric
potential and electric field.
Chapter Goal: To
understand how the electric
potential is connected to the
electric field.
Chapter 30. Potential and Field
Topics:
• Connecting Potential and Field
• Sources of Electric Potential
• Finding the Electric Field from the Potential
• A Conductor in Electrostatic Equilibrium
• Capacitance and Capacitors
• The Energy Stored in a Capacitor
• Dielectrics
Stop to think 30.1
page 916
Stop to think 30.2
page 918
Stop to think 30.3
page 920
Stop to think 30.4
page 922
Stop to think 30.5
page 927
Finding the Potential from the Electric
Field
The potential difference between two points in space is
where s is the position along a line from point i to point f.
That is, we can find the potential difference between two
points if we know the electric field.
We can think of an integral as an area under a curve. Thus
a graphical interpretation of the equation above is
EXAMPLE 30.2 The potential of a parallel-plate
capacitor
EXAMPLE 30.2 The potential of a parallel-plate
capacitor
Batteries and emf
The potential difference between the terminals of an ideal
battery is
ε-emf (electromotive force)
In other words, a battery constructed to have an emf of
1.5V creates a 1.5 V potential difference between its
positive and negative terminals.
The total potential difference of batteries in series is simply
the sum of their individual terminal voltages:
Finding the Electric Field from the
Potential
In terms of the potential, the component of the electric
field in the s-direction is
Now we have reversed Equation 30.3 and have a way to
find the electric field from the potential.
EXAMPLE 30.4 Finding E from the
slope of V
QUESTION:
Kirchhoff’s Loop Law
For any path that starts and ends at the same point
Stated in words, the sum of all the potential differences
encountered while moving around a loop or closed path
is zero.
This statement is known as Kirchhoff’s loop law.
Capacitance and Capacitors
The ratio of the charge Q to the potential difference ΔVC is
called the capacitance C:
Capacitance is a purely geometric property of two
electrodes because it depends only on their surface area
and spacing. The SI unit of capacitance is the farad:
1 farad = 1 F = 1 C/V.
The charge on the capacitor plates is directly proportional
to the potential difference between the plates.
Combinations of Capacitors
If capacitors C1, C2, C3, … are in parallel, their equivalent
capacitance is
If capacitors C1, C2, C3, … are in series, their equivalent
capacitance is
The Energy Stored in a Capacitor
• Capacitors are important elements in electric circuits
because of their ability to store energy.
• The charge on the two plates is ±q and this charge
separation establishes a potential difference ΔV = q/C
between the two electrodes.
• In terms of the capacitor’s potential difference, the
potential energy stored in a capacitor is
Uc 
Q
0
qdV 
Q
0
1
C
qdq 
1 Q
2
2 C

1
2
C (V )
2
EXAMPLE 30.9 Storing energy in a capacitor
QUESTIONS:
qdV
The Energy in the Electric Field
The energy density of an electric field, such as the one
inside a capacitor, is
The energy density has units J/m3.
Dielectrics
• The dielectric constant, like density or specific heat, is a
property of a material.
• Easily polarized materials have larger dielectric constants
than materials not easily polarized.
• Vacuum has κ = 1 exactly.
• Filling a capacitor with a dielectric increases the
capacitance by a factor equal to the dielectric constant.
Summary:
General Principles

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