Transcript Slide 1

Lecture A
Fundamentals and Background
Charge
• “Charge” is the basic quantity
in electrical circuit analysis
• Fundamental charge quantity is
the charge of a single electron
• Charge will be in integer
multiples of a single electron’s
charge
• Units of charge = Coulombs (C)
• One Coulomb  -6.21018
electrons
Electric Fields
• A charge induces an
electric field (E-field)
• The electric field is a vector
field
• Point charge E- field:

q
ˆ
ER 2
R
Analogy: E-field vs. Gravitational field
• Electric Field:

q
ˆ
ER 2
R
• Gravitational Field:

m
ˆ
  R 2
R
Forces on Charged Particles
• A second “charge” placed in the
electric field induces a force on
both charges
• Coulomb’s Law:
 q1 q 2

F  2  q2 E
R
• Electric field is essentially the
force per unit charge placed in the
field
• “Like” charges repel; opposite
charges attract
Analogy: Mass in a Gravitational Field
• Coulomb’s Law:
 q1 q 2

F  2  q2 E
R
• Newton’s Law:


m1m2
ˆ
F  R 2  m2
R
• Demo: static electricity charge on balloon
causes it to stick to wall
Energy Transfer
• In circuit analysis, we are primarily
concerned with energy transfer
• Charges move around
• Moving a charge in an electric field
changes the charge’s potential
energy
• Work to move charge from b to a:
b
 
 
Wba    F  ds  q  E  ds
b
a
a
Electric Potential Difference
•  Wba is the work required to move a charge
from point b to point a in an electric field
• Work is a form of energy  Wba is a difference in
potential energy (units are Joules, J)
• This difference is typically quantified as an Electric
Potential Energy Difference
• Electric potential difference is the electrical potential
energy difference per unit charge:
Wba
Vba 
q
Voltage
• Vba is generally referred to as a voltage difference;
(units of Vba are volts, V)
• Generally defined in terms of derivatives, for
infinitesimal variations in charge and energy:
dw
v
dq
change in energy
Joules

 Volts , V

Coulomb
change in charge
Notes on Voltage
• The potential energy difference is due to a physical
separation (a distance) between the two points
• This potential difference provides a force which can
move charges from place to place.
• This is sometimes called an electromotive force (emf)
Charge in motion & current
• Recall:
• We are concerned with energy transfer  charge motion
• emf (or potential energy difference, or voltage difference)
can move charges
• Current is the time rate of change of charge
dq
i
dt

change in charge Coulombs

 Amperes , A
Second
change in tim e
Charge Motion in Materials
• Common model of materials:
• Materials composed of atoms
• Atoms contain protons and
neutrons in a nucleus, surrounded
by a “cloud” of electrons
• Protons are positively charged, and
are bound “tightly” in the nucleus
• Electrons are negatively charged,
and bound less “tightly” to the
atom
Charge Motion in Materials -- continued
• Electrons can move from atom to atom within a
material.
• We can transfer charge through a material via electron
motion
• Current is defined as the motion of “positive” charge
• Positive current is (by definition) in opposite direction to
electron flow
Charge motion in materials -- continued
• We apply a potential difference across the material
• emf causes electron motion away from negatively charged end
• Current is in the direction of “positive” charge motion
Current Flow in Materials
• The less “tightly” bonded the electrons are to the atom,
the more “easily” the material allows current to flow
• The material conducts electricity more easily
• The material has less resistance or higher conductivity
• For example,
• conductors have low resistance to current flow  low
potential differences can provide high currents
• insulators have high resistance to current flow  nearly no
current flow, even with high potential differences
• Demo: touch electric fence with conductor
and insulator
General Passive Circuit Elements
• General, two-terminal,
passive circuit element
• Apply a voltage difference
across the terminals
• This voltage difference
results in current flow
• Our circuit elements will be
electrically neutral
• Current entering the element
is the same as the current
leaving the element
Power
• Power is the rate of change of energy with time
dW dW dq
P


 v i
dt
dq dt
• Units of power are Watts (W)
Power Generation and Dissipation
• Power dissipation:
• Current enters the positive voltage terminal
• Examples:
• Power dissipated as heat (light bulbs)
• Power converted to mechanical system (electric motors,
pumps)
• Power generation
• Current enters the negative voltage terminal
• Examples:
• Power generated by mechanical system (turbines,
generators)
• Power generated by chemical processes (batteries)
• Demos?
– Pulling mass across surface with DC motor (point out energy added,
dissipated)
– Pump water through horizontal tubing (point out energy exchange)