Electric Current
Definition: rate of positive charge flow
Symbol: i
Units: Coulombs per second ≡ Amperes (A)
i = dq/dt
where q = charge (in Coulombs), t = time (in seconds)
Note: Current has polarity.
EECS 42, Spring 2005
Week 2a
1
Electric Potential (Voltage)
• Definition: energy per unit charge
• Symbol: v
• Units: Joules/Coulomb ≡ Volts (V)
v = dw/dq
where w = energy (in Joules), q = charge (in Coulombs)
Note: Potential is always referenced to some point.
a
EECS 42, Spring 2005
b
Subscript convention:
vab means the potential at a
minus the potential at b.
vab ≡ va - vb
Week 2a
2
Electric Power
• Definition: transfer of energy per unit time
• Symbol: p
• Units: Joules per second ≡ Watts (W)
p = dw/dt = (dw/dq)(dq/dt) = vi
• Concept:
As a positive charge q moves through a
drop in voltage v, it loses energy
ƒ energy change = qv
ƒ rate is proportional to # charges/sec
EECS 42, Spring 2005
Week 2a
3
The Ideal Basic Circuit Element
i
• Polarity reference for voltage can be
indicated by plus and minus signs
+
v
_
• Reference direction for the current
is indicated by an arrow
Attributes:
• Two terminals (points of connection)
• Mathematically described in terms of current
and/or voltage
• Cannot be subdivided into other elements
EECS 42, Spring 2005
Week 2a
4
A Note about Reference Directions
A problem like “Find the current” or “Find the voltage”
is always accompanied by a definition of the direction:
i
- v +
In this case, if the current turns out to be 1 mA flowing
to the left, we would say i = -1 mA.
In order to perform circuit analysis to determine the
voltages and currents in an electric circuit, you need to
specify reference directions. There is no need to guess
the reference direction so that the answers come out
positive, however.
EECS 42, Spring 2005
Week 2a
5
Sign Convention Example
Suppose you have an unlabelled battery and you measure
its voltage with a digital voltmeter (DVM). It will tell you the
magnitude and sign of the voltage.
a
−1.401
DVM
+
b
With this circuit, you are
measuring vab.
The DVM indicates −1.401, so va
is lower than vb by 1.401 V.
Which is the positive battery
terminal?
Note that we have used the “ground” symbol ( ) for the reference
node on the DVM. Often it is labeled “C” for “common.”
EECS 42, Spring 2005
Week 2a
6
Sign Convention for Power
Passive sign convention
p = vi
p = -vi
i
+
v
_
i
i
_
+
v
_
v
+
i
_
v
+
• If p > 0, power is being delivered to the box.
• If p < 0, power is being extracted from the box.
EECS 42, Spring 2005
Week 2a
7
Power Calculation Example
Find the power absorbed by each element:
Conservation of energy
Î total power delivered
equals
total power absorbed
Aside: For electronics these are unrealistically large currents – mA is
more typical than A
vi (W)
918
- 810
- 12
- 400
- 224
1116
EECS 42, Spring 2005
Week 2a
p (W)
8
Circuit Elements
• 5 ideal basic circuit elements:
–
–
–
–
–
voltage source
current source
resistor
inductor
capacitor
active elements, capable of
generating electric energy
passive elements, incapable of
generating electric energy
• Many practical systems can be modeled with just
sources and resistors
• The basic analytical techniques for solving
circuits with inductors and capacitors are the
same as those for resistive circuits
EECS 42, Spring 2005
Week 2a
9
Electrical Sources
• An electrical source is a device that is capable of
converting non-electric energy to electric energy and
vice versa.
Examples:
– battery: chemical
electric
– dynamo (generator/motor): mechanical
electric
ÆElectrical sources can either deliver or absorb power
EECS 42, Spring 2005
Week 2a
10
Ideal Independent and Dependent Voltage
Sources
• Circuit element that maintains a prescribed voltage
across its terminals, regardless of the current
flowing in those terminals.
– Voltage is known, but current is determined by the circuit
to which the source is connected.
• The voltage can be either independent or dependent
on a voltage or current elsewhere in the circuit, and
can be constant or time-varying.
Circuit symbols:
vs +_
independent
EECS
42, Spring 2005
vs=µ vx +_
vs=ρ ix +_
voltage-controlled
Week 2a
current-controlled
11
EECS 42, Spring 2005
Week 2a
12
Other Independent Voltage Source Symbols
Sinusoidal AC source
v(t) = Vpeaksin(ωt)
Veffective = Vpeak\/2
(In US, 120 V, so
Vpeak = 170 V)
Battery (realistic source)
+
VS
EECS 42, Spring 2005
Week 2a
13
Realistic Voltage Source
„
„
„
A real-life voltage source, like a battery
or the function generator in lab, cannot
sustain a very high current. Either a
fuse blows to shut off the device, or
something melts…
Additionally, the voltage output of a
realistic source is not constant. The
voltage decreases slightly as the
current increases.
We usually model realistic sources
considering the second of these two
phenomena. A realistic source is
modeled by an ideal voltage source in
series with an “internal resistance”, R S.
Spring 2005
EECS 42, Spring 2005
Vs
+
−
RS
14
EE 42 Lecture 3
Week 2a
14
I-V Plot for a Real Battery
EECS 42, Spring 2005
Week 2a
15
Ideal Independent and Dependent Current
Sources
• Circuit element that maintains a prescribed current
through its terminals, regardless of the voltage
across those terminals.
– Current is known, but voltage is determined by the circuit
to which the source is connected.
• The current can be either independent or dependent
on a voltage or current elsewhere in the circuit, and
can be constant or time-varying.
Circuit symbols:
is
independent
EECS
42, Spring 2005
is=α vx
is=β ix
voltage-controlled
Week 2a
current-controlled
16
Electrical Resistance
• Resistance: Electric field is proportional to current
density, within a resistive material. Thus, voltage is
proportional to current. The circuit element used to
model this behavior is the resistor.
R
Circuit symbol:
Units: Volts per Ampere ≡ ohms (Ω)
• The current flowing in the resistor is proportional to the
voltage across the resistor:
v=iR
(Ohm’s Law)
where v = voltage (V), i = current (A), and R = resistance (Ω)
EECS 42, Spring 2005
Week 2a
17
Resistance of an actual resistor
Material resistivity
= ρ (Ω-cm)
T
L
W
Resistance = resistivity x length/(cross-sectional area)
R = ρ (L/WT)
EECS 42, Spring 2005
Week 2a
18
Electrical Conductance
• Conductance is the reciprocal of resistance.
Symbol: G
Ω
Units: siemens (S) or mhos ( )
Example:
Consider an 8 Ω resistor. What is its conductance?
EECS 42, Spring 2005
Week 2a
19
Short Circuit and Open Circuit
Wire (“short circuit”):
• R = 0 Æ no voltage difference exists
(all points on the wire are at the same potential)
• Current can flow, as determined by the circuit
Air (“open circuit”):
• R = ∞ Æ no current flows
• Voltage difference can exist,
as determined by the circuit
EECS 42, Spring 2005
Week 2a
20
Circuit Nodes and Loops
• A node is a point where two or more circuit elements
are connected.
• A loop is formed by tracing a closed path in a circuit
through selected basic circuit elements without
passing through any intermediate node more than
once
Example:
EECS 42, Spring 2005
Week 2a
21
Kirchhoff’s Laws
• Kirchhoff’s Current Law (KCL):
– The algebraic sum of all the currents entering any
node in a circuit equals zero.
• Kirchhoff’s Voltage Law (KVL):
– The algebraic sum of all the voltages around any
loop in a circuit equals zero.
EECS 42, Spring 2005
Week 2a
22
Example: Power Absorbed by a
Resistor 2
p = vi = ( iR )i = i R
p = vi = v ( v/R ) = v2/R
Note that p > 0 always, for a resistor.
Example:
a) Calculate the voltage vg and current ia.
b) Determine the power dissipated in the 80Ω resistor.
EECS 42, Spring 2005
Week 2a
23
“Lumped Element” Circuit
Modeling
(Model = representation of a real system which simplifies analysis)
• In circuit analysis, important characteristics are grouped
together in “lumps” (separate circuit elements) connected by
perfect conductors (“wires”)
• An electrical system can be modeled by an electric circuit
(combination of paths, each containing 1 or more circuit
elements) if
λ = c/f >> physical dimensions of system
Distance travelled by a particle travelling at the speed of light
in one period
Example: f = 60 Hz
λ = 3 x 108 m/s / 60 = 5 x 106 m
EECS 42, Spring 2005
Week 2a
24
Construction of a Circuit Model
• The electrical behavior of each physical
component is of primary interest.
• We need to account for undesired as well as
desired electrical effects.
• Simplifying assumptions should be made
wherever reasonable.
EECS 42, Spring 2005
Week 2a
25
Terminology: Nodes and Branches
Node: A point where two or more circuit elements
are connected
Branch: A path that connects two nodes
EECS 42, Spring 2005
Week 2a
26
•
Notation: Node and Branch
Voltages
Use one node as the reference (the “common” or
“ground” node) – label it with a symbol
• The voltage drop from node x to the reference node
is called the node voltage vx.
• The voltage across a circuit element is defined as the
difference between the node voltages at its terminals
Example:
EECS 42, Spring 2005
– v1 +
a R1 b
+
va +_ vs
_
c Week 2a
+
R2 vb
_
Å REFERENCE NODE27
Using Kirchhoff’s Current Law
(KCL)
Consider a node connecting several branches:
i2
i3
i1
i4
• Use reference directions to determine whether
currents are “entering” or “leaving” the node – with no
concern about actual current directions
EECS 42, Spring 2005
Week 2a
28
Formulations of Kirchhoff’s
Current
Law
(Charge stored in node is zero.)
Formulation 1:
Sum of currents entering node
= sum of currents leaving node
Formulation 2:
Algebraic sum of currents entering node = 0
• Currents leaving are included with a minus sign.
Formulation 3:
Algebraic sum of currents leaving node = 0
• Currents entering are included
with a minus sign.
Week 2a
EECS 42, Spring 2005
29
A Major Implication of KCL
• KCL tells us that all of the elements in a single
branch carry the same current.
• We say these elements are connected in series.
Current entering node = Current leaving node
i 1 = i2
EECS 42, Spring 2005
Week 2a
30
KCL Example
Currents entering the node:
-10 mA
i
Currents leaving the node:
5 mA
15 mA
3 formulations of KCL:
1.
2.
EECS3.
42, Spring 2005
Week 2a
31
Generalization of KCL
• The sum of currents entering/leaving a closed
surface is zero. Circuit branches can be inside this
surface, i.e. the surface can enclose more than one
node!
i2
i3
This could be a big
chunk of a circuit,
e.g., a “black box”
EECS 42, Spring 2005
i1
Week 2a
i4
32
Generalized KCL Examples
50 mA
5µA
2µA
i
i
EECS 42, Spring 2005
Week 2a
33
Using Kirchhoff’s Voltage Law
(KVL)
Consider a branch which forms part of a loop:
loop
+
v1
_
voltage
“drop”
loop
–
v2
voltage
“rise”
+ (negative drop)
• Use reference polarities to determine whether a
voltage is dropped – with no concern about actual
voltage polarities
EECS 42, Spring 2005
Week 2a
34
Formulations of Kirchhoff’s
Voltage
Law
(Conservation of energy)
Formulation 1:
Sum of voltage drops around loop
= sum of voltage rises around loop
Formulation 2:
Algebraic sum of voltage drops around loop = 0
• Voltage rises are included with a minus sign.
(Handy trick: Look at the first sign you encounter on each element when tracing the loop.)
Formulation 3:
Algebraic sum of voltage rises around loop = 0
• Voltage drops are included
with a minus sign.
Week 2a
EECS 42, Spring 2005
35
A Major Implication of KVL
• KVL tells us that any set of elements that are
connected at both ends carry the same voltage.
• We say these elements are connected in parallel.
+
va
_
+
vb
_
Applying KVL in the clockwise direction,
starting at the top:
vb – va = 0 Î vb = va
EECS 42, Spring 2005
Week 2a
36
KVL Example
Three closed paths:
1
+
va
−
b
+
vb
-
−
+ v2 −
v3
2
+
a
c
+
vc
−
3
Path 1:
Path 2:
Path 3:
EECS 42, Spring 2005
Week 2a
37
An Underlying Assumption of
KVL
• No time-varying magnetic flux through the loop
Otherwise, there would be an induced voltage (Faraday’s Law)
• Note: Antennas are designed to “pick up”
electromagnetic waves; “regular circuits”
often do so undesirably.
Avoid these loops!
v
B( t )
+
−
v( t )
How do we deal with antennas (EECS 117A)?
Include a voltage source as the circuit representation
of the induced voltage or “noise”.
(Use a lumped circuit model rather than a distributed (wave)
model.)
EECS 42, Spring 2005
Week 2a
38
Resistors in Series
Consider a circuit with multiple resistors connected in series.
Find their “equivalent resistance”.
I
R1
R2
VSS
+
−
• KCL tells us that the same
current (I) flows through
every resistor
• KVL tells us
R3
R4
Equivalent resistance of resistors in series is the sum
EECS 42, Spring 2005
Week 2a
39
Voltage Divider
I
R1
+
– V1
I = VSS / (R1 + R2 + R3 + R4)
R2
VSS
+
−
R3
+
– V3
R4
EECS 42, Spring 2005
Week 2a
40
When can the Voltage Divider Formula
be Used?
I
I
R1
R2
VSS
+
−
R1
+
– V2
R3
R4
R
2
V =
⋅V
2
SS
R +R +R +R
1 2 3 4
Correct, if nothing else
isEECS
connected
42, Spring 2005 to nodes
R2
VSS
+
−
+
– V2
R3
R4
R5
R
2
V ≠
⋅V
2
SS
R +R +R +R
1 2 3 4
because R5 removes condition
of2a resistors in series
Week
41
Resistors in Parallel
ISS
Consider a circuit with two resistors connected in parallel.
Find their “equivalent resistance”.
x
• KVL tells us that the
same voltage is dropped
I1
I2
across each resistor
R1
R2
Vx = I1 R1 = I2 R2
• KCL tells us
EECS 42, Spring 2005
Week 2a
42
General Formula for Parallel
Resistors
What single resistance R is equivalent to three resistors in parallel?
eq
I
I
+
V
+
R1
−
R2
R3
eq
≡
V
Req
−
Equivalent
conductance ofWeek
resistors
in parallel is the sum
EECS 42, Spring 2005
2a
43
Current Divider
x
ISS
EECS 42, Spring 2005
I1
I2
R1
R2
Week 2a
Vx = I1 R1 = ISS Req
44
Generalized Current Divider
Formula
Consider a current divider circuit with >2 resistors in parallel:
+
I
I1
R1
V
I3
I2
R2
R3
−
V=
I
⎛ 1 ⎞ ⎛ 1 ⎞ ⎛ 1 ⎞
⎟⎟
⎜ ⎟+⎜
⎟ + ⎜⎜
⎝ R1 ⎠ ⎝ R 2 ⎠ ⎝ R 3 ⎠
⎡
⎤
1/R 3
V
= I⎢
I3 =
⎥
+
+
R3
1/R
1/R
1/R
⎣ 1
2
3⎦
EECS 42, Spring 2005
Week 2a
45
E E 4 2 : C h ec k list o f T erm s
2 5 Ja n. 2 0 0 5
C ha rge , c urre nt, vo lta ge , resista nc e , c o nd uc ta nc e , e ne rg y, p o w e r
C o ulo m b , a m p e re , vo lt, o h m , sie m e n (m ho ), jo ule , w a tt
K irc hho ff’s C urre nt L a w (K C L ), K irc h ho ff’ s V o lta ge L a w
(K V L ), O h m ’s L a w
S e rie s c o nne c tio n, p a ra lle l c o n ne c tio n
D C (ste a d y), A C (tim e -va ry in g)
Ind e p e nd e n t a nd d e p e nd e nt id e a l vo lta ge a nd c urre nt s o urc e
V o lta ge d iv id e r, c urre nt d iv id e r
A na lo g (A /D ), D ig ita l (D /A )
EECS 42, Spring 2005
Week 2a
46