Chapter 1
Fundamental Electrical Concepts
Charge, current, voltage, power circuits, nodes, branches
Branch and node voltages, Kirchhoff Laws
Electrical Charge
Relates to electrical forces between particles Bipolar: positive or negative charge
Electrical effects due to movement and
separation of charge
Is measured in coulomb [C]
Symbol Q (static) or q (time varying)
Discrete: electron has charge e = -1.602 x 10-19 C
Coulomb’s law: Q1 Q 2 1
r
r
2 12 2 12 2 1 12 rˆ r Q Q F = ε §1.3 (charge = lading)Electrical Current
Moving electrical charge
Controlled movement and separation of charges determines function of circuit or system
Current can be:
Function of time: alternating current (ac) Constant: direct current (dc)
Symbol I (dc) or i (ac) Unit: ampere (A)
+ + + + + + + + + + – – – – – – – – – – Migration of electrons
Conducting source with Conducting target wire
(current = stroom)
ampere =
Electrical Current
+ + + + + + + + + + – – – – – – – – – – Migration of electronsConducting source with excess electrons Conducting target depleted of electrons wire + + + + + + + + + + – – – – – – – – – – + + + + + + + + + + + + + + + + + + + + – – – – – – – – – – – – – – – – – – – – Migration of electrons
Conducting source with excess electrons Conducting target depleted of electrons wire + + + + + + + + + + – – – – – – – – – – excess electrons shortage of electrons + pole - pole Positive current Electron flow battery
Electrical Current
Current: amount of charge being transferred per unit time: ampere = coulomb/second.
q q q q A q ∆t ∆q q t q I ∆ ∆ = dt dq i = (stroomsterkte)
Electrical Current
Current follows a path
has a direction: arrow and sign
and magnitude
-2 mA
-2 mA 2 mA 2 mA
Voltage or Potential Difference
Relates to the energy associated with charge transfer (current) unit: volt [V] symbol: V (dc) or v (ac) q w vab = ab + – vab a b
One volt is the amount of work (energy) it costs to transfer one coulomb of charge
Hydraulic Analogy
Pressure Difference ⇔ Potential Difference Water Flow ⇔ Current FlowVoltage is an across-quantity Current is a through-quantity
Voltage across terminals a and b Current through a wire
Voltage and Current
+ – vab a b i
current voltage
Power
unit watt [W] = joule/second [J/s] symbols: P, p §1.4 second work = p
Power = Rate of Work
= amount of work divided by time it takes
i x v p = voltage x current = second charge x charge work =
Unassociated
Associated: into plus terminal, leaving minus terminal
+ – v i
Reference Directions
+ – v i – + v i – + v i☺
Power Direction
V = 3V I = 20mA = 0.02A Battery power: ? absorbing p < 0 unassociated releasing p > 0 unassociated releasing p < 0 associated absorbing p > 0 associated Condition vi product Reference direction Assocociated! I1 = -ILamp power: ? >0 ⇒ absorbing
<0 ⇒ releasing
Note: total power = 0!
I1 V = (-0.02)(3) = -0.06 I V = (0.02)(3) = 0.06
Circuit Diagram
Way of visual communication of electrical model of circuit / system / product Example circuit diagram of battery charger §1.5Bierthermometer
All different schematics but identical circuits
Circuit Diagram
Only gives connectivity
Form or shape is not important
32
Node
Elements are connected together
Connections are called nodes (knooppunten)
Nodes are drawn as line segments in circuit diagram
Connected line segments form a node
One node connects two or more elements
Node has unique potential (Circuit behavior follows from
potential (voltage) difference between nodes!)
Circuit Diagram
dot jump gap cross
shift √ x x x 2 3 3 3 dot jump gap cross connection # nodes not prefered
Node Names
Nodes often have a unique
identifier or name or number or label or ...
a c d b e1 e2 e3 e4 e5 AMP INPUT OUTPUT COMMON 1 2 3 Idem elements Other annotations: Whatever is useful
Element values and type numbers, voltage, current, power, noise and any other relevant signal property, etc.
Path and Branch
Path (pad): trace of adjoining two-terminal elements
Branch (tak): a path that connects two nodes (and no more)
What are some branches? a - e1 - b What are some paths?
a - e1 - b - e2 - c a - e3 - d - e4 - b a c d b e1 e2 e3 e4 e5
Branch Voltages and Currents
Voltage across a branch (voltage is across-quantity)
Current through a branch (current is through-quantity)
a c d b e + + -Vab Ve §1.6
Can use two node names or element name to specify a branch and branch voltage
Node Voltages
Do they exist?
same branch voltages imply same behavior
NO
Only potential differences are important Voltage = potential difference
Node voltage can not be defined unambiguously
10V 15V 30V 20V 110V 115V 130V 120V -5V 0V 15V 5V
Vx ≡ Vx-reference
Node Voltages
Do they exist?
YES
Only when one arbitrary but specific node is chosen as reference node with a potential of 0V
Identical branch voltages Identical currents
Identical behavior
reference node = ground node = common node symbols: a c d b + -Vc 0V
Reference Node is Arbitrary
5V
2V
+3V
May choose one arbitrary
node as reference (0V)
One choice may be much more convenient for
calculation than other -a b c + 2V + 3V -d a b c Vc ? Vb ? d a b c Vb ? Vd ?
Loops
Loop (lus): closed path, begin node same as end node
How many loops?
a b d a b c d b c b a d c a c d b e §1.6
Voltage Drops
a b c d + 3V - + 2V - - 4V + Vab = Vac = Vad = 3V 5V 1VVoltage drop (spanningsval): difference in potential between two nodes along a path
!
Voltage Drops
Voltage drop (spanningsval): difference in potential between two nodes along a path
Take care of positive and negative sign reference
a b c d + V1 - + V2 - - V3 + Vab = Vac = Vad = Va – Vb = V1 Va – Vc = (Va – Vb) + (Vb – Vc) = V1 + V2 Va – Vd = (Va – Vb) + (Vb – Vc) + (Vc – Vd) = V1 + V2 – V3 voltage drop node potential
Kirchhoff’s Voltage Law (Spanningswet)
KVL: The algebraic sum of the
branch voltage drops around any loop (= closed path) is zero
vc vb va v1 v2 v4 v3 vd + + + + -- - KVL: v4 – v5 – v2 = 0 v4 – v5 – v2 = (vb – vd) – (vc – vd) – (vb – vc) = vb – vb – vd + vd – vc + vc = 0 v5 + –
☺
§1.7Kirchhoff’s Current Law (Stroomwet)
KCL: The sum of the currents entering a node is equal to the sum of the currents leaving the node
5µA
2µA
3µA
Analogy:
Flow of water in pipes Cars at highway
Circuit Elements
Transistors, switches, resistors, capacitors and many more
At least two terminals
Constitutive Relation
(Constitutieve Relatie)
Terminal is connection point
Current can flow into or out of terminal (and element)
Potential difference can exist between terminals:
branch voltage
Relation between branch voltage and terminal current defines function of element
v = f(i), i = f--1(v) +
– v
i
Note: functions of more than 1 variable in case of multi-terminal elements
Voltage v is defined
Current may have any value Idealized component
In practice, voltage will to some extend depend on current (and temperature, age, ...)
Voltage Source (Spanningsbron)
+ -v + -v ISO Symbol
Current Source (Stroombron)
Current i is defined Voltage arbitrary In practice .... ISO symbol i iLinear resistance: voltage proportional to current
Ohm’s Law (wet van Ohm)
v = i · R
R is resistance, unit: Ω (Ohm) = V/A
Resistance (Resistantie)
Resistance: The property of materials to impede the flow of electric charge
R
ISO symbol
i R
Resistor (Weerstand)
An actual circuit element having resistance as it’s main characteristic
Resistance means merely the electrical model of an ideal resistor
In practice, v = i R is only approximately or accurately valid in limited range of operating conditions (i.e. voltage, current, frequency, temperature)
Resistivity (Resistiviteit)
Resistance depends on
Material shape
of element
Consider rectangular resistive wire
Resistance R proportional to
– l length of resistor
– 1/AR inverse of cross-sectional area
– ρ specific resistivity of material
AR=hxw h i l w l R =
ρ
Current through Resistance
+ -v R i i = f (v,R) = v/R Constitutive relation (constitutieve relatie)Resistors in Series (serieschakeling)
+ -v R1 i i = f (v, R 1, R2) = ? R2 + -v1 + -v2 v = v1 + v2 = iR1 + iR2 = (R1 + R2) i v = Req i + v Req =∑
Rk i KVL: v1 + v2 –v = 0 Q: Did we use KCL? Equivalent resistance of series resistorsequal to the sum of individual resistances
V kΩ mA v=iR TIP! equivalent Req = 3kΩ
Resistors in Series: Example
+ -V=6V 1kΩ I 2kΩ + -v1 + -v2 v = i Req (Ohms Law) 6V = I x 3k
Ω
I = 6V/3kΩ
= 2.10-3 A = 2 mA V = 6V Determine I V = I Req (Also in DC case)See §1.2 for units and prefixes
V
Ω A
01 fundamental 14 TUE/EE 5CC00 netwerk analyse 04/05 - © NvdM
Bierthermometer LM3914N
Example
(Voltage Divider)
+ -v R1 R2 + -v1 + -v2 R3 + -v3 i LM3914NExample (Voltage Divider)
Calculate Vout 2 1R
R
V
I
+
=
V R1 R2 + -Vout + -INote (KCL): all current flows from source through R1 and R2, no current flows into output terminals (it can’t go anywhere there)
V R R R IR Vout 2 1 2 2 = + =
You will need this for first
programming assignment of the course “computation”
Potentiometers
Potentiometer = adjustable voltage divider
R (1−α)R
Potentiometers
Potentiometer
Typical audio amplifier:
1. Pre-amplifier 2. adjustable level reduction 3. power amplifier 1. 2. 3. R V + - Vout +
-Compute Vout as a function of α. Does Vout depend on R? (0 ≤ α ≤ 1 function of knob angle)
Summary
Charge, current, voltage Power
Circuits, Nodes, Branches, Loops Branch vs Node Voltages
KVL and KCL
Ideal Voltage and Current Sources
Resistance: Ohms Law, series connection Voltage division
Next: capacitor, inductor, combining ckt elements …