ELECTRICAL ENGINEERING REFERENCE INFORMATION
ELECTRICITY AND MAGNETISM BASICS, CIRCUIT THEOREMS AND EQUATIONS
Electrical engineering
(EE) is a discipline that deals with electricity, magnetism and their applications. EE applications include electronics, power conversion, data communications, computer science, information technologies, and other. The term EE usually encompasses electronic engineering or electronics. Electronics involves the design and analysis of electronic circuits. In academia and electronic industry, the terms electrical and electronics engineer often are used interchangeably.Find Science and
Engineering Degree Program Online
In other industries, the term electrical engineer may refer to those
who deal with utility and industrial power systems and other electric
equipment. In any case, both disciplines are overlapping.The theoretical foundation for EE is electromagnetism. The theory of classical electromagnetism is based on Maxwell's equations (see below), which provide a unified description of the behavior of electric and magnetic fields as well as their interactions with matter. In practice however, circuit designers normally use simplified equations of electricity and magnetism and theorems that use circuit theory terms, such as Ohm's law modified for AC circuits, voltage and current Kirchoff's laws, and power relationships.
This webpage is for those who already learned EE and needs a quick reference. Here you will find electricity and magnetism basics, electronics reference as well as the career related information on the web.
Electronic formulas and impedance calculations;
Understanding the physics of electronic circuits;
Distance learning, online degrees from accredited schools, salary surveys;
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MAXWELL'S EQUATIONS IN FREE SPACE (in SI units) |
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| LAW | DIFFERENTIAL FORM | INTEGRAL FORM |
|
Gauss' law for electricity Gauss' law for magnetism Faraday's law of induction Ampere's law |
 |
|
| NOTES:
E - electric field, ρ -
charge density, ε0 ≈
8.85×10-12 - electric
permittivity of free space, π ≈ 3.14159, k - Boltzmann's constant, q - charge, B - magnetic induction, Φ - magnetic flux, J - current density, i - electric current, c ≈ 299 792 458 m/s - the speed of light, µ0 = 4π×10-7 - magnetic permeability of free space,  .V
is divergence of V,
×V is the curl of V). |
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BASIC ELECTRICAL THEOREMS AND CIRCUIT ANALYSIS LAWS |
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| THE LAW | DEFINITION | RELATIONSHIP TO OTHER LAWS |
| Ohm's Law extended for AC circuits with single frequency sinusoidal signals | V=Z×Ĩ,
where V and Ĩ - voltage and current
phasors, Z - complex impedance (for resistive circuits: Z=R and V=R×I ) |
Lorentz force law and Drude model for resistors |
| Kirchhoff's Current Law (KCL) | The sum of electric currents which flow into any junction in a circuit is equal to the sum of currents which flow out | Conservation of electric charge |
| Kirchhoff's Voltage Law (KVL) | The sum of the voltages around a closed circuit must be zero | Conservation of energy |
You can download a reference sheet with the above equations in a pdf file.
ELECTRICAL NETWORK THEOREMS FOR AC CIRCUITS |
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| THE THEOREM | DEFINITION | CALCULATION |
Thevenin's
Theorem |
Any combination of a single frequency sinusoidal AC sources and impedances with two terminals can be replaced by a single voltage source V in series with an impedance Z. | V - open-circuit voltage phasor of the original
circuit; Z - impedance between the two terminals with all voltage sources shorted and all current sources opened. |
Norton's
Theorem |
Any combination of a single frequency sinusoidal AC sources and impedances with two terminals A and B can be replaced by a single current source I in parallel with an impedance Z. | I - short-circuit current phasor of the original
circuit; Z - impedance between the two terminals with all voltage sources shorted and all current sources opened. |
| Superposition Theorem | The current (voltage) phasor in any part of a linear circuit equals the algebraic sum of the current (voltage) phasors produced by each source separately. | To find an individual current (voltage) from each source, short all other voltage sources and open all other current sources. |
| Maximum Power Transfer Theorem | A voltage source delivers maximum power to a adjustable when the source and the load impedances are complex conjugates of each other | Active components of the source and load impedances should be equal, and reactive components should have equal magnitude but opposite sign. |
Delta to Wye Transformation |
A delta network of three impedances can be transformed into a star (Y) network of three impedances | Za =
ZcaZab / (Zab+Zbc+Zca) Zb = ZabZbc / (Zab+Zbc+Zca) Zc = ZbcZca / (Zab+Zbc+Zca) |
Star-Delta Transformation |
A star (Y)
network of three impedances can be transformed into a delta
network of three impedances |
Zab
= Za + Zb + (ZaZb / Zc) Zbc = Zb + Zc + (ZbZc / Za) Zca = Zc + Za + (ZcZa / Zb) |
