Electric_power

Electrical power is distributed via cables and electricity pylons like these in Brisbane, Australia.
Electric power is defined as the rate at which electrical energy is transferred by an electric circuit. When electric current flows through a circuit with resistance, it performs "work." Various devices convert this work into many useful forms, such as heat (electric heaters), light (light bulbs), motion (electric motors), and sound (loudspeaker).

Contents

1 Mathematics of electric power

1.1 In circuits
1.2 In space


2 See also
3 References
4 External links
5 Credits



Electricity can be produced by generation or from storage such as batteries. The SI unit of power is the watt.

Mathematics of electric power
In circuits
Electric power, like mechanical power, is represented by the letter P in electrical equations. The term wattage is used colloquially to mean "electric power in watts."
In direct current resistive circuits, instantaneous electrical power is calculated using Joule's Law, which is named after the British physicist James Joule, who first showed that heat and mechanical energy were interchangeable.





P
=
V
I



{\displaystyle P=VI\,}


where





P


{\displaystyle P}

 is the power (watt or W)




V


{\displaystyle V}

 is the potential difference (volt or V)




I


{\displaystyle I}

 is the current (ampere or A)
For example:





2



A


⋅
12



V


=
24



W





{\displaystyle 2\,{\mbox{A}}\cdot 12\,{\mbox{V}}=24\,{\mbox{W}}\,}

.
Joule's law can be combined with Ohm's law to produce two more equations:





P
=

I

2


R

=



V

2


R





{\displaystyle P=I^{2}R\,={\frac {V^{2}}{R}}\,}


where





R


{\displaystyle R}

 is the resistance (Ohm or Ω).
For example:





(
2



A



)

2


⋅
6

Ω
=
24



W





{\displaystyle (2\,{\mbox{A}})^{2}\cdot 6\,\Omega =24\,{\mbox{W}}\,}


and








(
12




V)



2




6

Ω



=
24



W





{\displaystyle {\frac {(12\,{\mbox{V)}}^{2}}{6\,\Omega }}=24\,{\mbox{W}}\,}


In alternating current circuits, energy storage elements such as inductance and capacitance may result in periodic reversals of the direction of energy flow. The portion of power flow that, averaged over a complete cycle of the AC waveform, results in net transfer of energy in one direction is known as real power (also referred to as active power). That portion of power flow due to stored energy, that returns to the source in each cycle, is known as reactive power.
The relationship between real power, reactive power and apparent power can be expressed by representing the quantities as vectors. Real power is represented as a horizontal vector and reactive power is represented as a vertical vector. The apparent power vector is the hypotenuse of a right triangle formed by connecting the real and reactive power vectors. This representation is often called the power triangle. Using the Pythagorean Theorem, the relationship among real, reactive and apparent power is:








(apparent power)



2


=



(real power)



2


+



(reactive power)



2




{\displaystyle {\mbox{(apparent power)}}^{2}={\mbox{(real power)}}^{2}+{\mbox{(reactive power)}}^{2}}


Real and reactive powers can also be calculated directly from the apparent power, when the current and voltage are both sinusoids with a known phase angle between them:







(real power)


=


(apparent power)


∗
c
o
s


(theta)




{\displaystyle {\mbox{(real power)}}={\mbox{(apparent power)}}*cos{\mbox{(theta)}}}








(reactive power)


=


(apparent power)


∗
s
i
n


(theta)




{\displaystyle {\mbox{(reactive power)}}={\mbox{(apparent power)}}*sin{\mbox{(theta)}}}


The ratio of real power to apparent power is called power factor and is a number always between zero and one.

In space
Electrical power flows wherever electric and magnetic fields exist in the same place. The simplest example of this is in electrical circuits, as the preceding section showed. In the general case, however, the simple equation 



P
=
I
V


{\displaystyle P=IV}

 must be replaced by a more complex calculation, the integral of the vector cross-product of the electrical and magnetic fields over a specified area, thus:






P

=

∫

S



E

×

H

⋅

d
A

.



{\displaystyle \mathbf {P} =\int _{S}\mathbf {E} \times \mathbf {H} \cdot \mathbf {dA} .\,}


The result is a scalar since it is the surface integral of the Poynting vector.

See also
Electricity
Nuclear Power
Fossil fuel power plant
ReferencesISBN links support NWE through referral fees
Croft, Terrell, and Wilford I. Summers. 1987. American Electricans' Handbook, 11th ed. New York: McGraw Hill. ISBN 0070139326
Fink, Donald G., and H. Wayne Beaty. 1978. Standard Handbook for Electrical Engineers, 11th ed. New York: McGraw Hill. ISBN 007020974X
Giancoli, Douglas. 2007. Physics for Scientists and Engineers, with Modern Physics (Chapters 1-37), 4th ed. Mastering Physics Series. Upper Saddle River, NJ: Prentice Hall. ISBN 978-0136139263
Tipler, Paul Allen, and Gene Mosca. 2004. Physics for Scientists and Engineers, Volume 2: Electricity and Magnetism, Light, Modern Physics, 5th ed. New York: W.H. Freeman. ISBN 0716708108
External links
All links retrieved September 18, 2017.

Electric power calculations

Credits
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