Voltage
32549
224498758
2008-07-09T03:11:26Z
Gerry Ashton
1479481
better without the comma
[[Image:High voltage warning.svg|right|thumb|International safety symbol "Caution, risk of electric shock" (ISO 3864), colloquially known as [[High voltage|''high voltage'']]'' symbol''.]]
'''Voltage''' (sometimes also called ''electric'' or ''electrical tension'') is the [[potential difference|difference of electrical potential]] between two points of an electrical or [[electronic circuit]], expressed in [[volt]]s.<ref>"voltage", ''A Dictionary of Physics''. Ed. John Daintith. Oxford University Press, 2000. Oxford Reference Online. Oxford University Press.</ref> It measures the potential energy of an [[electric field]] to cause an [[electric current]] in an [[electrical conductor]]. Depending on the difference of electrical potential it is called [[extra low voltage]], [[low voltage]], [[high voltage]] or [[extra high voltage]]. Specifically Voltage is equal to energy per unit charge.
==Explanation==
Between two points in an electric field, such as exists in an [[electrical circuit]], the difference in their [[electrical potential]]s is known as the electrical potential difference. This difference is directly [[Proportionality (mathematics)|proportional]] to the force that tends to push [[electron]]s or other charge-carriers from one point to the other. Electrical potential difference can be thought of as the ability to move electrical charge through a resistance. At a time in physics when the word ''force'' was used loosely, the potential difference was named the [[electromotive force]] or '''EMF'''—a term which is still used in certain contexts.
Voltage is a property of an [[electric field]], not individual electrons. {{Fact|date=May 2008}}An electron moving across a voltage difference experiences a net change in energy, often measured in [[electron-volt]]s. This effect is analogous to a mass falling through a given height difference in a [[gravitational field]].
'''
When using the term 'potential difference' or voltage, one must be clear about the two points between which the voltage is specified or measured. There are two ways in which the term is used. This can lead to some confusion.'''
===Voltage with respect to a common point===
One way in which the term voltage is used is when specifying the voltage of a point in a circuit. When this is done, it is understood that the voltage is usually being specified or measured with respect to a stable and unchanging point in the circuit that is known as [[ground]] or common. This voltage is really a voltage difference, one of the two points being the reference point, which is ground. A voltage can be positive or negative. "High" or "low" voltage may refer to the magnitude (the absolute value relative to the reference point). Thus, a large negative voltage may be referred to as a high voltage. Other authors may refer to a voltage that is more negative as being "lower".
===Voltage between two stated points===
Another usage of the term "voltage" is in specifying how many volts are across an electrical device (such as a resistor). In this case, the "voltage," or, more accurately, the "voltage across the device," is really the first voltage taken, relative to ground, on one terminal of the device minus a second voltage taken, relative to ground, on the other terminal of the device. In practice, the voltage across a device can be measured directly and safely using a [[voltmeter]] that is isolated from ground, provided that the maximum voltage capability of the voltmeter is not exceeded.
Two points in an electric circuit that are connected by an "ideal conductor," that is, a conductor without resistance and not within a changing [[magnetic field]], have a potential difference of zero. However, other pairs of points may also have a potential difference of zero. If two such points are connected with a conductor, no current will flow through the connection.
=== Addition of voltages ===
Voltage is additive in the following sense: the voltage between ''A'' and ''C'' is the sum of the voltage between ''A'' and ''B'' and the voltage between ''B'' and ''C''. The various voltages in a circuit can be computed using [[Kirchhoff's circuit laws]].
When talking about [[alternating current]] (AC) there is a difference between instantaneous voltage and average voltage. Instantaneous voltages can be added as for [[direct current]] (DC), but average voltages can be meaningfully added only when they apply to signals that all have the same frequency and phase.
=== Hydraulic analogy ===
{{main|Hydraulic analogy}}
If one imagines water circulating in a network of pipes, driven by pumps in the absence of [[gravity]], as an [[analogy]] of an electrical circuit, then the potential difference corresponds to the [[fluid pressure]] difference between two points. If there is a pressure difference between two points, then water flowing from the first point to the second will be able to do work, such as driving a [[turbine]].
This ''hydraulic analogy'' is a useful method of teaching a range of electrical concepts. In a hydraulic system, the work done to move water is equal to the [[pressure]] multiplied by the [[volume]] of water moved. Similarly, in an electrical circuit, the work done to move electrons or other charge-carriers is equal to 'electrical pressure' (an old term for voltage) multiplied by the quantity of electrical charge moved. Voltage is a convenient way of quantifying the ability to do work. In relation to electric current, the larger the gradient (voltage or hydraulic) the greater the current (assuming resistance is constant).
===Mathematical definition===
The electrical potential difference is defined as the amount of [[energy|work]] needed to move a unit [[electric charge]] from the second point to the first, or equivalently, the amount of work that a unit charge flowing from the first point to the second can perform. The potential difference between two points a and b is the [[line integral]] of the electric field '''E''':
: <math>V_a - V_b = \int _a ^b \mathbf{E}\cdot d\mathbf{l}.</math>
==Useful formulas==
===DC circuits===
: <math> V = \sqrt{PR} </math>
: <math> R = \frac{V}{I} </math>
where ''V'' = potential difference (volts), ''I'' = current intensity (amps), ''R'' = resistance (ohms), ''P'' = power (watts).
===AC circuits===
:<math> V = \frac{P}{I\cos\phi}</math>
:<math> V = \frac{\sqrt{PZ}}{\sqrt{\cos\phi}} \!\ </math>
:<math> V = \frac{IR}{\cos\phi}</math>
Where ''V''=voltage, ''I''=curr, ''R''=resistance, ''P''=true power, ''Z''=impedance, ''φ''=phasor angle between ''I'' and ''V''
===AC conversions===
:<math> V_{avg} = .637\,V_{pk} = \frac{2}{\pi} V_{pk} = \frac{\omega}{\pi}\int_0^{\pi/\omega} V_{pk} \sin(\omega t - k x) {\rm{d}}x \!\ </math>
:<math> V_{rms} = .707\,V_{pk} = \frac{1}{\sqrt{2}} V_{pk} = V_{pk} \sqrt{\langle \sin^2(\omega t - k x) \rangle} \!\ </math>
:<math> V_{pk} = 0.5\,V_{ppk} \!\ </math>
:<math> V_{avg} = .319\,V_{ppk}\!\ </math>
:<math> V_{rms} = .354\,V_{ppk} = \frac{1}{2 \sqrt{2}} V_{ppk}\!\ </math>
:<math> V_{avg} = 0.900\,V_{rms} = \frac{2 \sqrt{2}}{\pi} V_{rms}\!\ </math>
Where ''V''<sub>pk</sub>=peak voltage, ''V''<sub>ppk</sub>=peak-to-peak voltage, ''V''<sub>avg</sub>=average voltage over a half-cycle, ''V''<sub>rms</sub>=effective ([[root mean square]]) voltage, and we assumed a sinusoidal wave of the form <math> V_{pk} \sin(\omega t - k x) </math>, with a period <math> T = 2\pi/\omega </math>, and where the angle brackets (in the root-mean-square equation) denote a time average over an entire period.
===Total voltage===
Voltage sources and drops in series:
:<math> V_T = V_1 + V_2 + V_3 + ... + V_n \!\ </math>
Voltage sources and drops in parallel:
:<math> V_T = V_1 = V_2 = V_3 = ... = V_n \!\ </math>
Where <math> n \!\ </math> is the nth voltage source or drop
===Voltage drops===
Across a resistor (Resistor R):
:<math> V_R = IR_R \!\ </math>
Across a capacitor (Capacitor C):
:<math> V_C = IX_C \!\ </math>
Across an inductor (Inductor L):
:<math> V_L = IX_L \!\ </math>
Where ''V''=voltage, ''I''=current, ''R''=resistance, ''X''=reactance.
== Measuring instruments ==
[[Image:Digital Multimeter Aka.jpg|thumb|A [[multimeter]] set to measure voltage.]]
Instruments for measuring potential differences include the [[voltmeter]], the [[potentiometer]] (measurement device), and the [[oscilloscope]]. The voltmeter works by measuring the current through a fixed resistor, which, according to [[Ohm's Law]], is proportional to the potential difference across the resistor. The potentiometer works by balancing the unknown voltage against a known voltage in a [[bridge circuit]]. The cathode-ray oscilloscope works by amplifying the potential difference and using it to deflect an [[electron]] beam from a straight path, so that the deflection of the beam is proportional to the potential difference.
== Safety ==
Electrical safety is discussed in the articles on [[High voltage]] (note that even low voltage, e. g. of 50 Volts, can lead to a lethal electric shock) and '''[[Electric shock]].'''
==See also==
{{portalpar|Electronics|Nuvola_apps_ksim.png}}
* [[Alternating current]] (AC)
* [[Direct current]] (DC)
* [[Mains electricity]] (an article about domestic power supply voltages)
* [[Mains power systems]] (List of voltage by country)
* [[Ohm's law]]
* [[Voltage drop]]
==References==
<references/>
==External links==
{{Wiktionary}}
*[http://www.ndt-ed.org/EducationResources/HighSchool/Electricity/voltage.htm Elementary explanation of voltage at NDT Resource Center]
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