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Constant314 (talk | contribs) Restored revision 1191431161 by Constant314 (talk): It is a series circuit. Always has been. |
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{{Use dmy dates|date=July 2019|cs1-dates=y}}
{{Use list-defined references|date=December 2021}}
[[File:Series circuit.svg|thumb|A
[[Terminal (electronics)|Two-terminal]] components and [[electrical networks]] can be connected in '''series'''
Components connected in
Components connected in parallel are connected along multiple paths, and each component has the same [[voltage]] across it, equal to the voltage across the network. The current through the network is equal to the sum of the currents through each component.
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The two preceding statements are equivalent, except for [[Duality (electrical circuits)|exchanging the role of voltage and current]].
A circuit composed solely of components connected in series is known as a '''
In a
Consider a very simple circuit consisting of four light bulbs and a 12-volt [[automotive battery]]. If a wire joins the battery to one bulb, to the next bulb, to the next bulb, to the next bulb, then back to the battery in one continuous loop, the bulbs are said to be in series. If each bulb is wired to the battery in a separate loop, the bulbs are said to be in parallel. If the four light bulbs are connected in series, the same current flows through all of them and the voltage drop is 3 volts across each bulb, which may not be sufficient to make them glow. If the light bulbs are connected in parallel, the currents through the light bulbs combine to form the current in the battery, while the voltage drop is 12 volts across each bulb and they all glow.
In a
==
<!-- "Series circuit" redirects here. "Battery (electricity)" links here. -->
{{Electromagnetism|Network}}
'''
A
===Current<span class="anchor" id="Iseries"></span>===
<math display="block">I = I_1 = I_2 = \cdots = I_n</math>
In a
===Voltage===
In a
<math display="block">V = V_1 + V_2 + \dots + V_n = I \left( R_1 + R_2 + \dots + R_n \right)</math>
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==== Conductance ====
[[Electrical conductance]] presents a reciprocal quantity to resistance. Total conductance of a
<math display="block">\frac{1}{G_\text{total}} = \frac{1}{G_1} + \frac{1}{G_2} + \cdots + \frac{1}{G_n}.</math>
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==Applications==
A common application of
Series resistance can also be applied to the arrangement of blood vessels within a given organ. Each organ is supplied by a large artery, smaller arteries, arterioles, capillaries, and veins arranged in series. The total resistance is the sum of the individual resistances, as expressed by the following equation: {{math|1=''R''<sub>total</sub> = ''R''<sub>artery</sub> + ''R''<sub>arterioles</sub> + ''R''<sub>capillaries</sub>}}. The largest proportion of resistance in this series is contributed by the arterioles.<ref name="BRS"/>
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}}
==Further reading==
* {{cite book |author-last=Williams |author-first=Tim |title=The Circuit Designer's Companion |publisher=[[Butterworth-Heinemann]] |date=2005 |isbn=0-7506-6370-7 }}
* {{cite magazine |url=http://www.edn.com/design/components-and-packaging/4421194/Resistor-combinations--How-many-values-using-1kohm-resistors-- |title=Resistor combinations: How many values using 1K ohm resistors? |magazine=[[EDN magazine]] }}
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