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'''Electrical elements''' are conceptual abstractions representing [[idealized]] [[electrical component]]s, such as [[resistor]]s, [[capacitor]]s, and [[inductor]]s, used in the [[circuit analysis|analysis]] of [[electrical network]]s. Any electrical network can be analysed as multiple, interconnected electrical elements in a [[Schematic diagram#Electronic industry|schematic diagram]] or [[circuit diagram]], each of which affects the [[voltage]] in the network or [[Current (electricity)|current]] through the network. These ideal electrical elements represent real, physical [[Electronic component|electrical or electronic components]] but they do not exist physically and they are assumed to have ideal properties according to a [[lumped element model]], while components are objects with less than ideal properties, a degree of uncertainty in their values and some degree of nonlinearity, each of which may require a combination of multiple electrical elements in order to approximate its function. | |||
Circuit analysis using electric elements is useful for understanding many practical electrical networks using components. By analyzing the way a network is affected by its individual elements it is possible to estimate how a real network will behave. | |||
==One-port elements== | |||
Only nine types of element ([[memristor]] not included), five passive and four active, are required to model any electrical component or circuit.{{Citation needed|date=March 2012}} Each element is defined by a relation between the [[state variable]]s of the network: [[Current (electricity)|current]], <math>I</math>; [[voltage]], <math>V</math>, [[Electric charge|charge]], <math>Q</math>; and [[magnetic flux]], <math>\Phi</math>. | |||
* Two sources: | |||
**[[Current source]], measured in [[ampere]]s – produces a current in a conductor. Affects charge according to the relation <math>dQ = -I\,dt</math>. | |||
**[[Voltage source]], measured in [[volt]]s – produces a [[potential difference]] between two points. Affects magnetic flux according to the relation <math>d\Phi = V\,dt</math>. | |||
::<math>\Phi</math> in this relationship does not necessarily represent anything physically meaningful. In the case of the current generator, <math>Q</math>, the time integral of current, represents the quantity of electric charge physically delivered by the generator. Here <math>\Phi</math> is the time integral of voltage but whether or not that represents a physical quantity depends on the nature of the voltage source. For a voltage generated by magnetic induction it is meaningful, but for an electrochemical source, or a voltage that is the output of another circuit, no physical meaning is attached to it. | |||
::Both these elements are necessarily non-linear elements. See [[#Non-linear elements]] below. | |||
* Three [[Passivity (engineering)|passive]] elements: | |||
**[[Electrical resistance|Resistance]] <math>R</math>, measured in [[Ohm (unit)|ohms]] – produces a voltage proportional to the current flowing through the element. Relates voltage and current according to the relation <math>dV = R\,dI</math>. | |||
**[[Capacitance]] <math>C</math>, measured in [[farad]]s – produces a current proportional to the rate of change of voltage across the element. Relates charge and voltage according to the relation <math>dQ = C\,dV</math>. | |||
**[[Inductance]] <math>L</math>, measured in [[Henry (unit)|henries]] – produces the magnetic flux proportional to the rate of change of current through the element. Relates flux and current according to the relation <math>d\Phi = L\,dI</math>. | |||
* Four abstract active elements: | |||
** Voltage-controlled voltage source (VCVS) Generates a voltage based on another voltage with respect to a specified gain. (has infinite input impedance and zero output impedance). | |||
** Voltage-controlled current source (VCCS) Generates a current based on a voltage elsewhere in the circuit, with respect to a specified gain, used to model [[field-effect transistor]]s and [[vacuum tube]]s (has infinite input impedance and infinite output impedance). The gain is characterised by a [[transfer conductance]] which will have units of [[Siemens (unit)|siemens]]. | |||
** Current-controlled voltage source (CCVS) Generates a voltage based on an input current elsewhere in the circuit with respect to a specified gain. (has zero input impedance and zero output impedance). The gain is characterised by a [[transfer impedance]] which will have units of [[ohm]]s. | |||
** Current-controlled current source (CCCS) Generates a current based on an input current and a specified gain. Used to model [[bipolar junction transistor]]s. (Has zero input impedance and infinite output impedance). | |||
::These four elements are examples of [[#Two-port elements|two-port elements]]. | |||
===Non-linear elements=== | |||
In reality, all circuit components are non-linear and can only be approximated to linear over a certain range. To more exactly describe the passive elements, their [[constitutive relation]] is used instead of simple proportionality. From any two of the circuit variables there are six constitutive relations that can be formed. From this it is supposed that there is a theoretical fourth passive element since there are only five elements in total (not including the various dependent sources) found in linear network analysis. This additional element is called [[memristor]]. It only has any meaning as a time-dependent non-linear element; as a time-independent linear element it reduces to a regular resistor. The constitutive relations of the passive elements are given by;<ref name=Trajkovic>Ljiljana Trajković, "Nonlinear circuits", ''The Electrical Engineering Handbook'' (Ed: Wai-Kai Chen), pp.75–77, Academic Press, 2005 ISBN 0-12-170960-4</ref> | |||
*Resistance: constitutive relation defined as <math>f(V, I)=0</math>. | |||
*Capacitance: constitutive relation defined as <math>f(V, Q)=0</math>. | |||
*Inductance: constitutive relation defined as <math>f(\Phi, I)=0</math>. | |||
*Memristance: constitutive relation defined as <math>f(\Phi, Q)=0</math>. | |||
:where <math>f(x,y)</math> is an arbitrary function of two variables. | |||
In some special cases the constitutive relation simplifies to a function of one variable. This is the case for all linear elements, but also for example, an ideal [[diode]], which in circuit theory terms is a non-linear resistor, has a constitutive relation of the form <math> V = f(I)</math>. Both independent voltage, and independent current sources can be considered non-linear resistors under this definition.<ref name=Trajkovic/> | |||
The fourth passive element, the memristor, was proposed by [[Leon Chua]] in a 1971 paper, but a physical component demonstrating memristance was not created until thirty-seven years later. It was reported on April 30, 2008, that a working memristor had been developed by a team at [[HP Labs]] led by scientist [[R. Stanley Williams]].<ref>{{citation|last=Strukov|first=Dmitri B|last2=Snider|first2=Gregory S|last3=Stewart|first3=Duncan R|last4=Williams|first4=Stanley R|title=The missing memristor found|journal=Nature|volume=453|pages=80–83|year=2008|doi=10.1038/nature06932|url=http://www.nature.com/nature/journal/v453/n7191/full/nature06932.html|pmid=18451858|issue=7191|bibcode=2008Natur.453...80S}}</ref><ref>EETimes, 30 April 2008, [http://www.eetimes.com/news/latest/showArticle.jhtml?articleID=207403521 'Missing link' memristor created], EETimes, 30 April 2008</ref><ref>[http://technology.newscientist.com/article/dn13812-engineers-find-missing-link-of-electronics.html Engineers find 'missing link' of electronics] – 30 April 2008</ref><ref>[http://www.physorg.com/news128786808.html Researchers Prove Existence of New Basic Element for Electronic Circuits – 'Memristor'] – 30 April 2008</ref> With the advent of the memristor, each pairing of the four variables can now be related. Because memristors are time-variant by definition, they are not included in [[LTI system theory|linear time-invariant (LTI)]] circuit models.{{cn|reason=they are not included because they are not linear surely. It is perfectly feasible to have a time invariant memristor as a theoretical ideal element|date=May 2013}} | |||
There are also two special non-linear elements which are sometimes used in analysis but which are not the ideal counterpart of any real component: | |||
*[[Nullator]]: defined as <math> V = I = 0 </math> | |||
*[[Norator]]: defined as an element which places no restrictions on voltage and current whatsoever. | |||
These are sometimes used in models of components with more than two terminals: transistors for instance.<ref name=Trajkovic/> | |||
==Two-port elements== | |||
All the above are two-terminal, or one-port, elements with the exception of the dependent sources. There are two lossless, passive, linear [[two-port network|two-port]] elements that are normally introduced into network analysis. Their constitutive relations in matrix notation are; | |||
;Transformer: | |||
: <math> \begin{bmatrix} V_1 \\ I_2 \end{bmatrix} = \begin{bmatrix} 0 & n \\ -n & 0 \end{bmatrix}\begin{bmatrix} I_1 \\ V_2 \end{bmatrix}</math> | |||
;Gyrator: | |||
: <math> \begin{bmatrix} V_1 \\ V_2 \end{bmatrix} = \begin{bmatrix} 0 & -r \\ r & 0 \end{bmatrix}\begin{bmatrix} I_1 \\ I_2 \end{bmatrix}</math> | |||
The transformer maps a voltage at one port to a voltage at the other in a ratio of ''n''. The current between the same two port is mapped by 1/''n''. The [[gyrator]], on the other hand, maps a voltage at one port to a current at the other. Likewise, currents are mapped to voltages. The quantity ''r'' in the matrix is in units of resistance. The gyrator is a necessary element in analysis because it is not [[Reciprocity_(electromagnetism)#Reciprocity_for_electrical_networks|reciprocal]]. Networks built from the basic linear elements only are obliged to be reciprocal and so cannot be used by themselves to represent a non-reciprocal system. It is not essential, however, to have both the transformer and gyrator. Two gyrators in cascade are equivalent to a transformer but the transformer is usually retained for convenience. Introduction of the gyrator also makes either capacitance or inductance non-essential since a gyrator terminated with one of these at port 2 will be equivalent to the other at port 1. However, transformer, capacitance and inductance are normally retained in analysis because they are the ideal properties of the basic physical components [[transformer]], [[inductor]] and [[capacitor]] whereas a [[Gyrator#Implementation: a simulated inductor|practical gyrator]] must be constructed as an active circuit.<ref>Wadhwa, C.L., ''Network analysis and synthesis'', pp.17–22, New Age International, ISBN 81-224-1753-1.</ref><ref>Herbert J. Carlin, Pier Paolo Civalleri, ''Wideband circuit design'', pp.171–172, CRC Press, 1998 ISBN 0-8493-7897-4.</ref><ref>Vjekoslav Damić, John Montgomery, ''Mechatronics by bond graphs: an object-oriented approach to modelling and simulation'', pp.32–33, Springer, 2003 ISBN 3-540-42375-3.</ref> | |||
==Examples== | |||
The following are examples of representation of components by way of electrical elements. | |||
* On a first degree of approximation, a [[battery (electricity)|battery]] is represented by a voltage source. A more refined model also includes a resistance in series with the voltage source, to represent the battery's internal resistance (which results in the battery heating and the voltage dropping when in use). A current source in parallel may be added to represent its leakage (which discharges the battery over a long period of time). | |||
* On a first degree of approximation, a [[resistor]] is represented by a resistance. A more refined model also includes a series inductance, to represent the effects of its lead inductance (resistors constructed as a spiral have more significant inductance). A capacitance in parallel may be added to represent the capacitive effect of the proximity of the resistor leads to each other. A wire can be represented as a low-value resistor | |||
* Current sources are more often used when representing [[semiconductor]]s. For example, on a first degree of approximation, a bipolar [[transistor]] may be represented by a variable current source that is controlled by the input current. | |||
==See also== | |||
{{Commons|Electronic devices}} | |||
* [[Electronic component]] | |||
* [[Lumped element model]] | |||
* [[Distributed element model]] | |||
* [[Transmission line]] | |||
==References== | |||
{{Reflist}} | |||
{{DEFAULTSORT:Electrical Element}} | |||
[[Category:Electronics]] | |||
[[Category:Electrical systems]] | |||
[[ar:عنصر كهربائي]] | |||
[[ta:மின் உறுப்புகள்]] |
Revision as of 12:08, 12 July 2013
Electrical elements are conceptual abstractions representing idealized electrical components, such as resistors, capacitors, and inductors, used in the analysis of electrical networks. Any electrical network can be analysed as multiple, interconnected electrical elements in a schematic diagram or circuit diagram, each of which affects the voltage in the network or current through the network. These ideal electrical elements represent real, physical electrical or electronic components but they do not exist physically and they are assumed to have ideal properties according to a lumped element model, while components are objects with less than ideal properties, a degree of uncertainty in their values and some degree of nonlinearity, each of which may require a combination of multiple electrical elements in order to approximate its function.
Circuit analysis using electric elements is useful for understanding many practical electrical networks using components. By analyzing the way a network is affected by its individual elements it is possible to estimate how a real network will behave.
One-port elements
Only nine types of element (memristor not included), five passive and four active, are required to model any electrical component or circuit.Potter or Ceramic Artist Truman Bedell from Rexton, has interests which include ceramics, best property developers in singapore developers in singapore and scrabble. Was especially enthused after visiting Alejandro de Humboldt National Park. Each element is defined by a relation between the state variables of the network: current, ; voltage, , charge, ; and magnetic flux, .
- Two sources:
- Current source, measured in amperes – produces a current in a conductor. Affects charge according to the relation .
- Voltage source, measured in volts – produces a potential difference between two points. Affects magnetic flux according to the relation .
- in this relationship does not necessarily represent anything physically meaningful. In the case of the current generator, , the time integral of current, represents the quantity of electric charge physically delivered by the generator. Here is the time integral of voltage but whether or not that represents a physical quantity depends on the nature of the voltage source. For a voltage generated by magnetic induction it is meaningful, but for an electrochemical source, or a voltage that is the output of another circuit, no physical meaning is attached to it.
- Both these elements are necessarily non-linear elements. See #Non-linear elements below.
- Three passive elements:
- Resistance , measured in ohms – produces a voltage proportional to the current flowing through the element. Relates voltage and current according to the relation .
- Capacitance , measured in farads – produces a current proportional to the rate of change of voltage across the element. Relates charge and voltage according to the relation .
- Inductance , measured in henries – produces the magnetic flux proportional to the rate of change of current through the element. Relates flux and current according to the relation .
- Four abstract active elements:
- Voltage-controlled voltage source (VCVS) Generates a voltage based on another voltage with respect to a specified gain. (has infinite input impedance and zero output impedance).
- Voltage-controlled current source (VCCS) Generates a current based on a voltage elsewhere in the circuit, with respect to a specified gain, used to model field-effect transistors and vacuum tubes (has infinite input impedance and infinite output impedance). The gain is characterised by a transfer conductance which will have units of siemens.
- Current-controlled voltage source (CCVS) Generates a voltage based on an input current elsewhere in the circuit with respect to a specified gain. (has zero input impedance and zero output impedance). The gain is characterised by a transfer impedance which will have units of ohms.
- Current-controlled current source (CCCS) Generates a current based on an input current and a specified gain. Used to model bipolar junction transistors. (Has zero input impedance and infinite output impedance).
- These four elements are examples of two-port elements.
Non-linear elements
In reality, all circuit components are non-linear and can only be approximated to linear over a certain range. To more exactly describe the passive elements, their constitutive relation is used instead of simple proportionality. From any two of the circuit variables there are six constitutive relations that can be formed. From this it is supposed that there is a theoretical fourth passive element since there are only five elements in total (not including the various dependent sources) found in linear network analysis. This additional element is called memristor. It only has any meaning as a time-dependent non-linear element; as a time-independent linear element it reduces to a regular resistor. The constitutive relations of the passive elements are given by;[1]
- Resistance: constitutive relation defined as .
- Capacitance: constitutive relation defined as .
- Inductance: constitutive relation defined as .
- Memristance: constitutive relation defined as .
In some special cases the constitutive relation simplifies to a function of one variable. This is the case for all linear elements, but also for example, an ideal diode, which in circuit theory terms is a non-linear resistor, has a constitutive relation of the form . Both independent voltage, and independent current sources can be considered non-linear resistors under this definition.[1]
The fourth passive element, the memristor, was proposed by Leon Chua in a 1971 paper, but a physical component demonstrating memristance was not created until thirty-seven years later. It was reported on April 30, 2008, that a working memristor had been developed by a team at HP Labs led by scientist R. Stanley Williams.[2][3][4][5] With the advent of the memristor, each pairing of the four variables can now be related. Because memristors are time-variant by definition, they are not included in linear time-invariant (LTI) circuit models.Template:Cn
There are also two special non-linear elements which are sometimes used in analysis but which are not the ideal counterpart of any real component:
- Nullator: defined as
- Norator: defined as an element which places no restrictions on voltage and current whatsoever.
These are sometimes used in models of components with more than two terminals: transistors for instance.[1]
Two-port elements
All the above are two-terminal, or one-port, elements with the exception of the dependent sources. There are two lossless, passive, linear two-port elements that are normally introduced into network analysis. Their constitutive relations in matrix notation are;
- Transformer
- Gyrator
The transformer maps a voltage at one port to a voltage at the other in a ratio of n. The current between the same two port is mapped by 1/n. The gyrator, on the other hand, maps a voltage at one port to a current at the other. Likewise, currents are mapped to voltages. The quantity r in the matrix is in units of resistance. The gyrator is a necessary element in analysis because it is not reciprocal. Networks built from the basic linear elements only are obliged to be reciprocal and so cannot be used by themselves to represent a non-reciprocal system. It is not essential, however, to have both the transformer and gyrator. Two gyrators in cascade are equivalent to a transformer but the transformer is usually retained for convenience. Introduction of the gyrator also makes either capacitance or inductance non-essential since a gyrator terminated with one of these at port 2 will be equivalent to the other at port 1. However, transformer, capacitance and inductance are normally retained in analysis because they are the ideal properties of the basic physical components transformer, inductor and capacitor whereas a practical gyrator must be constructed as an active circuit.[6][7][8]
Examples
The following are examples of representation of components by way of electrical elements.
- On a first degree of approximation, a battery is represented by a voltage source. A more refined model also includes a resistance in series with the voltage source, to represent the battery's internal resistance (which results in the battery heating and the voltage dropping when in use). A current source in parallel may be added to represent its leakage (which discharges the battery over a long period of time).
- On a first degree of approximation, a resistor is represented by a resistance. A more refined model also includes a series inductance, to represent the effects of its lead inductance (resistors constructed as a spiral have more significant inductance). A capacitance in parallel may be added to represent the capacitive effect of the proximity of the resistor leads to each other. A wire can be represented as a low-value resistor
- Current sources are more often used when representing semiconductors. For example, on a first degree of approximation, a bipolar transistor may be represented by a variable current source that is controlled by the input current.
See also
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References
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ar:عنصر كهربائي ta:மின் உறுப்புகள்
- ↑ 1.0 1.1 1.2 Ljiljana Trajković, "Nonlinear circuits", The Electrical Engineering Handbook (Ed: Wai-Kai Chen), pp.75–77, Academic Press, 2005 ISBN 0-12-170960-4
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- ↑ Engineers find 'missing link' of electronics – 30 April 2008
- ↑ Researchers Prove Existence of New Basic Element for Electronic Circuits – 'Memristor' – 30 April 2008
- ↑ Wadhwa, C.L., Network analysis and synthesis, pp.17–22, New Age International, ISBN 81-224-1753-1.
- ↑ Herbert J. Carlin, Pier Paolo Civalleri, Wideband circuit design, pp.171–172, CRC Press, 1998 ISBN 0-8493-7897-4.
- ↑ Vjekoslav Damić, John Montgomery, Mechatronics by bond graphs: an object-oriented approach to modelling and simulation, pp.32–33, Springer, 2003 ISBN 3-540-42375-3.