Lecture
Electrical elements are conceptual abstractions representing idealized electrical components, such as resistors, capacitors, and inductors, used in the analysis of electrical networks. All electrical networks can be analyzed as a number of electrical elements interconnected by wires. Where the elements correspond roughly to real components, the representation may take the form of a schematic diagram or electrical circuit. This is called a lumped-element circuit model. In other cases, infinitesimal elements are used to model the network in a distributed-element model.
These ideal electrical elements represent real, physical electrical or electronic components, but they do not exist physically, and are assumed to have ideal properties, whereas actual electrical components have less-than-ideal properties, some degree of uncertainty in their values, and some degree of nonlinearity. To model the non-ideal behavior of a real circuit component, it may be necessary to combine several ideal electrical elements in order to approximate its function. For example, an inductor circuit element is assumed to have inductance but no resistance or capacitance, while a real inductor, a coil of wire, has some resistance in addition to its inductance. This can be modeled by means of an ideal inductive element in series with a resistance.
Analyzing a circuit using electrical elements is useful for understanding many practical electrical networks that use components. By analyzing the network's response affected by its individual elements, one can estimate how the real network will behave.
Circuit elements can be classified in different categories. One is by how many terminals they need to connect them to other components:
Elements can also be divided into active and passive:
Another distinction is between linear and nonlinear:
Only nine types of elements (the memristor is not included), five passive and four active, are needed to model any electrical component or circuit. Each element is defined by a relationship between the network's state variables: current, ; voltage, ; charge, ; and magnetic flux, .
in these relations does not necessarily represent anything physically meaningful. In the case of a current generator, , the time integral of the current, represents the amount of electric charge physically supplied by the generator. Here there is a time integral of the voltage, but whether or not it represents a physical quantity depends on the nature of the voltage source. For a voltage generated by magnetic induction, it makes sense, but for an electrochemical source, or a voltage that is the output of another circuit, no physical meaning is attached to it.
Both of these elements are necessarily nonlinear elements. See #Nonlinear Elements below.
These four elements are examples of two-port elements.

Conceptual symmetries of the resistor, capacitor, inductor, and memristor.
In reality, all circuit components are nonlinear and can only be approximated as linear within a certain range. In order to describe passive elements more accurately, their constitutive relation is used instead of simple proportionality. From any two circuit variables, six constitutive relations can be formed. From this it can be assumed 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 a memristor. It has meaning only as a time-dependent nonlinear element; as a time-independent linear element it reduces to a regular resistor. Consequently, it is not included in linear time-invariant (LTI) circuit models. The constitutive relations of the passive elements are defined as follows:
where 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, for the ideal diode, which from the point of view of circuit theory is a nonlinear resistor, has a constitutive relation of the form. Both independent voltage and independent current sources can be regarded as nonlinear resistors under this definition.
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 of specialists at HP Labs led by scientist R. Stanley Williams. With the advent of memristors, every pairing of the four variables could be related to one another.
There are also two special nonlinear elements which are sometimes used in analysis but are not the ideal analogue of any real component:
They are sometimes used in models of components with more than two terminals: transistors, for example.
All of 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 commonly introduced in network analysis. Their constitutive relations in matrix form are as follows:
Transformer
Gyrator
The transformer maps the voltage at one port to the voltage at the other in the ratio n. Meanwhile, the currents between the same two ports are mapped by 1/n. The gyrator, on the other hand, maps the voltage at one port to the current at the other. Likewise, currents are transformed into voltages. The quantity r in the matrix is in units of resistance. The gyrator is a necessary element in analysis because it is non-reciprocal. Networks built from basic linear elements alone are required to be reciprocal and therefore cannot by themselves represent a non-reciprocal system. It is not necessary, however, to have both a transformer and a gyrator. Two gyrators in cascade are equivalent to a transformer, but a transformer is usually retained for convenience. The introduction of the gyrator also makes either capacitance or inductance redundant, since a gyrator terminated with one of them at port 2 will be equivalent to the other at port 1. However, the transformer, capacitor, and inductor are generally retained in analysis, since they are the ideal properties of the basic physical components of the transformer, inductor, and capacitor, whereas in a practical gyrator they must be implemented as an active circuit.
Below are examples of representing components by means of electrical elements.
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