Search results
Results from the WOW.Com Content Network
In the special case of entirely zero admittance or exactly zero impedance, the relations are encumbered by infinities. However, for purely-reactive impedances (which are purely-susceptive admittances), the susceptance is equal to the negative reciprocal of the reactance, except when either is zero. In mathematical notation:
In electrical engineering, impedance is the opposition to alternating current presented by the combined effect of resistance and reactance in a circuit. [1]Quantitatively, the impedance of a two-terminal circuit element is the ratio of the complex representation of the sinusoidal voltage between its terminals, to the complex representation of the current flowing through it. [2]
In electrochemistry, faradaic impedance [1] [2] is the resistance and capacitance acting jointly at the surface of an electrode of an electrochemical cell.The cell may be operating as either a galvanic cell generating an electric current or inversely as an electrolytic cell using an electric current to drive a chemical reaction.
In electrical circuits, reactance is the opposition presented to alternating current by inductance and capacitance. [1] Along with resistance, it is one of two elements of impedance; however, while both elements involve transfer of electrical energy, no dissipation of electrical energy as heat occurs in reactance; instead, the reactance stores energy until a quarter-cycle later when the energy ...
Reactance is the imaginary part of the complex electrical impedance.Both capacitors and inductors possess reactance (but of opposite sign) and are frequency dependent. The specification that the network must be passive and lossless implies that there are no resistors (lossless), or amplifiers or energy sources (passive) in the network.
For a generic multi-port network definition, it is assumed that each of the ports is allocated an integer n ranging from 1 to N, where N is the total number of ports. For port n , the associated Z-parameter definition is in terms of the port current and port voltage, I n {\displaystyle I_{n}\,} and V n {\displaystyle V_{n}\,} respectively.
The electrical impedance of this circuit is easily obtained remembering the impedance of a capacitance which is given by: = where is the angular frequency of a sinusoidal signal (rad/s), and =. It is obtained: Z ( ω ) = R t 1 + R t C dl i ω {\displaystyle Z(\omega )={\frac {R_{\text{t}}}{1+R_{\text{t}}C_{\text{dl}}i\omega }}}
Decreased impedance is implemented by an inverting amplifier having some moderate gain, usually < <. It may be observed as an undesired Miller effect in common-emitter, common-source and common-cathode amplifying stages where effective input capacitance is increased.