Submitted by Sudeepta Pramanik on Fri, 06/17/2011 - 19:29

RESISTOR:

ResistorResistor is energy absorbing element in electrical circuit. It's unit is ohm.

The potential difference v across the terminals of resistor R, is directly proportional to the current i flowing through it.

That is,

           V=IR; Here R is called the resistance of resistor R

The reciprocal of resistance is defined as conductance( G).

Hence,

         (1/R)=G    &     I=VG

The power absorbed by a resistor is given by

         P=VI

 

INDUCTOR:

inductorInductor is an energy storing element in electrical circuit. It's unit is henry.

The potential difference v across the terminals of inductor is directly proportional to rate of change of current through it.

That is, [tex]V = L\frac{{di}}{{dt}}[/tex]; Here the term L is the proportionality constant and known as inductance of the inductor.

Hence, current through inductor is

                                                     [tex]I = \frac{1}{L}\int\limits_0^t {} Vdt + I(0)[/tex]

Where I(0) is the initial current of the inductor.

The energy stored in an inductor over the interval [tex]\left( {{t_1},{t_2}} \right)[/tex] is,

        [tex]E\left( {{t_1},{t_2}} \right) = \int\limits_{{t_1}}^{{t_2}} {VIdt = \int\limits_{{t_1}}^{{t_2}} {L(dI/dt)} } Idt = \frac{L}{2}[\mathop I\nolimits^2 ({t_2})\_\mathop I\nolimits^2 ({t_1})][/tex]

Inductor store the energy in the form of current.

    

CAPACITOR:

capacitorCapacitor is another energy storing element in electrical circuit. It's unit is farad.

The potential difference v between the terminals of capacitor is proportional to the charge q on it. That is

                                                                          [tex]v \propto q[/tex]

                                                                           v=q/C; where C is the proportionality constant and is called the capacitance.

Now, [tex]i = \frac{{dq}}{{dt}} = C(\frac{{dv}}{{dt}})[/tex]

         [tex]\int {dv = \frac{1}{C}\int {idt} } [/tex]

Hence, [tex]V(t) = \frac{1}{C}\int\limits_0^t {i(t)dt}  + q(0)/C[/tex]

where q(0) is the initial charge across the capacitor C.

The energy stored in a capacitor over the interval [tex]\left( {{t_1},{t_2}} \right)[/tex] is,

[tex]E\left( {{t_1},{t_2}} \right) = \int\limits_{{t_1}}^{{t_2}} {VIdt = \int\limits_{{t_1}}^{{t_2}} {VC(dv/dt)} } dt = \frac{C}{2}[\mathop V\nolimits^2 ({t_2})\_\mathop V\nolimits^2 ({t_1})][/tex]

Capacitor store the energy in the form of voltage.

 

 

Comments

Related Items

Elecrical Circuit Theory and Networks

1. Basic Circuit Elements and Waveforms | 2. Mesh and Node Analysis | 3. Graph Theory and Network Equation | 4. Fourier Series | 5. The Laplace Transform | 6. Application Laplace Transform | 7. Network Theorems | 8. Resonance | 9. Analogous System ....

Definitions of Electrical Circuits

An electric circuit is a path of connected elements in which electrons can flow from a voltage or current source. Before going into discussion of network analysis or Circuit is required to know certain definitions.

Conservation of Energy

The law of conservation of energy states that energy cannot be created no destroyed, but it can be converted from one form to other. Electrical technology isn't also against it. Here are some examples of energy conservation which belongs to electrical technology.

Standard Input Signals

A signal is function of independent variable that carry some information. Practically the input and also output signals of any system are complex (they are combination of other signal) in nature. Thus it is being tough to analyze the characteristic performance of any system by those signal.

Magnetic Coupling

A magnetic coupling is a coupling where energy can be transferred from one circuit to another, not connected through any physical mechanical connection but using magnetic flux