Resistance is proportional to the length and inversely Symbol of a resistor X R Resistance is proportional to the length and inversely proportional to the cross sectional area of the material Where, is defined as resistivity, in Ohm-meter ( ), which is simply the resistance per unit length times cross-sectional area.

Series connection Parallel connection X Y (a) (b) Resistances connected in series and parallel are calculated using the following formula.

L X Y Symbol Purpose-made conductor coils are called inductors. When current flows electromagnetic field is established. The electromagnetic lines of force surrounds the conductor and the magnetic lines of force becomes concentrated. When the current changes, the electromagnetic field changes accordingly and the changing electromagnetic field causes an induced voltage in a direction in opposite to the flow of current. This property is referred to as inductance.

Surface-1 Surface-2 Electrode-1 Electrode-2 Dielectric material C X Y A capacitor is an energy storage passive component. The term capacity signifies "what is the capacity of the surfaces in holding the electrical charges." It stores charge and hence electric field energy. The equivalent capacitance of a series combination is always less than any individual capacitance in the combination and can be expressed using the following equation. On the other hand, the parallel connection adds up all the individual capacitances

Inductive reactance versus inductance and frequency curve. Capacitance Capacitive reactance (b) Inductive reactance versus inductance and frequency curve. Capacitive reactance versus capacitance and frequency curve.

p-type Semiconductor material Immobile Acceptor atoms (Trivalent) A piece of intrinsic Semiconductor material n-type Semiconductor material Immobile Donor atoms (Pentavalent) _ (a) (b) (c) Terminal Flow of current Flow of electrons Flow of holes A B If the donors are added, the intrinsic semicond-uctor becomes n-type semiconductor and if the acceptors are added it becomes p-type semicon-ductor. n-type semico-nductor materials have loosely-attached free-electrons and p-type semiconductor materials have loosely-attached free-holes. The electrons and holes, in the respective extrinsic semi conductors, are called charge carriers

A depletion layer is a layer in which the charge carriers are absent p-type n-type + - Majority carriers (holes) Majority carriers (electrons) Depletion layer Uncovered immobile atoms Potential barrier Electrode (a) (b) Semiconductor diodes or junction diodes are two terminal electronic devices made up of two types of semiconductor materials. One side of the device has n-type material and the other side has p-type. A depletion layer is a layer in which the charge carriers are absent

+ - Voltage source Forward-biased p-n junction diode Reverse-biased p-n junction diode (a) (b) Voltage in volts Current is mA I is the diode current, q is charge of the carriers, k is a constant, V is the applied voltage T is temp. in degrees K The behavior of a junction diode is such that it offers a low resistance to electric current in one direction and a high resistance to it in the reverse direction. This property is a requirement in the context of signal manipulation and processing. The current equation in the diode is given above.

Varactor exploits the depletion layer in terms of a parallel plate Reverse voltage Capacitance Diode voltage Current Negative coefficient of resistance Varacter Tunnel Varactor exploits the depletion layer in terms of a parallel plate capacitor, whose capacitance is controlled by applying reverse voltage. The capacitance across the junction is inversely proportional to the width of the depletion layer. The varactors useful for designing VCO, FM modulators and demodulators and tuning circuits. In the tunnel diode, the current through the device decreases as the voltage increases within a certain range This property, known as negative resistance, makes it useful as a switch and oscillators.

(Common to both input and Output) + - Diode Common terminal called GROUND (Common to both input and Output) Amplitude Time (b) (a) (c) (d) In general, junction diodes are referred to as rectifiers because when an alternating signal (voltage or current) say a sinusoidal or rectangular signal is applied (assuming ideal diode) the output would be a signal containing only positive half-cycles.

A pnp transistor (b) An npn transistor (c) Symbol of a pnp Emitter (E) Collector (C) Emitter (E) Collector (C) P N P N P N A pnp transistor (b) An npn transistor (c) Symbol of a pnp (d) Symbol of npn Base (B) Base (B) (a) (b) C B E p-n-p (Symbol) (d) C B n-p-n (Symbol) E (c) E C n-p-n B C E input Output Common-emitter configuration C input B n-p-n n-p-n Output Input Output B E Common-collector configuration Common-base configuration (e) (f) (g) (e) The common emitter configuration of an n-p-n transistor (f) the common collector configuration of an n-p-n transistor (g) The common base configuration of an n-p-n transistors

(a) In mA In volts in mA SATURATION REGION Cut- Off Region (b) ACTIVE REGION The output characteristics of a typical transistor is shown. The shadow portion of the figure provides much information about the transistor. The entire quadrant is divided into three regions, the active region, the saturation region, and the cut-off region. Each point in the quadrant is called an operating point or Q-point of the transistor.

Emitter current Collector current Base current B E C The collector current is the sum of the emitter current and the base current.

+Vcc The characteristic of a transistor is such that a small voltage change in the base-emitter junction will produce large current change in the collector and emitter, whereas small changes in the collector-emitter voltage have little effect on the base. A typical transistorized amplifying circuit is given. C B n-p-n E + _ Output + _ input Common-emitter configuration Ground - Biasing voltage (source) - Collector to Emitter voltage - Base to Emitter voltage - Resistance at input circuit - Biasing resistances - Load resistance - Feedback resistance - Blocking capacitor (it block dc component) - Coupling capacitor (to next stage) -Feedback capacitor

Drain (D) Source (S) (Gate (G) _ + n-type P-type n-channel Depletion layer Junction Field Effect Transistor (JFET) or simply FET are of two types, p-channel FET and n-channel FET. In each case, a semiconductor bar called channel of one type of semiconductor material is located inside a bulk of material of the other kind. Bipolar junction transistors have low input impedance small high-frequency gain, and are to some extend non-linear. However, high input impedance is desirable for low power consumption. FET overcomes this problem.

p n Base-1 Base-2 Emitter + - (a) Ground E (b) A Equivalent circuit UJT Symbol (c) (d) Characteristics Emitter current Equivalent diode Cathode Anode A typical construction of a transistor defines itself as a unijunction transistor (UJT), a transistor with only one junction and three terminals. UJT exhibits a negative resistance characteristic as can be seen from the V-I plot This switching feature can be exploited in designing oscillators.

p n Anode Cathode Gate + - SCR Symbol Ground (a) (b) (c) Characteristics SCR current Gate voltage Forward breakover voltage Forward conduction Reverse breakdown voltage J1 J2 J3 SCR stands for Silicon Controlled Rectifier. SCRs are four-layered diodes and shows negative resistance characteristics. It has three junctions and three terminals. The application of a forward voltage is not enough for conduction since the junction is reverse biased. A gate signal can control the conduction of the rectifier.

+ _ Inverting terminal Noninverting terminal Positive supply Negative supply Output Input signal can either be connecter to inverting or noninverting terminal Operational Amplifiers (OPAMP) are analog ICs and are basically amplifiers, but can be configured in a variety of ways in order to design low- and high-pass filters, differential amplifiers, oscillators, impedance matching circuits (unit follower), sample and hold (S/H) circuits, current limiters, rectifiers, instrumentation amplifiers, comparators, zero crossing detectors, and so on.

- + Open-loop (Closed-loop) (a) (b) The gain of the OPAMP is defined as the ratio of output voltage to the input voltage. Two different types of gains are encountered in the OPAMP: open-loop gain and closed loop gain. Open-loop gains again are of two types, open-loop differential mode gain and open-loop common mode gain