resistance is proportional to the length and inversely proportional to the cross sectional area of...
TRANSCRIPT
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.
X X
R
A
lR
Symbol of a resistor
m
1R 4R3R2R
X
Y
1R3R
4R2R
(a)(b)
X
Y
Resistances connected in series and parallel are calculated using the following formula.
Series connection Parallel connection
nserieseq RRRRR ................321_
nparalleleq RRRRR
1...................
1111
321_
L
X Y
i
NkL
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.
l
N turns
A
l
N turns
A
Symbol
Surface-1
Surface-2
Electrode-1
Electrode-2
Dielectric material
C
X
Y
dC r
0
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
Inductance
Inductive reactance
Frequency
Inductive reactance
(a)
Capacitance Frequency
Capacitive reactance 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 Terminal
Terminal Terminal
Terminal Terminal
_
_
Flow of current
Flow of electrons
Flow of current
Flow of holes
A
A
A
B
B
B
Flow of current
Flow of electrons
_
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
p-type n-type +
+
+
-
-
-
Majority carriers (holes)
_
_
__
_ _
_
_
_
_
_
Majority carriers (electrons)
Depletion layer
Uncovered immobile atomsUncovered immobile atoms
Potential barrier
Electrode Electrode
n-typep-type
(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
+ -
Voltage source
Reverse-biased p-n junction diode
(a) (b)
Voltage in volts
Current is mA
TV
Current is mA
Voltage in volts
0IbV
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.
)1(0 kT
qV
eII
I is the diode current, q is charge of the carriers, k is a constant, V is the applied voltageT is temp. in degrees K
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.
input Output +
-
+
-
Diode
Common terminal called GROUND
(Common to both input and Output)
Amplitude
Time
Amplitude
Time
Amplitude
Time
Amplitude
Time
(b)
(a)
(c)
(d)(a)
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.
P N P N P N
Collector (C) Collector (C)Emitter (E) Emitter (E)
Base (B)Base (B)
B
C
E
input
Output
Common-collector configuration
B
E C
OutputInput
Common-base configuration
n-p-n
n-p-n
B
C
Einput
Output
Common-emitter configuration
n-p-n
(a) (b)
(f)
C
Bn-p-n (Symbol)
E
(c)
C
B
E
p-n-p (Symbol)
(d)
(e) (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) A pnp transistor(b) An npn transistor
(c) Symbol of a pnp(d) Symbol of npn
CEV
123 BBB III
3BI
2BI
1BI
(a)
In mA
In volts
in mA
in mA
in mA
CI
SAT
UR
AT
ION
RE
GIO
N
Cut- Off Region
CEV(b)
In mA
In volts
CI
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
BE C
EJ CJ
%2
%100
%98
The collector current is the sum of the emitter current and the base current.
BEC III
B
C
E
input
Output
Common-emitter configuration
n-p-n
+Vcc
Ground
+
_
+
_BEV
CEV
1R
2R
LR
ER
cC
EC
bCiR
ccV iR- Biasing voltage (source)
CEV - Collector to Emitter voltage
BEV - Base to Emitter voltage
- Resistance at input circuit
- Biasing resistances
- Load resistance
1R 2R
LR
ER - Feedback resistance bC- Blocking capacitor (it block dc component)
cC - Coupling capacitor (to next stage)EC -Feedback capacitor
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.
DI
DI
DSV
Drain (D)
Source (S)
(Gate (G)
GSV_
+
_
+
n-type
P-t
ype
n-channel
P-type
Depletion layerD
eple
tion
la
yer
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.
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.
p
n
Base-1
Base-2
Emitter+
-
+
-
(a) Ground
1EBV12BB
V
2B
1B
E
(b)
1R
2R
AA
Equivalent circuit
pV
+
-
1B
2B2B
1B
UJT Symbol
(c)
E
(d)
Characteristics
Emitter current
1EBV
pV
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
p
n
Anode
Cathode
Gate
+
- DV
GV
SCR Symbol
+
-
Anode
Cathode
Ground
Gate
(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.
DV 2J
+
_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.
-
+inV+
-
oV+
-
-
+inV+
-
oV+
-
1R
fR
1R
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