Physics expriment
Physics lab
Experiment1
aimrify Ohm`s law and calculate the value of resistance
using V-I curve.
Materials Required
resistor , voltmeter, ammeter, battery,
rheostat,connecting wires and key
THEORY: - Ohm's Law deals with the relationship between voltage and
current in an ideal conductor.
This relationship states
that:
The potential difference
(voltage) across an ideal conductor is proportional to the current through it.
The
constant of proportionality
is called the "resistance", R. Ohm's Law is given by:
V = I R
Where V is the potential
difference between two points which include a resistance R. I is the current
flowing through the
resistance.
Or
Ohm’s law states that the
current through a conductor between two points is directly proportional to the
voltage
across the two points, and
inversely proportional to the resistance between them. V, I, and R, the
parameters of Ohm's law.
I = V / R
Ohm's law is among the most
fundamental relationships in electrical engineering. It relates the current,
voltage, and resistance for a
circuit element so that if we know two of the three quantities we can
determine the third. Thus, if
we measure the current flowing in a resistor of known value, we can deduce
the voltage across the
resistance according to V = IR. Similarly, if we measure the voltage across a
resistor and the current
through it, we calculate the resistance of the element to be R = V/I. Not only
does
this reduce the number of
measurements that must be made, it also provides a way to check the results
of several different
measurement methods.
Observations
VIcharacteristics |
Of ohm's law |
||
Resistor Used |
1KΩ |
||
Readings
Obtained |
|||
Voltage (V) |
Current (mA) |
||
0 |
0 |
||
1 |
1 |
||
2 |
2 |
||
3 |
3 |
||
4 |
4 |
||
5 |
5 |
||
6 |
6 |
||
7 |
7 |
||
8 |
8 |
||
9 |
9 |
||
10 |
10 |
||
11 |
11 |
||
12 |
12 |
|
PROCEDURE
Note : Connection of battery
are important as per polarity.
1. Connect 6V battery/ DC
power supply (external) across red & black
terminals as shown in the
printed circuit diagram.
2. Switch ON the piano type
switch provided on the front panel.
3. Vary the resistance of
Potentiometer & note down the corresponding
current & voltage.
Expriment2
Aim: To study V-I characteristics of p-n diode.
(a)
in forward bias (b) in reverse bias
Apparatus
A p-n junction (semi-conductor) diode, a volt battery, a high resistance rheostat,
one volt voltmeter, one 0-100 mA
ammeter, one way key, connecting wires and pieces of sand paper ,Multisim
software, resistors, multimeter, DC power source
THEORY
If a region of n-type semiconductor is in
intimate contact with a region of p-type semiconductor, they
form p-n junction.A PN junction is formed
at the interface between the indium saturated p-region and the n-type
semiconductor. The holes from the p-zone
cross over to n-zone and electrons from n-zone cross over to pzone.This flow
continues- until there are positive and negative layers on both sides of the
junction to stop the
flow.We call it the depletion layer or the
potential barrier. It exists at the junction before any external field is
applied.
FORWARD BIASING : When the positive
terminal of the battery is connected to p-type and negative terminal
to n-type region of a PN junction as shown
in Fig. (1a). The PN Juntion is said to be forward biased. This applied
potential difference
provides the necessary energy for the holes
and electrons to diffuse through the
junction
on barrier. The holes in the p-region are
pushed forward towards the n-region and
electrons from the n-region because of
negative applied potential cross over to
pregion. Hence the diode starts conducting.
As the potential is increased, there is
gradual increase in the current initial but then current shoots up. This
happens because at this applied potential
almost all the majority carriers (i.e. holes and electrons) cross over.
REVERSE BIASING : In this case the
negative terminal of the battery is
connected
to the p-region and positive terminal is
connected to the n-region as shown in
(2a).The holes of p-region move towards the
-ve terminal and electrons towards the
positive terminal of the battery or the
deflection layer becomes thick or we can
say that the junction barriers gets
strengthened. Practically there should be no flow of current but in fact a very
small current flows which is called reverse
current.
This current is due to the thermally
generated electron-hole pairs within both p and n type materials.
As the reverse bias is increased to
sufficient high value, the covalent bonds near the junction break down and
as a result of this large number of
electron holes pairs are liberated.Thus the current rises abruptly as shown
in Fig. (2b). The voltage at which the
current rises abruptly is called breakdown voltage.
PROCEDURE
Forward
Bias Characteristics :
1.
Make all the connections as shown in Connections
Diagram Fig. (1) using patchcords by connecting Series Resistance in circuit.
2.
Keep 3V/ 30 switch at 3V side & 100 A/ 10mA
at 10mA side.
3.
Keep Set Volts 3V/ 30V Switch at 3V DC.
4.
Keep Potentiometer Knob’s (Set Volts) at extreme
left side.
5.
Switch ON the instrument using ON/ OFF Indicator
switch provided on the front panel.
6.
Set the voltage at 0.2V and note down the
corresponding current reading in the Table No. (1b).
7.
Keep on increasing voltage in the steps of 0.2V
& note down corresponding current in the Table No.
(1b).
Reverse
Bias Characteristics :
1.
Make all the connections as shown in Connections
Diagram Fig. (2) using patchcords by connecting Series Resistance in circuit.
2.
Keep 3V/ 30 switch at 30V side & 100 A/ 10mA
at 100 A side.
3.
Keep Set Volts 3V/ 30V Switch at 30V DC.
4.
Keep Potentiometer Knob’s (Set Volts) at extreme
left side.
5.
Switch ON the instrument using ON/ OFF Indicator
switch provided on the front panel.
6.
Set the voltage at 0.2V and note down the
corresponding current reading in the Table No. (2b).
7.
Keep on increasing voltage in the steps of 0.2V
& note down corresponding current in the Table No.
(2b).
Comments
Post a Comment