LAB 1 - D’ARSONVAL GALVANOMETER
UNIVERSITI MALAYSIA PERLIS
NDJ 30003 – ELECTRONIC INSTRUMENTATION
LAB 1
D’ARSONVAL GALVANOMETER
Prepared
by:
Ts. Ahmad
Syahir Bin Ahmad Bakhit
Name : IRFAN BIN RAMZAN
Matrix No. : 192020084
Program : COMPUTER ENGINEERING
Date : 13/9/2021
OBJECTIVES
To find the internal resistance and the current sensitivity of the galvanometer.
INTRODUCTION
The galvanometer contains a coil of wire in a magnetic field, which will experience a torque when a current passes through the wire of the coil. The coil is attached to a pointer and a spring so that the amount of deflection of the pointer is proportional to the current in the wire of the coil.
1. Set the potentiometer to 510Ω. Connect the circuit as in the Figure 1.1 and keep the voltage source in minimum position such that voltage output from the voltage terminals are 0V.
2. Increase
the voltage supply and the galvanometer pointer will deflect towards right hand
side or left hand side. You can replace the galvanometer with the DMM/Ammeter
in the Multisim. Assume Rg is 1.2 Ω for the given galvanometer. Vary
the voltage supply until the galvanometer shows its maximum deflection, which
the pointer should comes to 30 positions (divisions).
3. Connect
the multimeter across the voltage terminal to measure the voltage and record
this value as VFS.
4. Turn
OFF the supply and do not disturb the voltage source. Now connect the resistance, RS and
construct the circuit as in Figure 1.2.
Select the 10 Ω for RS. Switch ON the instrument, then the
pointer of the galvanometer will return back by a few divisions.
Figure 1.2: The circuit diagram with shunt resistor, RS
5. Without
disturbing the voltage source, adjust the potentiometer, R2 until
the pointer scale comes to full scale deflection which is 30 positions
(divisions).
6. Turn
OFF the supply and disconnect R2. Measure the absolute values of R2
using multimeter and record the value in the Table 2.1.
7. The values of VFS, R1, R2, RS, are known, determine the galvanometer resistance, Rg by calculation. Then calculate its current sensitivity, K. Repeat from step 5 for RS = 5 Ω and 2 Ω and R1 = 220 Ω.
8. Finally
disconnect the galvanometer from the circuit and connect multimeter across the
terminal of galvanometer to measure its internal resistance. Record the value as Rg (measured).
.
RESULTS
N |
R1 (Ω) |
VFS (V) |
Rs (Ω) |
R2 (Ω) |
|
Rg Ω |
|
Mean
of Rg |
K (A/div) |
Mean
of K |
Meas. |
Calc. |
%e |
||||||||
30 |
510 |
15.34 |
10 |
450 |
1.2 |
1.33 |
10.83 |
1.39 |
0.53m |
0.55m |
5 |
410 |
1.23 |
2.50 |
0.55m |
||||||
2 |
300 |
1.40 |
16.67 |
0.59m |
||||||
220 |
6.64 |
10 |
190 |
1.58 |
31.67 |
0.52m |
||||
5 |
170 |
1.47 |
22.50 |
0.54m |
||||||
2 |
130 |
1.39 |
15.00 |
0.59m |
RL = 100kΩ
2)
1MΩ
10MΩ
100MΩ
Conclusion:
Throughout these lab activities, based
on the tabulated data obtained from the experiment, it is safe to concluded
that D’Arsonval Galvanometer (replaced with voltmeter particularly in this
experiment) are sensitive to the change of resistance in the circuit adjusted
by potentiometer.
As the Rs value drop, we can see how
the current also drop in response. This strongly support the basic rules of
voltage, resistance and current which V=I/R. As the voltage value are to be
remain constant, only the current value would change in response to the changes
of resistance value.
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