PHYSICS INVESTIGATORY PROJECT
AIM:-
CHARGING AND DISCHARGING OF CAPACITORS IN R-C CIRCUIT
PURPOSE
THE GOAL OF THIS PROJECT IS TO verify that 63% charge is stored in a capacitor in an R-C circuit at its time constant and 63% charge remains when capacitor is discharged and hence plot a graph between voltage and time
PHYSICS INVESTIGATORY PROJECT
AIM:-
CHARGING AND DISCHARGING OF CAPACITORS IN R-C CIRCUIT
PURPOSE
THE GOAL OF THIS PROJECT IS TO verify that 63% charge is stored in a capacitor in an R-C circuit at its time constant and 63% charge remains when capacitor is discharged and hence plot a graph between voltage and time
Physics investigatory project for class 12 on the topic " to estimate charge induced on two styro foam / pith balls separated by a distance "
Just change the name and cover page.
Physics investigatory project for class 12 on the topic " to estimate charge induced on two styro foam / pith balls separated by a distance "
Just change the name and cover page.
To study various factors on which the internal resistance/EMF dependsaslipranay
This project for helping student to have an idea to make their own project and score a good marks in their boards practical and making us proud.
Have a superb boards practical.
Thank you
Pranay Raj
#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std;
const int N = 40;
void sum(int*p, int n, int d[]){
int i;
*p = 0;
for(i = 0; i < n; ++i)
{
*p = *p + d[i];
}
}
int main(void){
int i;
int accum = 0;
int data[N];
for(i = 0; i < N; ++i)
{
data[i] = i;
}
sum(&accum, N, data);
cout<<"sum is " << accum << endl;
return 0;
}#include <iostream>
using namespace std
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This presentation provides a briefing on how to upload submissions and documents in Google Classroom. It was prepared as part of an orientation for new Sainik School in-service teacher trainees. As a training officer, my goal is to ensure that you are comfortable and proficient with this essential tool for managing assignments and fostering student engagement.
2. Index
S.No. Heading
1. Certification
2. Acknowledgement
3. Aim
4. Introduction
5. Apparatus
6. Theory
7. Procedure
8. Observations
9. Result
10. Inference
11. Precaution
12. Sources of error
13. Conclusion
14. Bibliography
3. Certification
This is to certify that Ojaswi Mishra, a
student of class XII-B, has completed
research successfully on the project title
“Factors on which internal resistance of
cell depends” under the guidance of ,
Mr. R.G. Goswami (subject teacher)
during the year 2020-21 in partial
fulfillment of chemistry practical
examination conducted by AISSCE, New
Delhi.
Signature of examiner
Signature of Signature of
chemistry teacher Principal
4. Acknowledgement
I would like to take this opportunity
to thank my teacher, Mr. R.G.
Goswami whose support, guidance
and encouragement have enable me
to complete this project.
6. Introduction
There is a great need of batteries in our daily use
electronic appliances and the use is increasing
every day. Thus, the batteries need to be made
more powerful so that their potential can be
increased greatly. This project report is based on
practical analysis for the factors affecting the
internal resistance of a cell.
When the internal resistance of the cell is decreased
we can increase the potential difference across it, and
hence make it more reliable.
Internal Resistance
The resistance within a battery, or other
voltage source, that causes a drop in the
source voltage when there is a current.
7. Internal resistance is defined as the
resistance offered by the electrolyte of the
cell to the flow of ions.
Its S.I. unit is Ohm (Ω).
For a cell of e.m.f. (E) and internal resistance (r),
connected to an external resistance (R) such that (I)
is the current flowing through the circuit,
E = V + Ir
Internal resistance, r = E – V
I
8.
9. Apparatus
A potentiometer, a battery (or battery eliminator),
two one way keys, a rheostat, a galvanometer, a
resistance box, an ammeter, a cell (Leclanche cell),
a jockey, a setsquare, connecting wires and sand
paper.
10. Theory
The internal resistance of a cell is the resistance
offered by its electrolyte to the flow of ions. The
internal resistance of a cell
Is directly proportional to the distance between the
electrodes. Let x be the distance between the
electrodes, then,
r ∝ x
Is inversely proportional to facing surface area of
the electrodes in electrolyte. Let A be the surface
area of the electrodes, then,
r ∝ 1/A
Decreases with increase in temperature of
electrolyte.
Is inversely proportional to concentration of
electrolyte.
The internal resistance of a cell is given by:
r = E – V
I
11. Circuit diagram
The above circuit includes:
A power supply
Two one way keys
A galvanometer
A Resistance Box
A Leclanche cell
A shunt resistance
12. Procedure
Clean the ends of the connecting wires with sand paper
and make tight connections according to the circuit
diagram.
Tighten the plugs of the resistance box.
Check the e.m.f. of the battery and of the cell and make
sure that e.m.f. of the battery is more than that of the cell,
otherwise null or balance point will not be obtained.
To study variation of internal resistance with distance of
Separation
Keep both the electrodes at a distance of 16 cm.
Take maximum current from the battery,
making rheostat resistance small.
Without inserting a plug in key K2, adjust the rheostat so
that a null point is obtained on the last wire of the
potentiometer.
Determine the position of the null point accurately
using a set square and measure the balancing length
(l1) between the null point and the end P.
Next introduce plugs in both keys K1 and K2. At the same
time, take out a small resistance (1 – 5W)
13. from the shunt resistance box connected in
parallel with the cell.
Slide the jockey along a potentiometer wire and
obtain the null point.
Measure the balancing length (l2) from end P.
Record these observations.
Now keep the electrodes 12 cm apart.
Then remove the plugs of keys K1 and K2. Wait
for some time and repeat steps 7 to 10.
Next, keep the electrodes 9 cm apart to obtain
another set of observations.
To study variation of internal resistance with area
of electrodes
Keeping all other factors constant, increase the
area of electrodes in the electrolyte by dipping
them into the electrolyte at different depths for
each observation.
Obtain three such observations by repeating
steps 7 to 10. Record your readings.
14. To study variation of internal resistance with
concentration of electrolyte.
Keeping all other factors constant, decrease the
concentration of electrolyte by adding distilled water for
different observations.
Obtain three such observations by repeating step 7 to
10. Record your readings.
15.
16. Observations
S.No. Ammeter
reading
Position of null
point
(cm)
Shunt
Resistance
(R)
Internal
Resistance
(r)
With R
(l1)
Without
R (l2)
1. 0.3 660.5 35.5 1 0.94
2. 0.3 660.5 77.2 2 1.77
3. 0.3 660.5 108.3 3 2.51
Table for effect of separation between electrodes:
S.No Separation
between
l1(cm) and
d(cm)
Balancing
point
l2(cm)
Balancing
point
r(Ω)
Internal
Resistance
(r)
r
d
electrodes
1. 1.2 326.6 276.9 0.456 0.38
2. 2.5 320.7 219.1 0.45 0.38
3. 3.7 660.5 350.9 1.406 0.38
19. Inference
The internal resistance of a cell is directly
proportional to the separation between the
electrodes.
r ∝ d
The internal resistance of a cell is inversely
proportional to the area of the electrodes
dipped in electrolyte.
r ∝ 1
A
The internal resistance of a cell is inversely
proportional to the temperature of electrolytes.
r ∝ 1
T
The internal resistance of a cell is inversely
proportional to the concentration of the
electrolyte.
r ∝ 1
C
20.
21. Precaution
The connections should be neat, clean
and tight.
The plugs should be introduced in the
keys only when the observations are to
be taken.
The positive polls of the battery E and
cells E1 and E2 should all be connected
to the terminal at the zero of the wires.
The jockey key should not be rubbed
along the wire. It should touch the wire
gently.
The ammeter reading should remain
constant for a particular set of
observation. If necessary, adjust the
rheostat for this purpose.
22. Sources of error
The auxiliary battery may not be
fully charged.
The potentiometer wire may not be
of uniform cross-section and
material density throughout its
length.
End resistances may not be zero.
