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Lab 4 - Electrostatic Potential and Electric Fields | PHYS 132, Lab Reports of Physics

Material Type: Lab; Class: Electromagnetism and Optics-GTSC1; Subject: Physics; University: Mesa State College; Term: Spring 2008;

Typology: Lab Reports

Pre 2010

Uploaded on 08/18/2009

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Phys 132L
Spring 2008
Laboratory 4: Electrostatic Potential and Electric Fields
In one dimension, the electric field and the electrostatic potential are related via
either
V(x1)V(x2) = Zx2
x1
Edx(1)
or
E=
dV
dx .(2)
There are analogous relationships for three dimensional cases. Of the two quantities
the electrostatic potential is far easier to measure and the entire electrostatic potential
landscape can be mapped using a voltmeter. Once the landscape is mapped Eq. (2)
can be invoked to determine the electric field. An important additional rule, inferred
from Eq. (2), is that the electric field points opposite to the gradient of the electrostatic
potential and that these gradients are perpendicular to equipotential lines, i.e. lines along
which the electrostatic potential is constant. The aim of this laboratory is to investigate
these relationships and to exploit them to determine the electric fields produced by
various arrangements of charge distributions.
1 Electrostatic Potentials and Electric Fields: Parallel Conductors
In this part of the experiment you will investigate the electrostatic potentials and
the electric fields produced by parallel conductors. Each conductor, or electrode, will be
connected to one terminal of the output of a power supply.
a) The electrodes will eventually be drawn onto a sheet of conductive paper (black
paper with a grid) using an ink pen that contains silver ink particles suspended in
a solvent. Using a light colored pencil trace, on a conductive sheet, two parallel
lines extending along the length of the sheet and separated by 6cm.The electrodes
will be drawn on top of these lines.
b) When used properly the conductive (silver) ink pen can produce highly conductive
lines. Vigorously shake the conductive ink pen (with the cap on) for 10-20 seconds
to disperse any particle matter suspended in the ink. You should be able to hear
something moving inside the pen while you do this.
c) Drawing with the pen requires simultaneously depressing the tip of the pen and
squeezing the barrel of the pen. Practice doing this on a piece of scrap paper until
you can produce a continuous silver line of approximately uniform width.
d) Draw the electrodes on the conductive paper, following the lines that you traced
earlier. It is essential that the electrodes are continuous; any break will disrupt the
conductivity.
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Phys 132L Spring 2008

Laboratory 4: Electrostatic Potential and Electric Fields

In one dimension, the electric field and the electrostatic potential are related via either

V (x 1 ) − V (x 2 ) = −

∫ (^) x 2

x 1

Edx (1)

or

E = − dV dx

There are analogous relationships for three dimensional cases. Of the two quantities the electrostatic potential is far easier to measure and the entire electrostatic potential landscape can be mapped using a voltmeter. Once the landscape is mapped Eq. (2) can be invoked to determine the electric field. An important additional rule, inferred from Eq. (2), is that the electric field points opposite to the gradient of the electrostatic potential and that these gradients are perpendicular to equipotential lines, i.e. lines along which the electrostatic potential is constant. The aim of this laboratory is to investigate these relationships and to exploit them to determine the electric fields produced by various arrangements of charge distributions.

1 Electrostatic Potentials and Electric Fields: Parallel Conductors In this part of the experiment you will investigate the electrostatic potentials and the electric fields produced by parallel conductors. Each conductor, or electrode, will be connected to one terminal of the output of a power supply.

a) The electrodes will eventually be drawn onto a sheet of conductive paper (black paper with a grid) using an ink pen that contains silver ink particles suspended in a solvent. Using a light colored pencil trace, on a conductive sheet, two parallel lines extending along the length of the sheet and separated by 6 cm. The electrodes will be drawn on top of these lines. b) When used properly the conductive (silver) ink pen can produce highly conductive lines. Vigorously shake the conductive ink pen (with the cap on) for 10-20 seconds to disperse any particle matter suspended in the ink. You should be able to hear something moving inside the pen while you do this. c) Drawing with the pen requires simultaneously depressing the tip of the pen and squeezing the barrel of the pen. Practice doing this on a piece of scrap paper until you can produce a continuous silver line of approximately uniform width. d) Draw the electrodes on the conductive paper, following the lines that you traced earlier. It is essential that the electrodes are continuous; any break will disrupt the conductivity.

e) Configure the power supply so that it provides a DC voltage between 5.0 V to 15 V. Connect one terminal of the output to one electrode and the other to the other electrode. f) Use the voltmeter to measure the electrostatic potential difference between two widely separated points on the same silver electrode. Repeat this for the other electrode. g) Measure the electrostatic potential difference between two points, one on each of the electrodes. Try this at a few different locations. Note the extent to which this varies.

In the following parts you will measure electrostatic potentials relative to that of the negative electrode, which is that at the lower potential. Throughout these part, you will hold the “COM” voltmeter probe on the negative electrode while varying the position of the other probe in the gap between the negative and positive electrode, which is that at the higher potential.

h) Place the other voltmeter probe on the positive electrode and slowly drag it across the gap between the two electrodes. Comment on the behavior of the electrostatic potential as you do this. Does it change continuously or jump? Does it increase, decrease or fluctuate up and down as you cross the gap? i) Map at least 10 points on any single equipotential line in the gap between the two electrodes. Draw the equipotential curve that passes through these points and label the value of the electrostatic potential on this curve. Repeat this for five approximately equally spaced equipotential lines. Comment on the shape of these curves. j) The gradient of electrostatic potential is the direction in which the electrostatic potential increases most rapidly and is parallel to the electric field. To measure the gradient tape the two probes together so that their heads are not touching and remain fixed close distance apart. With this configuration, place the pair of probes at several locations along one equipotential line and determine the direction of the gradient of electrostatic potential. Indicate this with arrows on the sheet. k) Measure the electrostatic potential difference (from the negative electrode) at about eight to ten equally spaced points along a line perpendicular to the electrodes. Record electrostatic potential differences and the distances from each point to the negative electrode. Plot the electrostatic potential difference vs. distance from the negative electrode. What type of graph is this? What does the shape of this graph imply for the magnitude of the electric field between the electrodes? Determine the magnitude of the electric field between the electrodes.

2 Electrostatic Potentials and Electric Fields: Circular Conductors The same approach can be applied to any arrangement of conductors. In this part of the experiment you will investigate the fields and potentials produced by conductors arranged as illustrated.