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Coulomb’s Law Lab Manual, Lab Reports of Physics

To determine electrostatic force between two charged conducting spheres depends on the distance between the spheres and depends on the charge on the spheres.

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2020/2021

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Brooklyn College 1
Coulomb’s Law
Purpose
a. To determine how the electrostatic force between two charged conducting spheres
depends on the distance between the spheres and
b. To determine how the electrostatic force between two charged conducting spheres
depends on the charge on the spheres.
Theory
Electrostatic force between two charges is (a) directly proportional to the magnitude of the
product the two charges and (b) inversely proportional to the square of the distance between their
centers.
If Q1 and Q2 are the magnitude of the two point charges, and R is the distance between their
centers, electrostatic force between them is expressed by the equation below.
𝐹 = 𝑘 |𝑄1||𝑄2|
𝑅2 (1)
where k is a constant of proportionality, called Coulomb’s constant, k = 8.99 x 109 N.m2/C2. In this
experiment, you are going to verify the Coulomb’s law by using a Coulomb balance.
Apparatus
High Voltage Power Source (0- 6 kV), PASCO Coulomb Balance
Description of Apparatus
You will be using a Pasco Coulomb balance in this lab which is shown in Fig. 1. The
Coulomb Balance is a delicate and very sensitive torsion balance that can be used to investigate the
nature of the electrostatic force between charged
objects. You will use two identical conductive
spheres in this experiment. One conductive
sphere is mounted on a rod which is counter-
balanced and suspended on a thin torsion wire.
An identical conductive sphere is mounted on a
slide assembly so that it can be positioned at
various distances from the suspended sphere.
The spheres are held by plastic support rods for
electrical insulation. The ruler on the slide
assembly measures the distance between the
centers of the two spheres when the suspended
sphere is at its equilibrium position. When the
conducting spheres are charged, the sphere
suspended on torsion wire gets deflected due to
electrostatic force. Rotating knob is used to
bring the charged sphere back to equilibrium
position.
Charged spheres
Torsion wire
Sliding assembly
Rotating Knob
Fig. 1. PASCO Coulomb balance
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Coulomb’s Law

Purpose

a. To determine how the electrostatic force between two charged conducting spheres depends on the distance between the spheres and b. To determine how the electrostatic force between two charged conducting spheres depends on the charge on the spheres.

Theory

Electrostatic force between two charges is (a) directly proportional to the magnitude of the product the two charges and (b) inversely proportional to the square of the distance between their centers.

If Q 1 and Q 2 are the magnitude of the two point charges, and R is the distance between their centers, electrostatic force between them is expressed by the equation below.

|𝑄 1 ||𝑄 2 | 𝑅^2

where k is a constant of proportionality, called Coulomb’s constant, k = 8.99 x 10^9 N.m^2 /C^2. In this experiment, you are going to verify the Coulomb’s law by using a Coulomb balance.

Apparatus

High Voltage Power Source (0- 6 kV), PASCO Coulomb Balance

Description of Apparatus

You will be using a Pasco Coulomb balance in this lab which is shown in Fig. 1. The Coulomb Balance is a delicate and very sensitive torsion balance that can be used to investigate the nature of the electrostatic force between charged objects. You will use two identical conductive spheres in this experiment. One conductive sphere is mounted on a rod which is counter- balanced and suspended on a thin torsion wire. An identical conductive sphere is mounted on a slide assembly so that it can be positioned at various distances from the suspended sphere. The spheres are held by plastic support rods for electrical insulation. The ruler on the slide assembly measures the distance between the centers of the two spheres when the suspended sphere is at its equilibrium position. When the conducting spheres are charged, the sphere suspended on torsion wire gets deflected due to electrostatic force. Rotating knob is used to bring the charged sphere back to equilibrium position.

Charged spheres

Torsion wire

Sliding assembly

Rotating Knob

Fig. 1. PASCO Coulomb balance

Complete experimental set up is shown in Fig. 2. The spheres are charged by means of a very stable high voltage (kilovolt) power supply and a charging probe. The electrostatic force between the spheres causes the torsion wire to twist. The torsion balance can be brought back to its equilibrium position by twisting the torsion wire in the opposite direction using the rotating knob. The angle through which the torsion wire must be twisted to reestablish equilibrium is directly proportional to the electrostatic force between the two spheres.

F  (2)

The proportionally constant depends on the torsional constant of the wire.

By varying the distance between the spheres and the amount of charge on the spheres, it is possible to verify Coulomb's Law. Although it is possible, using this apparatus, to measure the value of the constant, k, appearing in Coulomb's Law, we will not attempt to do so in the present experiment. We will attempt to verify that the value of the exponent of R is 2 and that the force is proportional to the product of the two charges.

Procedure

! CAUTION!

THE APPARATUS IS VERY DELICATE AND MUST BE HANDLED WITH CARE. Please pay close attention to using proper technique. Do not touch the spheres with your hands. Do not disturb the table where the Coulomb balance is sitting. If in doubt about any procedure, ask!

!!Be careful working in this lab since you are using a Kilovolt power supply!!

Fig. 2. Experimental set up

Charging probe (red)

High voltage power supply

Grounding probe (black)

  1. Move the sliding sphere back to maximum separation and repeat step 2, to recharge the spheres. This must be done between measurements to minimize the effects of charge leakage.
  2. Repeat step 3. Do not look at the dial while you are rotating it! Try to obtain honest, independent measurements. Repeat this measurement several times until you have obtained three measurements which agree within two degrees. Use the average of those three measurements as your final result (expressed to the nearest tenth of a degree) and record in table 1.
  3. Repeat steps 1-5 for distances R = 14, 10, 7, 6, and 5 cm. If the zero has shifted, you will have to repeat the previous set of measurements.

Part II. Force versus Charge

In this part of the experiment, you will keep the distance between the spheres constant and measure the force for different values of the charge, keeping Q 1 = Q 2 always.

  1. Keep the separation between the spheres held constant at R = 5 cm,
  2. The charge transferred to a sphere is proportional to the charging voltage. Thus, you can produce different charges on the spheres by adjusting the voltage of the power supply. Use meter settings of 6 (for 6 kV). Always ground both spheres before charging and make sure that they are at maximum separation during charging. Follow the same procedures outlined in part A and record the data in table 2.
  3. Repeat the above step for meter settings 5, 4, 3, 2, and 1. You will obtain six data points by this method.

Computation and Analysis

Because you are using charged spheres rather than point charges to test Coulomb's Law, the effective distance between the charges is not equal to the distances between the centers of the spheres. An approximate expression for the corrected distance ( R’ ), adequate for our purposes, is given by

𝑅′ = 𝑅 (1 + 2.3 𝛽) (3)

with 𝛽 = 𝑎^3 𝑅^3 ^ and^ a^ = 1.90 cm

where R is the distance between the centers of the spheres and a is the radius of each sphere. It is assumed here that the conducting spheres are identical and carry identical charges.

For each value of R used in part I, calculate R' using the above expression. Also tabulate your

data for 1/(R')

2 , ln R' , and ln θ.

  1. Plot a graph of ln θ versus lnR ’ from your data in Table 1. Draw the best straight line from the scattered data point and determine the slope of this line. Estimate the uncertainty in this slope. Question: What does the slope of this line tell you? Hint: If 𝜃 = 𝑏 (𝑅′)−𝑛^ then ln 𝜃 = ln 𝑏 − 𝑛 ln 𝑅′
  2. Plot θ vs 1/R’^2. Draw a best fitting straight line that you can through your data points.

Question: Should this straight line pass through the origin? What can you conclude from this graph?

  1. From the data in Table 2, plot a graph of angle of deflection ( θ ) versus the product of Q 1 and Q 2 , (Q 1 xQ 2 ). Make a best fit-curve to the plotted data. Explain your results in the report.

Questions to be answered in your report

  1. Explain, qualitatively, why the effective distance between the spheres, R' , is always greater than the distance, R , between their centers. A diagram, showing the distribution of charges on each conducting sphere, should be included as part of your explanation.
  2. When the spheres are very far apart, the correction to R is very small, i.e., R' = R. However, as the spheres are brought closer together the correction becomes larger, i.e., (R'- R) / R increases as R decreases. Explain, on physical grounds, why this must be so, referring to your answer to question 1.
  3. Identify as many possible sources of errors in these measurements as you can think of and, in each case, suggest ways in which the error might be reduced experimentally or corrected for in some fashion.