Physics Laboratory 5

Electric potentials and fields

In this laboratory you will explore the connection between electric field lines and equipotential surfaces.  Objects with net electric charge attract or repel each other.  If you want to change the position of a charged object relative other charged objects, you, in general, have to do (positive or negative) work.  But sometimes it is possible to move a charged object relative to other charged objects along a surface without doing any work.  The potential energy of the charged object does not change as you move it.  If an electric charge can travel along a surface without the electric field doing any positive or negative work, then the surface is called an equipotential surface.

Open a Microsoft Word document to keep a log of your experimental procedures and results.  Complete all the tasks (in blue).  Answer all questions.


Activity 1

The concept of work

image(a)  The work W done on an object by a constant force is defined as W = Fd.  It is equal to the magnitude of the force, multiplied by the distance the object moves in the direction of the force.
The SI unit of work is Nm = J.
An object travels from point A to point B while two constant forces of equal magnitude are exerted on it, as shown in the figure on the right. 

image(b)  An object travels from point A to point B while two constant forces of unequal magnitude are exerted on it, as shown in the figure on the right. 

Work and the electric field

imageIn the diagram on the right, the red dot denotes a positive point charge.  Points W, X, Y, and Z and the point charge lie in the same plane.  Points W and Y are equidistant from the charge, as are points X and Z.
Draw the electric field vectors at points W, X, Y, and Z.
(c)  A particle with charge +qe travels along a straight line from point W to point X.

       image

(d)  A particle travels from point X to point Z along the circular arc shown.

       image

Electric potential difference

A potential energy function is a function of the position of an object.  It can only be defined for conservative forces.  A force is conservative if the work it does on an object depends only on the initial and final position of the object and not on the path. 
(e)  Suppose the moving charge in part (c) increases from +qe to +1.8 qe.

(f)  The electric potential difference  ∆VWX between two points W and X is defined to be the negative of the work done by the electric field on a charge q, divided by q, as q travels from W to X.

When a net force does work on an object, its kinetic energy changes.
Wnet = ½m(vf2 - vi2) = ∆K.
(g)  A particle of charge |qe| = 3*10-6 C and mass m = 3*10-8 kg is released from rest at point W.  The speed of the particle is measured to be 30 m/s as it passes point X. 

image

(h) Assume you have a test charge at rest at a distance of 2 cm from the charge on the right.  You want to move it.

What path could you choose, so you would not have to do any work?   What is the shape of the equipotential surface?   (Remember that in general you can move in three dimensions.)  Explain your reasoning.

image(i)  Find some equipotential surfaces for the charge configuration shown on the right, which consists of two charged metal plates placed parallel to each other.

What is the shape of the equipotential surfaces?  Remember you are trying to decide how a test charge could move so that the electric field does no work on it.  Sketch your predictions and explain your reasoning.

image(j)  Find some equipotential surfaces for the electric dipole charge configuration shown on the right.

Sketch your predictions and explain your reasoning.

(k)  Review these 3-dimensionl representations of equipotential surfaces and field lines.

Choose several different configurations.

Do these 3D representations help you visualize the relationship between electric field lines and equipotential surfaces?


Activity 2

Review these 3-dimensionl representations of equipotential sufaces and field lines.

(a)  Equipotential surfaces of a charged sphere

(b)  Field lines and equipotential surfaces

Now use a spreadsheet to calculate the electric potential at grid points in the in the x-y plane due to 1, 2, 3, or 4 small, uniformly-charged spheres.  The x-y plane is divided into a 25 x 25 grid.  The upper left corner of the grid corresponds to x = 0.5 m, y = 0.5 m, and the lower right corner corresponds to x = 24.5 m, y = 24.5 m.  The charged spheres can be placed anywhere on the grid.  They will be located in the x-y plane.  The spreadsheet calculates the potential at each grid point and produces a surface and a contour plot of the potential.

The potential at r = (x,y,z) outside a uniformly charged sphere centered at r' = (x',y',z') is
V(r) = kq/|r - r'| = kq/((x - x')2 + (y - y')2 + (z - z')2)1/2.

In the x-y plane we have z = 0 and
V(x,y) = kq/((x - x')2 + (y - y')2)1/2.

The constant k has a value of 9*109 in SI units.  If we measure q in units of nC = 10-9C, then kq = 9*q Nm2/C

Download this Microsoft Excel spreadsheet.

Examine the spreadsheet
Cells B1 -Z1 contain the x-coordinates and cells A2 - A26 the y-coordinates of the grid points
Cells A31 - C34 contain the x- and y-coordinates (in units of m) of the positions and the magnitudes (in units of nC) of four charges.
The spreadsheet initializes with a +10 nC charge at x = 13 m, y = 13 m and all the other charges have zero magnitude. 
(When you add more charges, let the x- and y-coordinates always be integers.  This avoids "divide by zero" errors, since the grid points have half integer x- and y-coordinates.)

tsble

Cell B2 contains the formula

=9*$C$31/SQRT((B$1-$A$31)^2+($A2-$B$31)^2)
+9*$C$32/SQRT((B$1-$A$32)^2+($A2-$B$32)^2)
+9*$C$33/SQRT((B$1-$A$33)^2+($A2-$B$33)^2)
+9*$C$34/SQRT((B$1-$A$34)^2+($A2-$B$34)^2)

This is the sum of V(x,y) = kq/((x - x')2 + (y - y')2)1/2 due to the four charges.
Cell B2 is copied into the other cells of the grid. The grid consists of cells B2 - Z26.
The spreadsheet shows two plots of the potential at the grid points. The contour lines are equipotential lines.  They are spaced in 5V intervals.

(a) Start with just the one +10 nC charge at x = 13 m, y = 13 m.

Describe the graphs.  What do they tell you about the potential outside a uniformly charged sphere?   Can you get information about the electric field outside a uniformly charged sphere from these graphs, i.e. can you draw field lines?  Estimate the magnitude and direction of the electric field in units of V/m = N/C at x = 20 m, y = 13 m.

(b)  Now change the positions and magnitudes of your charges.  Use the numbers below.

x y q
5    13    10   
20 13 10
0 0 0
0 0 0

Just type in the new numbers into the cells A31 - C34 and the spreadsheet and the graphs will update automatically.

Paste the upper graph into your word document.  Describe both graphs.  What do they tell you about the potential of this charge distribution?

(c)  Again change the positions and magnitudes of your charges.  Use the numbers below.

x y q
5    13    10   
20 13 -10
0 0 0
0 0 0

Paste the upper graph into your word document.  Describe both graphs.  What do they tell you about the potential of this charge distribution?

(d)  Again change the positions and magnitudes of your charges.  Use the numbers below.

x y q
10    10    5  
20 10 -10
10 20 -10
20 20 5

Paste the upper graph into your word document.  Describe both graphs.  What do they tell you about the potential of this charge distribution?


Convert your log into a lab report.  See the grading scheme for all lab reports.

Name:
E-mail address:

Laboratory 5 Report

Save your Word document (your name_lab5.docx), go to Canvas, Assignments, Lab 5, and submit your document.