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Lab 3 Electric Field Potential XXXXXXXXXXName _____________________ Lab Goal: To understanding how the Electric Field and Potential area connected Lab 3 uses the PhET simulation Charges and Field....

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Lab 3 Electric Field Potential      XXXXXXXXXXName _____________________
Lab Goal: To understanding how the Electric Field and Potential area connected
Lab 3 uses the PhET simulation Charges and Field. This lab will be a warm up for next week’s lab when we start working with the Electricity Lab Kit. With this simulation you will take a closer look at the Electric Field and examine and get an understanding of the Potential.
XXXXXXXXXXhttps:
phet.colorado.edu/en/simulations/charges-and-fields
Objectives: In this lab, you will
· Verify the formula for the electric field of the point charge
· Explore the electric field lines of various charge configurations and the superposition principle
· Explore the relationship between the electric field and electric potential
As usual, please read through the whole lab and then play with the new equipment: the voltmeter and the measuring tape.
Remember to always reset the simulation window by clicking on the lower left corner.
Part I: Electric field of the point charge
(this may be a review, but it is worth doing this so that you can have a connection to potential)
Procedure:
1) Click on “Grid.” Place one positive charge in the center of the grid. Click on “Electric Field.”
Can the a
ows that the program uses be THE visualization of the electric field lines of the electric field?
If these a
ows are not the electric field lines, draw what they should look like. How are they similar and different from the field lines?
If these a
ows are the field lines, continue with the lab activity. How are they similar and different from the field lines?
2) Click on “Values”. Place electric field sensors (yellow circles) on five various points on the grid. (For convenience, choose points on the intersections of the major grid lines.) Assuming the point charge is placed in the origin of the coordinate system, record the following information in the table below. Note the scale on the grid and make sure to use co
ect units.
    Sensor #
    x
    y
    
    
    
    Electric
Field angle
    1
    
    
    
    
    
    
    2
    
    
    
    
    
    
    3
    
    
    
    
    
    
    4
    
    
    
    
    
    
    5
    
    
    
    
    
    
Note that the information in the columns 2 – 5 pertains to the location of the sensors and the information in the columns 6 – 7 is magnitude and direction of the electric field calculated by the simulator.
Conclusions:
a) Prove that the electric field of the point charge is radial by comparing your values in column 5 (position angle) and in column 7 (electric field angle). Explain.
) Calculate the value of for all five sensors. Add another column to the table above to record your results. Do they show that the magnitude of the electric field of the point charge is inversely proportional to the distance squared? Explain. Use the values you found and the value of the point charge 1nC to find constant k experimentally.
Question: Suppose that you used a negative point charge instead of a positive. Look at the data you recorded in the table – which of the columns would change, and how? Use the simulator to check your answer.
Part II: Electric Field of Multiple Charges
Procedure:
1) Use the charges to create an electric dipole with a horizontal axis by placing a positive and a negative charge (equal in magnitude but opposite in sign) 1 meter away from each other. (Axis of a dipole is a line passing through both charges.) Place positive charge on the left and negative on the right.
2) Describe the field at the following locations, and explain these results using the superposition principle.
· On the horizontal axis to the right of the dipole
· On the horizontal axis between charges
· On the horizontal axis to the left of the charges
· On the vertical line bisecting the line segment connecting the charges, above the dipole
· On the vertical line bisecting the line segment connecting the charges, below the dipole
3) Is there a location where the electric field is exactly zero?
4) Remove the negative charge and replace it with equal in magnitude positive charge. Observe the change in electric field, and again describe the field at the following locations, explaining these results using the superposition principle.
· On the horizontal axis to the right of the charges
· On the horizontal axis between charges
· On the horizontal axis to the left of the charges
· On the vertical line bisecting the line segment connecting the charges, above the charges
· On the vertical line bisecting the line segment connecting the charges, below the charges
5) Is there a location where the electric field is exactly zero?
6) Remove these charges and a
ange exactly four charges – two positive and two negative – on the grid in a way that the electric field in the center of the grid is zero. Insert the screenshot in this document.
7) Use as many charges as you want to create a configuration of charges that results in a uniform electric field in some region of the grid. Insert the screenshot in this document.
Part III: Electric Potential
Procedure:
1) Clear the charges and place one positive charge in the center of the grid, on the intersection of major gridlines. Grab a voltage sensor, and move it around the grid, observing how the values change. Then, do the same for one negative charge in the center of the grid.
2) Create an electric dipole by placing one positive and one negative charge on a horizontal grid line. Measure the electric field and electric potential at the point midway between the charges and at several points on the vertical line bisecting the line segment connecting the charges.
3) Create a charge configuration similar to that of a dipole but use two charges of the same sign instead. Measure the electric field and electric potential at the point midway between the charges and at several point on the vertical line bisecting the line segment connecting the charges.
4) Based on your data, what is the main difference between the superposition principle for the electric fields and electric potential?
PART IV: Relationship between field and potential
1) Place four charges, two positive and two negative, at four random points on a grid. Click on “Values.” Drag the voltage sensor in the vicinity of the charges and click on the pencil icon. A line will appear labeled by a number.
a) Move the sensor in a way such that the intersection of crosshairs remains on the line. Does the number on the sensor change? What is the physical meaning of this line?
) Move the sensor to a different spot and click “plot” again. In this manner, create 8 to 10 lines.
c) Take an electric field sensor and move it on an equipotential line. What can you say about the way magnitude and direction of the electric field changes as the sensor travels around the line?
d) Place a few electric field sensors in a few points between the equipotential lines. Where do the electric field vectors point in terms of increase and decrease of the values on the equipotential lines?
2) Remove the charges and lace a positive charge in the center of the grid. Draw five equipotential circles with the potentials of 10 Volts, 8 Volts, 6 Volts, 4 Volts and 2 Volts. (It might be hard to get the precise values but try to get as close as you can).
Take an electric field sensor and move it in a straight line, crossing the equipotential lines. Describe the relationship between the distance between the equipotential lines and the strength of the electric field.
Conclusions:
Use the observations above and the concept of work to describe and explain
· the relative orientation between the equipotential lines and field lines
· the relationship between the direction of the electric field and increase or decrease in potential
· the relationship between the magnitude of the electric field and the distance between the pairs of lines with the equal potential difference
Part 1 B I G Analysis:
You have explored the effect of the charges and the distances on the FORCE magnitude.
You have collected data on charge magnitude, distances, and forces.
You know that the equation for electric force, Coulomb’s force, is
XXXXXXXXXXy = m x
In this experiment you have values for F, . In effect, the table of values are “measurements you took” of observational parameters. Basically, you observed

Now to calculate K. From alge
a (and our first lab) we learned how to plot data, fit a line to the data and get the slope of the (fitted) line using trendlines.
For this analysis you will make 2 plots and compute K and compare you value with the accepted value for K = 8.99 * 109 Nm2 / C2.
Use Procedure Part B for one plot and then use Procedure Part c for the other plot.
Compare both of these values with the actual value.
x
y
1
tan
-
=
q
|
|
E
2
|
|
E
´
2
2
y
x
+
=
Answered Same Day Sep 24, 2021

Solution

Anil answered on Sep 24 2021
146 Votes
Lab 3 Electric Field Potential      Name _____________________
Lab Goal: To understanding how the Electric Field and Potential area connected
Lab 3 uses the PhET simulation Charges and Field. This lab will be a warm up for next week’s lab when we start working with the Electricity Lab Kit. With this simulation you will take a closer look at the Electric Field and examine and get an understanding of the Potential.
https:
phet.colorado.edu/en/simulations/charges-and-fields
Objectives: In this lab, you will
· Verify the formula for the electric field of the point charge
· Explore the electric field lines of various charge configurations and the superposition principle
· Explore the relationship between the electric field and electric potential
As usual, please read through the whole lab and then play with the new equipment: the voltmeter and the measuring tape.
Remember to always reset the simulation window by clicking on the lower left corner.
Part I: Electric field of the point charge
(this may be a review, but it is worth doing this so that you can have a connection to potential)
Procedure:
1) Click on “Grid.” Place one positive charge in the center of the grid. Click on “Electric Field.”
Can the a
ows that the program uses be THE visualization of the electric field lines of the electric field?
If these a
ows are not the electric field lines, draw what they should look like. How are they similar and different from the field lines?
If these a
ows are the field lines, continue with the lab activity. How are they similar and different from the field lines?
Yes, these a
ows are the visualization of electric field. These a
ows represent the direction of electric field at different points. So, if we join the a
ows pointing in similar direction, we get the electric filed lines. There a
ows are similar to electric field lines. Only difference is that electric filed line are continuous which represent the locus of points at which electric filed is in same direction (magnitude can be different).
2) Click on “Values”. Place electric field sensors (yellow circles) on five various points on the grid. (For convenience, choose points on the intersections of the major grid lines.) Assuming the point charge is placed in the origin of the coordinate system, record the following information in the table below. Note the scale on the grid and make sure to use co
ect units.
    Sensor #
    x
    y
    
    
    
    Electric
Field angle
(deg)
    1
    1
    0
    1
    0
    9.10
    0
    2
    1
    1
     = 1.414
    45
    4.53
    45
    3
    0
    1
    1
    90
    9.10
    90
    4
    -1
    0
    1
    180
    9.10
    180
    5
    0
    -1
    1
    270 (-90)
    9.10
    -90.1
Note that the information in the columns 2 – 5 pertains to the location of the sensors and the information in the columns 6 – 7 is magnitude and direction of the electric field calculated by the simulator.
Conclusions:
a) Prove that the electric field of the point charge is radial by comparing your values in column 5 (position angle) and in column 7 (electric field angle). Explain.
From the table, we can see that position vector r (assuming positive charge position as center) at each different points making same angle with positive x-axis (given in column 5) as the angle of electric field (in column 7) at that point. So, from this we can say that direction of position vector and electric field are same. Hence electric field off point charge is radial.
) Calculate the value of for all five sensors. Add another column to the table above to record your results. Do they show that the magnitude of the electric field of the point charge is inversely proportional to the distance squared? Explain. Use the values you found and the value of the point charge 1nC to find constant k experimentally.
    Sensor #
    x
    y
    
    
    
    Electric
Field angle
(deg)
    
    1
    0.5
    0
    0.5
    0
    36.4
    0
    9.1
    2
    1
    0
    1
    0
    9.10
    0
    9.10
    3
    1.5
    0
    1.5
    0
    4.02
    0
    9.045
    4
    1
    1
     = 1.414
    45
    4.53
    45
    9.06
    5
    1
    0.5
    1.118
    26.56
    7.35
    26.7
    9.187
From column 8, we can see that all values are approximately same. That means is constant and does not change with r.
So electric filed is inversely proportional to square of the distance covered.
Question: Suppose that you used a negative point charge instead of a positive. Look at the data you recorded in the table – which of the columns would change, and how? Use the simulator to check your answer.
If we take a negative point charge of same magnitude, then all values will remain same except the direction of angle (in column 7). The direction off angle will become opposite (i.e 180 + values in column 7). So electric filed due to negative charge is radially inward, while due to positive charge, it is radially outward.
Part II: Electric Field of Multiple Charges
Procedure:
1) Use the charges to create an electric dipole with a horizontal axis by placing a positive and...
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