Equipotential Lines and Electric Fields Labratory Experiment

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SUMMARY

The discussion centers on a laboratory experiment involving equipotential lines and electric fields, specifically using a voltage of 12 volts. Key equations include E=F/q for electric field calculations and ΔV = Ed for potential difference. Participants express confusion regarding the interpretation of the charge (q) and how to calculate ΔV using a voltmeter. The consensus is that the multimeter readout represents ΔV, and the electric field can be approximated by measuring the distance between equipotential lines.

PREREQUISITES
  • Understanding of electric fields and forces (E=F/q)
  • Familiarity with potential difference calculations (ΔV = Ed)
  • Experience using a voltmeter for measuring voltage
  • Knowledge of equipotential lines in electrostatics
NEXT STEPS
  • Learn how to accurately use a voltmeter for measuring potential differences
  • Study the relationship between electric field strength and equipotential lines
  • Explore advanced concepts in electrostatics, such as Gauss's Law
  • Investigate practical applications of equipotential surfaces in electrical engineering
USEFUL FOR

Students in physics courses, laboratory instructors, and anyone involved in experiments related to electric fields and equipotential lines.

llauren84
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Homework Statement


Our lab is not online, but this is so similar to what we did. http://physics.fullerton.edu/~SAM/PDF/Lab%20Manuals/212/Individual%20Experiments/Equipotential%20Surfaces%20E6.pdf" Instead of the ten that they set their voltage to, we set ours to 12.

Homework Equations



Eq. 1: E=Fq , where E and F are vectors, E is the electric field, F is the force on the charge, and q is the small positive test charge.
Eq. 2: \DeltaV = Ed, where \DeltaV is the potential difference, E is the electric field strength, and d is the distance between potentials.

The Attempt at a Solution



I am so confused and unfortunately, I can't ask the professor at this time. I have a few questions.
(1) I am not sure what q is exactly. Is that the number that the multimeter reads or is it the number 12 that we set our voltage to?
(2) How can I calculate \DeltaV?
(3) Do you think I should be doing different calculations for points on different equipotential lines if the q is the readout from the multimeter at those points or along the curve?

Basically, I just have no idea what to calculate. I am so used to charts as our data and I'm having a hard time taking the info from the curves that we drew to actual calculations.

Please help. Thanks so much. :confused:
 
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llauren84 said:
I am so confused and unfortunately, I can't ask the professor at this time. I have a few questions.
(1) I am not sure what q is exactly. Is that the number that the multimeter reads or is it the number 12 that we set our voltage to?
(2) How can I calculate \DeltaV?
(3) Do you think I should be doing different calculations for points on different equipotential lines if the q is the readout from the multimeter at those points or along the curve?

Basically, I just have no idea what to calculate. I am so used to charts as our data and I'm having a hard time taking the info from the curves that we drew to actual calculations.

Please help. Thanks so much. :confused:

(1) You don't know q, and don't need to worry about it.
(2) You measure it with a voltmeter.
(3) I'm not sure what you mean here. Along any equipotential curves, delta-V should be equal. You can approximate the electric field by measuring the distance between two equipotential curves and using the formula V=Ed; I think this is what the lab wants you to do.
 
llauren84 said:
Eq. 1: E=Fq , where E and F are vectors, E is the electric field, F is the force on the charge, and q is the small positive test charge.

Not E=Fq, but F=qE.
 
mikelepore said:
Not E=Fq, but F=qE.
Thank you =)

ideasrule said:
(2) You measure it with a voltmeter.
So the multimeter readout is the \DeltaV?
 

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