Faraday's Law of Induction - Experiment Giving Weird Results?

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Discussion Overview

The discussion revolves around an experiment attempting to induce current in a coil using Faraday's Law of Induction. Participants are comparing their experimental results with theoretical calculations and exploring discrepancies between the two. The scope includes theoretical reasoning, experimental methodology, and potential sources of error.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Experimental/applied

Main Points Raised

  • Participants express concern over the significant difference between experimental and theoretical results, questioning potential errors in their methodology.
  • One participant suggests that the internal resistance of inexpensive multimeters may affect current measurements, proposing the use of an op-amp based current amplifier for more accurate readings.
  • Another participant notes that the resistance of the copper wire is likely lower than the measured 3 ohms, attributing some resistance to contact points.
  • Discussion includes the idea of using more turns in the coil to increase induced voltage and improve measurement accuracy.
  • One participant calculates the wire resistance per meter based on the coil dimensions and questions the gauge of wire used, suggesting it may be too fine for the reported resistance.
  • Concerns are raised about the speed of the milliammeter, which may not accurately capture the transient current due to its stabilization time.
  • Another participant introduces the concept of a counter magnetic field generated by the loop current, which could reduce the effective magnetic field and thus the induced current.

Areas of Agreement / Disagreement

Participants generally agree that there are discrepancies between the experimental and theoretical results, but multiple competing views on the causes of these discrepancies remain. No consensus is reached on the specific sources of error or the best approach to resolve the issues.

Contextual Notes

Limitations include potential inaccuracies in measurements due to the multimeter's internal resistance, the gauge of wire used, and the transient nature of the induced current. The discussion does not resolve these limitations.

Who May Find This Useful

This discussion may be useful for students and educators involved in experimental physics, particularly those interested in electromagnetism and the practical applications of Faraday's Law of Induction.

Peter2
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Member advised to use the homework template for posts in the homework sections of PF.

Homework Statement


[/B]

Hi everyone, some school mates sugested id try this forum for help with this work i have :)
- will try to keep it short

We were trying to induce current in a coil and confirm the experimental results with math, but the math is way off and nobody is sure why...Experiment:
  • Cooper Coil (3Ω) (measured with multimeter)
  • Rectangle (6.5 cm x 3,5 cm) → Area ≈ 0.002275 m2
  • Number of Turns 6
  • Magnet Rectangle (4cm x 10cm x 5cm) (3050 Gauss) → 0.305 Tesla
  • Δt of passing the magnet was around 1sec... but we had a hard time keeping this scientific and precise
Results:
  • Digital Multimeter set to 2mA - Average of the readings turned out 0.0048
  • 0.0048mA → 48x10-7 A
  • I = V/A → V = 0.000014 Volts

Homework Equations



Now for the Theoric Rusults:

  • Φ = B ⋅ A ⋅ cosθ → Φ= 0.305 ⋅ 0.002275 ⋅ cos0 = 0.000694
  • ξ= - N ⋅ (dΦ/dt) → ξ = - 6 ⋅ 0.000694/1 = 0.004163 Volts

The Attempt at a Solution



Why there is such a big difference in our math vs our experience?
Are we doing something wrong?Thanks for any help ;) Cheers!
 
Last edited:
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Peter2 said:

Homework Statement


[/B]

Hi everyone, some school mates sugested id try this forum for help with this work i have :)
- will try to keep it short

We were trying to induce current in a coil and confirm the experimental results with math, but the math is way off and nobody is sure why...Experiment:
  • Cooper Coil (3Ω) (measured with multimeter)
  • Rectangle (6.5 cm x 3,5 cm) → Area ≈ 0.002275 m2
  • Number of Turns 6
  • Magnet Rectangle (4cm x 10cm x 5cm) (3050 Gauss) → 0.305 Tesla
  • Δt of passing the magnet was around 1sec... but we had a hard time keeping this scientific and precise
Results:
  • Digital Multimeter set to 2mA - Average of the readings turned out 0.0048
  • 0.0048mA → 48x10-7 A
  • I = V/A → V = 0.000014 Volts

Homework Equations



Now for the Theoric Rusults:

  • Φ = B ⋅ A ⋅ cosθ → Φ= 0.305 ⋅ 0.002275 ⋅ cos0 = 0.000694
  • ξ= - N ⋅ (dΦ/dt) → ξ = - 6 ⋅ 0.000694/1 = 0.004163 Volts

The Attempt at a Solution



Why there is such a big difference in our math vs our experience?
Are we doing something wrong?Thanks for any help ;) Cheers!
The equations are simple enough and you are only doing estimates, but if you got reasonably good measurements of the resistance and current, I think you should get results that are reasonably consistent with the theoretical calculations. One thing that inexpensive multimeters often have is an internal resistance that affects the measurements. I do think the resistance of your copper wire is likely to be considerably less than 3 ohms, and if you got a good reading of the current in the circuit without the meter's resistance supplying some impedance to the current flow, I do think the current may have been higher than what you measured. I would recommend using an op-amp based current amplifier (current to voltage amplifier) circuit and measure the output of that circuit with an oscilloscope. Alternatively, you could measure the EMF produced by connecting the coils to the high impedance (1 Mohm) input of the oscilloscope and simply measure the voltage generated from the process of moving the magnet through the coils.
 
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Many thanks for the reply Charles.

Cool, i was worried something was off with the equations, ill add an op - amp and retry the experiment, and maybe even try a new coil with more (30-40) loops to try and compensate for the multimeters internal resistance :wink:
 
Peter2 said:
Many thanks for the reply Charles.

Cool, i was worried something was off with the equations, ill add an op - amp and retry the experiment, and maybe even try a new coil with more (30-40) loops to try and compensate for the multimeters internal resistance :wink:
Copper wire I believe is quite low resistance. Much of your resistance could occur at the contact point, etc. Perhaps your best EMF measurement would be done directly by reading the voltage from the coils on an oscilloscope. Extra loops to give you a higher voltage would probably improve the accuracy.
 
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I agree with Charles. 3 Ohms sounds high for just 6 turns of wire.
 
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It might be interesting to investigate what gauge of wire would be required to produce the reported coil resistance of 3 Ω.

The perimeter of the 6.5 cm x 3.5 cm rectangular coil is 20 cm. With 6 turns that yields a total wire length (excluding any connection leads) of 1.2 m. So the wire resistance per meter would be 2.5 Ω/m (or 0.762 Ω/ft for fans of feet and inches). That's close to a 39 gauge copper wire, with a diameter a bit less than a hair's width (less than 0.1 mm). That's a pretty fine wire.

Perhaps the OP can share what he observed regarding the thickness of the coil wire? Did it appear to be as thin as a hair?

An alternative is that the wire is not copper but some other material with more ohms-per-meter. For example, a 20 gauge nichrome wire might fit the bill.
 
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You milliammeter is probably much too slow to record the current accurately. The current will come & go in under 1 sec. Most digital m/a meters need several seconds to stabilize the reading.

Use a current-sampling resistor (say 1K ohms in series with the coil & look at the voltage across it with a 'scope. Voltage should peak around 4 mV and current around 4mV/1K = 4 μA.
 
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Also, you may be generating a counter B field by the loop current sufficient to reduce the vector sum of your applied magnet B field
and the counter-B field to reduce the current appreciably below computed numbers. emf = d/dt A(external B - induced B). The induced effective B as a function of current is very difficult to compute for a thin loop. But using a 1K resistor as I proposed reduces the induced B field to practically zero.
 
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