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A small voltage like that could be coming from any number of extraneous influences. At that level the signal to noise ratio is low.
For a 10-degree Celsius temperature difference, a Type K thermocouple will generate approximately 0.41 millivolts (mV).
When dealing with low millivolt readings one has to be very careful to eliminate all extraneous influences and doing this is by no means simple. Even two different metals with a degree of surface oxidation can produce voltages in those ranges. As I said previously a vacuum chamber, sealed fluid containers, optimum insulated stands(Alan's polyethylene) and now I add another condition, a double layer Faraday screen are the minimum to do this with good signal to noise ratio. There could well be extra requirements to get a true result, I don't know as I am not an experimental physicist.
It is still not clear to me why an alternating current will induce a unipolar static charge on a nearby conductor.
Quote from: paul cotter on 13/12/2024 12:14:00It is way more likely that you dealing with artefacts from environmental effects rather than science has missed something as fundamental as this.My experiment is simple enough to be replicated by anyone else. Let's see how many of you can get the same results as mine. Do you find any problem with my theoretical background?
It is way more likely that you dealing with artefacts from environmental effects rather than science has missed something as fundamental as this.
Quote from: hamdani yusuf on 10/12/2024 13:15:54We will study the hypothesis that magnetic force is not only affected by the magnitude of electric charge that moves inside a conductor (or convector), but also affected by the mass of the particle.A very simple experiment that will disabuse you of this conclusion would be to measure the magnetic field produced by a given current around wires of materials with different Hall coefficients. I think you will find that the nature of the charge carrier is irrelevant.
We will study the hypothesis that magnetic force is not only affected by the magnitude of electric charge that moves inside a conductor (or convector), but also affected by the mass of the particle.
Hamdani, i have no intention of joining another long winded discussion that goes nowhere.
When you are dealing with low millivolt readings it is essential to make sure you are not dealing with some artefact of the local environment. I have already stated what I think would be the minimum requirements to avoid spurious readings and as I am not an experimental physicist I may have missed other necessary conditions. The history of science reveals a multitude of misleading of experiments where not all factors were taken into account. If I was to set up such an experiment I would have used Teflon stands until Alan pointed out that such a procedure would be prone to error- one small example of where thing could go wrong and in experimental science it is imperative to eliminate all possible contamination.
Your primary assumption is that you have measured what you think you have measured.
Your secondary assumption is that an alternating magnetic field can induce a unidirectional charge transfer between nearby conductors - in other words, that transformers are selfrectifying.
The third table shows the force experienced by test particle, which is simply the multiplication of each cell in both tables above. v+ -4 -3 -2 -1 0 1 2 3 4v- -4 0 -3 -4 -3 0 5 12 21 32-3 4 0 -2 -2 0 4 10 18 28-2 8 3 0 -1 0 3 8 15 24-1 12 6 2 0 0 2 6 12 200 16 9 4 1 0 1 4 9 161 20 12 6 2 0 0 2 6 122 24 15 8 3 0 -1 0 3 83 28 18 10 4 0 -2 -2 0 44 32 21 12 5 0 -3 -4 -3 0
I need to make assumption that my Voltmeter is reliable. I justified this assumption by measuring other electrical sources first, like batteries and USB charger. So far, I found no indication that it's false.
The magnetic force on a charge is zero if the charge is stationary.
It took Maxwell over 10 years and multiple papers to shape those equations in these final forms. The main difficulty was that Faraday?s field concept, on which his equations were based, was extremely hard to grasp. Maxwell had to rely on complicated mechanical models of molecular vortices in ether to come up with them. In this video, we will go through his heroic journey. Timestamps:0:00 - 0:42 Intro0:43 - 3:47 Status of Electromagnetism at his time3:48 - 5:06 Divergences and Flux5:07 - 6:33 How did Maxwell derive the first two equations?6:35 - 7:05 Limitations of hydrodynamics approach7:06 - 7:49 Molecular's vortices theory7:50 - 10:22 How did Maxwell derive the last two equations?10:23 - 10:47 Speed of light10:48 - 12:05 Maxwell's later abstract approach12:06 - 13:49 Why was his theory discarded by colleagues?13:50 - 14:48 Legacy of his equations
As many of you have correctly pointed out(many thanks for that), several embarassing typos have crept into the video. Here are some of the corrections: a. At 5:00, the clockwise curl should be negative, while the counterclockwise curl positive. b. At 10:00, "magnetic" should be "electric".c. At 10:21, displacement current (D) should be replaced with current density (J).d. In the displayed Maxwell equations, the propotional sign should have been replaced with the full equation. e. At 6:27, Laplace should be replaced by Lagrange. We would also like to add some remarks: a. Many animations, especially about divergences and flux, are borrowed from 3blue1brown channel. We have credited them in description but we should have also done in the video. We apologize for that, and make sure to correct it in coming videos. b. We do have a section regarding Oliver Heaviside's contribution at 14:08. Unfortunately, we are still not convinced that Maxwell equations should be renamed "Maxwell-Heaviside" equations. But, we will do more research, and maybe even change our mind:)
But non-zero if the wire moves relative to the charge.
Quote from: hamdani yusuf on 15/12/2024 14:26:32But non-zero if the wire moves relative to the charge.Which doesn't happen in your experiment. Your theoretical approach is incorrect. The current in the wire does not depend on the difference between drift velocities.