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No, it was found by expirement.

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No, it was found by expirement.

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Depends on whether a path integral or a normal integral is easier to determine.

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According to Coulomb's law, the electrostatic force between two point charges is directly proportional to the product of their magnitudes and inversely proportional to the square of distance between their centers.

And Biot Savart's law gives the magnetic field at point due to a small current element. And, according to Biot Savart's law ,the magnitude of magnetic field is directly proportional to the product of current element Idl and Sin theta and inversely proportional to the square of distance between two point charges.

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----> ampere's law :

which is to be used while finding magnetic fields inside the enclosed surface. we are allowed to use it to any surface however the surface have to be in such ways that the path must pass through the point and the path must have enough symmetry so that is constant along the large path of it!

----> Biot Savart law : we often use biot savart to find magnetic fields

generated by an electric current carrying wire of radius "r" and since the radius is perpendicular with I we don't worry about messy integration!

thus we left with : dB =( µ_0 Idl) / (4πr^2)

also knowing that l = 2πr helps so we substitute it in! and we eventually end up with : dB =( µ_0 Id2πr) /(4πr^2)

Thus B = µ_0 I / 2πr

Combining Ampere Law to Biot savart.

Thus we can derive Biot savart from ampere by the following:

§ B.dl = µ_0 I (encl)

B § dl = µ_0 I (encl) hence B (2πr) is

B(2πr) = µ_0 I

so B = (µ_0 I) / 2πr

faith nshuti.

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A classic and ancient experiment is to get a compass, a battery (9volt is fine), and some wire. Notice that the compass changes when the circuit is closed (wire connected to the two terminals). You can also see that the compass gets affected less when it is far from the wire versus next to it.

If your interested in the math behind the experiment, you may want to do some research on the Biot-Savart Law. The Biot-Savart law describe the magnetis field when the current is constant, or not time-varying. A more general form of the equation is called Ampere's Law, and the more general case of that is Maxwell's equations.

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