INTERACTIVE EXPERIMENTS AND EXHIBITS
COILS, SOLENOIDS AND OTHER THINGS
Let’s see a property of the magnetic field on the inside of the solenoid when the wire is electrified.
This is a solenoid with about 100 windings in two layers. The wire is thick and, on connecting it to a 1.5 V battery, the current can be about 1A.
When the length of a solenoid having n windings per unit of length and electrified by current I is much greater than its radius, the induction field inside it is parallel to its axis and its modulus is given by the following expression:
André Marie Ampere (1775-1836), France, a great mathematician and physicist.
The fundamental Theorem of Ampere connects generic configurations of currents to the fields they generate.
Ampere’s theorem is important since it allows calculation of the field generated by currents in a circuit of different forms.
If in the solenoid we introduce a nucleus of material having magnetic permeability µ this is magnetized with a magnetic induction µ times greater. Ferromagnetic materials (iron, nickel and many others) may reach values of µ of even 1000. This is why electric motors, electromagnets and so on always have an iron nucleus.
One instrument that Ampere made much use of consisted of the magnetic needle of a compass inside a coil of isolated wire through which he sent the current to see or measure. This was the first kind of galvanometer, later known as the “tangent compass” since the current is proportional to the tangent of the needle’s angle of deflection.
This small instrument, which anyone can build, is sufficiently sensitive to reveal the thermoelectric current generated at the copper-costantan joint when it is heated (the thermoelectric effect or Seebeck effect)