Moving Charges and Magnetism

 


1. The space in the surroundings of a magnet or a current-carrying conductor in which its magnetic influence can be experienced is called magnetic field. Its SI unit is Tesla (T).

2. Oersted experimentally demonstrated that the current-carrying conductor produces magnetic field around it.

Oersted experimentally

When key K is closed, then deflection occurs in the compass needle and vice-versa,

3. Biot-Savart’s Law According to this law, the magnetic field due to small; current-carrying element dl at any nearby point P is given by


Biot-Savart’s Law

4. The relationship between μ0, ε0 and c is

The relationship between μ0, ε0 and c is

where, c is velocity of light, ε0 is permittivity of free space and μ0 is magnetic permeability.

5. Magnetic field at the center of a circular current-carrying conductor/coil.

Magnetic field at the center of a circular current-carrying conductor/coil











6. Magnetic field at the centre of semi-circular current-carrying conductor.
Magnetic field at the centre of semi-circular current-carrying conductor.








7. Magnetic field at the centre of an arc of circular current-carrying conductor which subtends an angle 0 at the centre.

Magnetic field at the centre of an arc of circular current-carrying conductor which subtends an angle 0 at the centre.

8. Magnetic field at any point lies on the axis of circular current-carrying conductor

Magnetic field at any point lies on the axis of circular current-carrying conductor

9. Magnetic field due to straight current-carrying conductor at any point P at a distance r from the wire is given by
Magnetic field










10. The following figure shows the graphical representation of variation of B with distance from straight conductor.


Moving Charges and Magnetism

11. Ampere’s Circuital Law The line integral of the magnetic field B around any closed loop is equal to μ0 times the total current I threading through the loop, i.e.
Magnitude of magnetic field of a straight wire using Ampere’s law







13. Magnetic Field due to a Straight Solenoid
                (i) At any point inside the solenoid,
                    B = μ
0nI
                        where, n = number of turns per unit length.
               ii) At the ends of the solenoid,
                    B = 1/2 μ
0nI

Magnetic Field due to a Straight Solenoid

14. Magnetic Field due to Toroidal Solenoid


    (i) Inside the toroidal solenoid,
        B =μ
0nI, here, n =N/2Ï€r ,N= total number of turns

        (ii) In the open space, interior or exterior of toroidal solenoid,
        B= 0

Magnetic Field due to Toroidal Solenoid



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