Magnetic Filed Due to Solenoid
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A solenoid is a long cylindrical helix, which is obtained by winding closely a large number of turns of insulated copper wire over a tube of cardboard or china clay. When electric current is passed through it, a magnetic field is produced around and within the solenoid.
Consider a rectangular Amperean loop PQRS. Along PQ the field is zero. Along transverse sections PS and QR, the field component is zero. Let the magnetic field along SR be B.
∮ Bdl cosθ = μ0i
∮ B→dl→ = ∮ Bdl cosθ
= R∫S Bdl cos0 + Q∫R Bdl cos90o + P∫Q Bdl cos180 + S∫P Bdl cos90o
= B R∫S dl + 0 + 0 + 0 = Bl
Current passing through loop – 𝒏𝒍𝒊
Thus, the number of turns per unit length is ‘n’, then the total number of turns is ‘nh’. The enclosed current is Ie = I(𝑛ℎ) where I is the current in the solenoid.
From Ampere’s circuit law
BL = μ0Ie, Bh = μ0I(nh)
B = μ0nI
The direction of the field is given by the right-hand rule. The solenoid is commonly used to obtain a uniform magnetic field.