Faraday’s law states that an electromotive force is induced in a circuit proportional to the rate at which the magnetic flux connecting it changes. Therefore, emf is the result of rotating a coil in a uniform magnetic field around an axis that passes through the center and perpendicular to the field’s direction.
emf= -dՓ/dt ՓB =B.Acos𝝷
=-d(B.Acos𝝷)/dt
=-BA d/dt cos𝝷
= -BA = sin d𝝷/dt
= emf = BAsin d𝝷/dt
Therefore, when sin𝝷 ↑, emf↑
Sin𝝷 = max when𝝷 =𝞹 /2
The angle between the coil’s plane and the magnetic field is zero when cosθ is maximum or θ is zero, or B⟂A when plane ∥ B, that is, when the angle between the area vector and the magnetic field is π/2.
Faraday’s law states that an electromotive force is induced in a circuit proportional to the rate at which the magnetic flux connecting it changes. Therefore, emf is the result of rotating a coil in a uniform magnetic field around an axis that passes through the center and perpendicular to the field’s direction.
emf= -dՓ/dt ՓB =B.Acos𝝷
=-d(B.Acos𝝷)/dt
=-BA d/dt cos𝝷
= -BA = sin d𝝷/dt
= emf = BAsin d𝝷/dt
Therefore, when sin𝝷 ↑, emf↑
Sin𝝷 = max when𝝷 =𝞹 /2
The angle between the coil’s plane and the magnetic field is zero when cosθ is maximum or θ is zero, or B⟂A when plane ∥ B, that is, when the angle between the area vector and the magnetic field is π/2.