A conducting disc of radius r rotates with a small but constant angular velocity ω about its axis. A uniform magnetic field B exists parallel to the axis of rotation. Find the motional emf between the center and the periphery of the disc.
Given:
Radius = r
Angular velocity = w
Magnetic field = B
Diagram:
Formula used:
In this case, the velocity will increase radially.
Let us consider a strip of width dx at a distance x from the centre.
Hence, induced emf of this portion will be , where B = magnetic field, dx = width of the element, x = distance of the element from the centre, w = angular velocity
Hence, integrating on both sides using proper limits, we get
=> Total motional emf (Ans)