We analyze the kinematic and the dynamic self-excited disk dynamo mode
ls for natural dynamos. In the kinematic model (given disk angular vel
ocity), the magnetic field can either increase or decrease exponential
ly with time, or it can be constant if the angular velocity has a spec
ific value that is a function of the geometry and of the resistance of
the circuit. With the dynamic disk dynamo (given mechanical power inp
ut), there are both transient and steady-state solutions, and the stea
dy-state magnetic flux density is proportional to the square root of t
he power input. The polarity of the induced magnetic held in either dy
namo is the same as the seed field, and erratic polarity reversals can
be expected if the power input is erratic.