In the half-wave rectifier, this corresponds to the
slightly-less-cartoonish model of the diode, in which you take into
account the voltage drop and the forward and backward
resistances of the diode. When the diode is forward-biased at greater
than
(assume here 0.6 V), the output follows the positive
swing of the input. You get a positive hump, but at lower than the signal voltage
according
to
, taking into
account both the voltage drop across the diode,
, and the
voltage division (note that here, because
is small, the voltage
divider factor is
). Then, during the negative swing of the
input, you treat the diode as a large resistance
, and the output
follows the input according to the voltage divider equation, as
, where
is now a
small number- so you get a much reduced (but non-zero) negative swing
on the output.