For any camera, of course, the delivered DR at any ISO is the raw
saturation level divided by the read noise at that ISO. This is the
definition that Clark uses when he reports 'camera dynamic range';
unfortunately, he doesn't record those for more than a handful of
cameras, and spends most of his time quoting values for 'sensor
dynamic range', which is not what the camera delivers.
So how does he get at this 'sensor DR'? Read noise has two broad
classes of contributions -- those upstream of the ISO amplifier and
those downstream. The latter don't get amplified proportionally by
the ISO setting, while the former do; thus by measuring the read
noise at several ISO settings one can determine the upstream and
downstream contributions separately, see the table below fig 15 on
page 3 of my article
http://theory.uchicago.edu/~ejm/pix/20d/tests/noise/noise-p2.html#read_vs_iso
It turns out that low ISO read noise is dominated by the downstream
contributions -- the ISO amplifier itself and the ADC -- while high
ISO read noise is almost entirely due to the amplified upstream
contribution, which comes from the sensor. If the downstream
electronics weren't overwhelming the sensor contribution at low ISO,
the delivered DR
would be the full well capacity/high ISO read
noise (all measured in electrons), which on pro level Canons and
Nikons is about 14 stops. It is only the limitations of the
amplifier/ADC combination that are preventing the delivery of that DR
in current cameras.