To calculate electron beam dose distributions accurately, numerical me
thods of electron transport calculations must account for the statisti
cal variation (or ''straggling'') in electron energy loss. This paper
shows that the various energy straggling theories that are applicable
to short path lengths all derive from a single statistical model, know
n as the compound Poisson process. This model in tum relies on three a
ssumptions: (1) the number of energy-loss events in a given path lengt
h is Poisson distributed; (2) events are mutually independent; and (3)
each event has the same probability distribution for energy loss (i.e
., the same energy-loss cross section). Applying the principles of the
compound Poisson process and using fast Fourier transforms, a new met
hod for calculating energy-loss spectra is developed. The spectra calc
ulated using this method for 10, 20, and 30 MeV electrons incident on
graphite and aluminum absorbers agreed with Monte Carlo simulations (E
Gs4) within 1% in the spectral peak. Also, stopping powers derived fro
m the calculated spectra agreed within 1.2%, with stopping powers tabu
lated by the International Commission on Radiation Units and Measureme
nts. Several numerical transport methods ''propagate'' the electron di
stribution (in position, direction, and energy) over small discrete in
crements of path length. Thus the propagation of our calculated spectr
a over multiple path length increments is investigated. For a low atom
ic number absorber (graphite in this case), calculated spectra agreed
with EGS4 Monte Carlo simulations over the full electron range, provid
ed the path length increments were sufficiently small (less than 0.5 g
/cm2). It is concluded from these results that numerical methods of el
ectron transport should restrict the size of path length increments to
less than 0.5 g/cm2 if energy straggling is to be modeled accurately.