The transfer function for the Differential Mobility Analyzer (DMA) is deriv
ed based on particle trajectories for both nondiffusing particles and diffu
sing particles. The effect of particle diffusion is assessed by using a Mon
te-Carlo method for particles of sizes 1, 3, 10, 30, and 100 mm. This appro
ach includes both the effect of wall losses and axial diffusion. The range
of validity of the Stolzenburg analysis is assessed by comparing his transf
er function, the peak of his transfer function, and its dimensionless width
with similar calculations based on the Monte-Carlo. For particle sizes sma
ller than 10 nm, the Monte-Carlo method indicates large wall losses, which
result in a reduction in the peak of the transfer function by as much as a
factor of 10 to 30, sensitivity to the flow-field, and skewmess of the tran
sfer function. It is shown that Stolzenburg's approximate formula for the s
tandard deviation of the width of the transfer function agrees with Monte-C
arlo simulations for particle sizes of 3 nm and larger.