Electron energy spectra and angular distributions, including angular s
preads, were measured using magnetic spectrometer techniques, at isoce
nter, for two clinical linear accelerators: one scanning beam machine,
which achieves field flatness by scanning a pencil beam over the desi
red field at the patient plane, and one scattering foil machine, which
disperses the electrons through a graded-thickness scattering foil. A
ll measurements were made at isocenter (in the patient plane), in air,
1 m from the nominal accelerator source. The energy measurements were
confined to electrons traveling along the central axis; any widely sc
attered electrons were effectively neglected. The energy spectra of th
e scanning beam machine are all of nearly Gaussian shape and energy fu
ll-width-at-half-maximum intensity (FWHM) of about 5% of the peak mean
energy (denoted [E(0)]). The energy spectra of the scattering foil m
achine have a variety of forms as a function of energy, including even
spectra with double peaks, and spectra which changed with time. The F
WHM values ranged from 9%-22% of [E(0)] The angular spread measuremen
ts, at isocenter, yielded sigma(theta x) x [E(0)] approximate to 295
mrad-MeV for the scanning beam machine, and 346 mrad-MeV for the scatt
ering foil machine, where sigma(theta x) denotes the standard deviatio
n of the plane-projected angular distribution. These angular spreads a
re 30%-40% smaller than angular spreads reported by others on a very s
imilar machine using the penumbra method. Possible causes of this disc
repancy are discussed. (C) 1996 American Association of Physicists in
Medicine.