During electron beam processing, a fraction of the incident power gets back
scattered from the target surface, which can be as high as 40% of the incid
ent beam power depending on the beam energy and atomic number of the target
material. In the case of a strip electron gun, a uniform magnetic field is
used for focusing and deflection of electron beam through 270 degrees. Wit
h the strip beam (78 mm x 5 mm, 36 kW), experimental results of the 2-D dis
tribution of the backscattered electron current from copper target in its p
lane, parallel and perpendicular to the focal strip are presented. These re
sults are compared with calculated data using reported energy distribution
of backscattered electrons (E.H.Darlington, J. Phys. 8 (1975) 85). The inte
grated heat flux associated with backscattered electron is experimentally m
easured and compared with calculated values for incident power of 86 kW. Wi
th 12.25 kW/cm(2) of incident strip beam power, the back reflected electron
peak power density was observed to be 59W/cm(2). This power density will b
e higher for high incident power densities and for targets of high atomic n
umbers and dan be used in precoating treatments of substrate such as outgas
sing and cleaning, keeping it at elevated temperature during continuous coa
ting process, and also for outgassing, cleaning and sharing heat load requi
red for pre-melting of the feeder material during melting and casting. (C)
2001 Elsevier Science Ltd. All rights reserved.