############################################################################## # Flags: nomenu, noprompt, nomessage, # ############################################################################## # section: -wlosses # ############################################################################## # symbol = h_1 # # quantity = h # # solution = 1 # # frequency = auto -- [auto | Real] # # bbxlow = -1.0000e+30, bbylow = -1.0000e+30, bbzlow = -1.0000e+30 # # bbxhigh= 1.0000e+30, bbyhigh= 1.0000e+30, bbzhigh= 1.0000e+30 # # # # # # @metalpower : undefined (symbol: undefined) # ############################################################################## # doit, ?, return, end, help, ls # ##############################################################################The conductivities that are used in the pertubation formula may be entered in the section -material. The result of the computation is available as the symbolic variable @metalpower. The wall losses are computed as:
The integration is performed over all metallic surfaces that would appear in a plot as produced by the section -3darrowplot. This implies, that wall losses are NOT computed for electric symmetry planes, since the material on the symmetry planes are not shown in -3darrowplot.
symbol= QUAN_ISOL
:
quantity= QUAN
:
solution= ISOL
:
frequency
:
"auto"
, the frequency is taken from the dataset.
If frequency
is specified as a number, that value is taken for
the integrand.
bbxlow=,bbxhigh=,bbylow=bbyhigh=,bbzlow=,bbzhigh=
:
doit
:
@metalpower
for subsequent
calculations.