IES Luminaires and Spectral Radiance
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IES Luminaires and Spectral Radiance
The IES file format[1] for the transfer of photometric data defines
the distribution of light from a luminaire. The distribution is defined for
a point light source even though most luminaires have a luminous aperture
of some area. The file format specifies luminous intensities,
, for a
set of directions, thus allowing for non uniform distributions. In order to
compute spectral radiance from this information we must make two
assumptions: that the photometry can be spread uniformly across the
luminous apperature and that a spectrum exists which defines the color of
the luminaire. If the luminous apperature is polygonal, we can make the
first assumption understanding that the photometry will be correct for
distances in which the luminaire subtends a "small" solid angle of the
hemisphere above the illuminated point. The photometry will be incorrect if
the luminaire subtends a "large" solid angle with respect to the
illuminated point, however, in most cases the results will look reasonable.
Usually the type of lamp used in the luminaire will be defined in the
IES file. By maintaining a database of spectra that correspond to particular
lamp types, the second assumption can be made. In the case that no
lamp type is specified a default spectrum can be used. Some of
these spectra can be found in the IES Lighting
Handbook[3] others are distributed by the lighting
manufacturers. Fortunately, these spectra are defined in terms of
or spectral radiant flux
. This will allow us to derive a
function of spectral radiance
. The derivation is as
follows:
The known quantities are luminous intensity
,
spectral radiant flux
, the maximum spectral luminous
efficacy
, and the photopic luminous efficiency curve
. The goal is spectral radiance
.
However, based on our assumption that the photometry can be spread
uniformly across the surface of the luminaire, the following
relationship holds:
Therefore if we solve for spectral radiant intensity,
,
we will have a solution for
. Observe also that
spectral radiant flux is in units of
and that spectral
radiant intensity is in units of
. This merely points
out that
where
is a scalar determined by
, the direction in which
the spectral radiant flux is traveling.
can be solved for by
using
. From the previous definitions we know
and since
does not depend on
it can be moved out of the integral
thus
Radiance is then by Equation (1):
Copyright (C) 1995 Kurt Zimmerman
Department of Computer Science
Indiana University
kuzimmer@cs.indiana.edu