3.5
trobosco
ic effect and flicke
peration of a metal halide lamp on a ma
netic ballast
nder supply voltage with 50 Hz
requency results in
eriodic
luctuation o
the luminous
lux with double
the suppl
requenc
. When the current
low drops
ear the zero crossin
, the plasma also has
ar less
ra
at
on.
ut even on pass
n
t
e zero cross
n
, t
e
luminous
lux does not reach zero so that the
lasma
st
as on-
o
n
ra
at
on.
The human eye reacts with di
erin
sensitivity to
varyin
licker
requencies, and can,
or example, no
lon
er perceive
luctuations in luminous
lux above
100 Hz. Literature provides di
erin
ways o
depictin
the sensitivit
o
the human e
e
or periodic luminous
lux
luctuations at various
requencies. Fi
. 17 shows
an example accordin
to Kelly and Hen
er
1
When operatin
at 50 Hz, the luminous
lux or intensity
luctuates with watta
e, i.e. with 100 Hz as shown in
. 15.
terature uses var
ous equat
ons to eva
uate
chan
es in luminous intensity that can be perceived
y t
e
uman eye.
c
er
s eva
uate
accor
n
to
EN 50006 standard,
or exam
le, with a
licker
actor
1
whereb
m
= time-de
endent modulation de
th
the luminous intensit
= filter curve for flicker sensitivit
dependin
on
licker
requenc
ccordin
to Afshar
2
, adaptin
the evaluation also to
short-term changes and implementation in a
ilter
o
a li
ht si
nal, such as in Fi
. 15, results in values
or
the
licker
actor as shown in Fig. 16. The perceptibility
t
r
m
t
1.
v
n t
x-
amp
e rema
n
e
ow 1,
.e. no v
s
e c
anges can
e
perce
ve
n t
e
t
()
∑
=
i
ii
fGfmF )²
1
0
²
)
Fi
. 15: Luminous intensit
o
a metal halide lamp at
50
z c
o
e operat
on, s
own
n ar
trar
un
t
Fi
. 16: Flicker
actor calculated
rom the luminous
ntensit
si
nal
or a metal halide lamp at 50 Hz choke
operat
on, s
own
n ar
trar
un
ts
Fig. 17: Eye sensitivity curve
or
licker as per Kelly
1960 and Hen
er 1985
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