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Light
intensity
We should specify a standard source in order to
define the light intensity in a clearer way. A standard source is
any body which radiates energy, although not all the energy is
considered lighting energy (the one we perceive through the sense
of sight) but part of that lighting energy is converted into heat
and non visible radiations. So, part of that energy which is emitted
by a source, is not a visible energy. The lighting radiations
come from the warming of a given material by which energy radiates.

This standard source consists of a cylindrical
tube made of heat-resistant material (Torio), with the highest
melting point, surrounded by pure platinum.The tube gets wider in
its end forming a solid angle of a steradian.
Once this total radiator is heated over a
temperature of 2045 K ,it emits
a certain quantity of radiant energy, 1mē/600000 of this energy
is our measurement of reference and it is what we call candle (cd).
The light intensity (I),
fundamental feature of the source of radiation is given by the
lighting flux F which is emited in a specified way by a unit of
solid angle W, in other words, the lighting power of the source
which is expressed in watts.

Since the lighting flux is measured in
lumens, the unit of light intensity will be the lumen in
a steradian, which is called candle (cd).
However, measuring the power that belongs
exclusively to the visible area is not an easy task because most
of the sources emit in a broader area of the electromagnetic
spectrum.
In order to measure the intensity of a source
it is necessary to define a unit which must be constant and
invariable in relation to a given surface in order to measure the
intensity of a source.
The International System of Unities (IS)
included the CANDLE as a unit of measure of light intensity of
a source.
The candle (cd) may be defined as the lighting intensity in a certain direction of a source which emits
monochromatic radiation with a 540 x 1012 Hz
frequency equivalent to 555 nm in the vacuity. The candle has an
intensity of radiation in that direction of 1/683 watts per each
steradian.
The "chosen frequency" is the one to
which the eye is more sensible and is usually quantized in the
Light Literature as one wavelength of 555 nanometers.
The wavelength varies according to the
environment through which the light goes right, so if we
want to specify this, we could say that the light wavelength we
understand is not the one used by the standard mode.
Our strange choice of the 683 factor is
because we want the value to be identical to the
one obtained with the previous version of the unit: the 1cmē
emission of solidified platinum shine.
The steradian (sr) is the
cone light that is given off from the source which lights 1mē
of a dark surface in a meter radius around the source. (That is
to say, 1 steradian covers 1mē of a surface of 1m of diameter
sphere).
The apparent shine of a source when is
looked directly at it must not be confused with its light emission. The
shine of a source is measured through the candle by square metre (cd/mē) and its magnitude is called
luminance.
The luminence (L) is the
lighting magnitude which determines the impression of a more or
less brightness produced by a surface. The luminence is a common
concept in the shine of an object, either with relation to the own
produced light, or reflected (source which emits light, source
of light which is only reflected or source of light which has both
emissions). It is defined as the luminous sensation which is
produced in the retina of the eye because of the effect of the
light. It is the superficial density of the light intensity and
is expressed as the relation between the luminous intensity and
the surface from which is emitted:

V-LAMBDA
Curve
The measurement of the light intensity requires information about the relative sensitivity of the human
eye for different wavelengths.
The eye has two different sensitivities
according to the kind of lighting. The photopic vision for
normal and strong lightings and the scotopic vision for the low
ones.
Because of this fact the same sensation of
shine is not produced for equal quantities of lighting flux of
different wavelengths. So, for example, for the
same sensation of shine, it obtains a higher sensation of shine
for the yellow-green than for the ends of the red-purple.
The light intensity of a white light source is
defined by the product of the watts which are emitted for each
wavelength through the output of that wavelength by exciting the eye,
which output is 555nm. This factor of output is known as
V-lambda curve.
The curve defines the relation between
the sense of human light and the physical concept of light, which
is the quantity the instruments of measurement react to.
The watts which are emitted by a source of light can
be measured by absorbing all the light in a black ideal surface and by
measuring the heat that has been produced. A filter which belongs to the V-lambda curve can be
placed in front of a black surface in order to convert the result and
with that the eye and the human brain may value the brightness. The measurement
instruments have sensors of
filtrate which are able to turn the absorbed light by the
V-lambda into electric current.
Lumen
and lux
The lighting flux (f) is the power
(energy per one unit of time) of the lighting energy which is measured
according to its visual effect (it is equivalent to one candle per each
steradian). That is, it indicates the quantity of
light which is emitted in a unit of time in an specific direction (spatial
distribution of the light which is emitted by the source). Its unit is
the lumen (lm).683 lumens are the equivalent of one watt, emitted to 555 nm
wavelength, which
is the equivalent of the highest sensitivity of the
human eye.
The definition of lumen, the unit of a lighting flux,
is:
"The lighting flux (dF) is a source of light
Intensity I (cd) at an angle with a solid element given
by dF=IdR"
This means that the flux of a light source equals
its intensity in candle multiplied by the solid angle over which the
light is emitted, taking into account the variation of intensity that
it produces in different directions.

In the image we can observe a point of light of the
green ray emitting a 300 cd light intensity for a 30š angle.
We have already seen the concept of solid angle;
if we take into consideration a source which emits a certain radiant
energy and that this supposedly does it in all directions, we
can consider this one as an sphere. The solid angle will determine one
cone which takes up a certain surface or area (s), in relation to
the radius unit.
In these conditions, the measurement in steradians
of the solid angle W is defined due to:
Since the area of a sphere is 4πr2
if we replace it, we will get:

When S = r2 the solid angle will be of
one steradian. According to this we could define the lumen in this way:
"It is the lighting flux that goes through a
solid angle of a steradian in one second, emitted by a precise
source whose intensity is of one candle."

The output is a magnitude derived from the
lighting flux. When we talked about light intensity we mentioned that not
all electric current consumed by a lamp (light bulb, fluorescent,
etc.) is turned into visible light. Part of it gets lost by heat,
part by non visible radiation (infrared or ultraviolet) etc.
We define the lighting output (h) as the
quotient between the produced lighting flux and the consumed electric
power, characterized by the lamps (25 W, 60 W...). The bigger it
is,, the
better the lamp will be and the consumption will be less. The unit is
lumen per
watt (lm/W).

The lumen formally derives from the candle, based
on a light of simple wavelength. A lamp of several wavelength has an exit of lumens
which is calculated from the watts emitted as the radiation multiplied
by the luminous efficiency in each wavelength, as it was described in
the case of the candle.
The designer needs to translate the values of cd
into Luminous Energy which reaches an object to a certain distance
from the lamp. It is this energy which makes the object visible and
which turns pale its nuances of color. The energy density which
reaches the object is expressed in lumens per square meter (Lm/mē),
what is known as lux.
This value can be easily calculated from the
diagram by a starting point. The candle value (300cd) given by 60° is the same
that 300 lumens flowing in the cone of a steradian (sr),
that by definition takes up 1mē of the surface of 1m diameter sphere.
If our object were in that distance, it would
be receiving 300 lm/mē.
In order to deduce the value of any other distance,
the same rule must be used in the reverse way. As far as 3m of the
lamp, the flux over 1mē declines to 1/9 from the 300lm. The lux
value is 33.
The illuminance (E) is the lighting flux that falls on a
surface, divide by the size of such surface (s).
The illuminance is the magnitude of assessment of the light level of a surface or of a spatial
zone.
Its unit of measure is the Lux (Lx), equivalent to the
light which falls on each mē of a surface and on which a lighting
flux of a lumen is distributed uniformly.
The illuminance depends on the distance from the focus to
the lighted object. It is something similar to what happens when we listen
to a car moving away; at the beginning we can hear it loud and clear, but
later it decreases until it gets lost. What happens with the illuminance
is known as the reverse law of the squares which relates the lighting
intensity and the distance to the source. This law is only valid if the
direction of the ray of incidental light is perpendicular to the surface.
Reverse law of squares:
In case the ray of light that falls on isn't
perpendicular, we have to break up the illuminance to the surface in an
horizontal and vertical component.
The horizontal component of the lighting (EH)
is known as the cosine law. It isn't difficult to see that if
= 0 we have the inverted law of the squares. If we express EH y
EV
depending on the distance of the focus to the surface (h) we have:

Normally, if a point is being lighted by more than a
lamp, its total lighting is the sum of the received light.
Units
and conversion tables.
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Measurements
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Units
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Symbol
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Conversion
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Light
intensity
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Candle
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cd
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cd
= lm/sr
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Lighting
flux
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Lumen
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lm
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lm
=cd/sr
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Illuminance
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Lumen
per square foot
Candle
foot = lm/ft2
Phot
= lm/cm2
Nox
= millilux
m-candle
= lux
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Lm/ftē
fc o ft cd
Phot
Nox
m-cd
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1lm/ft2
= 10.79lm/m2
1fc
= 10.76lx
1Phot
= 10-4lx
1Phot
= 0.929fc
1Nox
= 10-3lx
1m-cd
= 1lm/m2 = 1lx
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