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This issue is sponsored by the Philips Romania, Lighting Division

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C Ţicleanu<br />

horizontal illuminance within <strong>the</strong> ax<strong>is</strong> of<br />

<strong>the</strong> main light-pipe was measured at certain<br />

d<strong>is</strong>tances from <strong>the</strong> diamond dome. In order<br />

to assess <strong>the</strong> potential of light d<strong>is</strong>tribution<br />

through <strong>the</strong> horizontal branches, vertical<br />

illuminance on <strong>the</strong> inner wall of <strong>the</strong> lightpipe<br />

was measured at certain d<strong>is</strong>tances from<br />

<strong>the</strong> diamond dome.<br />

Basing on <strong>the</strong>se values, a recurrence law<br />

was found to predict <strong>the</strong> illuminance at a<br />

certain point of <strong>the</strong> light-pipe for a certain<br />

value of <strong>the</strong> external horizontal illuminance<br />

at roof level.<br />

If E0 <strong>is</strong> <strong>the</strong> external horizontal<br />

illuminance at roof level, <strong>the</strong>n <strong>the</strong><br />

horizontal illuminance Eh,l within <strong>the</strong> lightpipe<br />

ax<strong>is</strong> at <strong>the</strong> d<strong>is</strong>tance l from <strong>the</strong> diamond<br />

dome will be<br />

Eh , l = E0<br />

− ϕ()<br />

l (4)<br />

where ϕ(l) <strong>is</strong> <strong>the</strong> recurrence function<br />

determined using <strong>the</strong> CurveExpert 1.3<br />

software based on <strong>the</strong> Levenberg-<br />

Marquardt method of nonlinear regression.<br />

The same applies for <strong>the</strong> vertical<br />

illuminance Ev,l on <strong>the</strong> inner wall of <strong>the</strong><br />

main light-pipe, which at <strong>the</strong> d<strong>is</strong>tance l<br />

from <strong>the</strong> diamond dome will be<br />

Ev , l = E0<br />

−ψ<br />

() l (5)<br />

where <strong>the</strong> recurrence function ψ(l) was<br />

determined using <strong>the</strong> same method as<br />

above.<br />

Beside <strong>the</strong> light transm<strong>is</strong>sion of <strong>the</strong> main<br />

light-pipe, <strong>the</strong> transm<strong>is</strong>sion character<strong>is</strong>tics<br />

of <strong>the</strong> secondary branch pipe were assessed.<br />

Basing on <strong>the</strong> same algorithm, <strong>the</strong><br />

illuminance Ebδ at <strong>the</strong> d<strong>is</strong>tance δ from <strong>the</strong><br />

ramification within <strong>the</strong> ax<strong>is</strong> of <strong>the</strong> branch<br />

was expressed as a function of <strong>the</strong> initial<br />

illuminance Eb at <strong>the</strong> entrance in <strong>the</strong> branch<br />

and <strong>the</strong> d<strong>is</strong>tance δ:<br />

42<br />

INGINERIA ILUMINATULUI 18-2006<br />

( δ )<br />

E b,<br />

δ = Eb<br />

− β<br />

(6)<br />

where <strong>the</strong> recurrence function β(δ) results<br />

using <strong>the</strong> same algorithm as for <strong>the</strong> main<br />

light-pipe.<br />

The first measurements were taken using<br />

a 75 W incandescent lamp as <strong>the</strong> light<br />

source for <strong>the</strong> main duct. The illuminance<br />

within <strong>the</strong> ax<strong>is</strong> of <strong>the</strong> light-pipe at <strong>the</strong><br />

d<strong>is</strong>tance L=23 cm from <strong>the</strong> lamp socket’s<br />

base plane was considered as <strong>the</strong> initial<br />

illuminance E0. Several measurements were<br />

taken and <strong>the</strong> mean values are shown in <strong>the</strong><br />

table below.<br />

Horizontal illuminance within pipe ax<strong>is</strong><br />

L, cm l, cm Eh,l, cm ΔEh, cm<br />

23 0 31,500 0<br />

33 10 29,533 1967<br />

43 20 28,467 3033<br />

53 30 27,733 3767<br />

63 40 25,833 5667<br />

73 50 24,333 7167<br />

Vertical illuminance on pipe’s inner wall<br />

L l Ev,l ΔEv<br />

23 0 12,000 19,500<br />

33 10 9750 21,750<br />

43 20 8850 22,650<br />

53 30 8425 23,075<br />

63 40 8150 23,350<br />

73 50 7875 23,625<br />

L <strong>is</strong> <strong>the</strong> d<strong>is</strong>tance from <strong>the</strong> socket’s base<br />

plan at which <strong>the</strong> horizontal and vertical<br />

illuminances Eh,l and Ev,l are measured, l <strong>is</strong><br />

<strong>the</strong> length at <strong>the</strong> measurement point relative<br />

to <strong>the</strong> point where <strong>the</strong> initial illuminance E0<br />

<strong>is</strong> measured, and ΔEh and ΔEv are <strong>the</strong><br />

differences of illuminance E0–Eh,l and E0–<br />

Ev,l respectively.<br />

In order to see <strong>the</strong> light amplification<br />

effect specific to <strong>the</strong> SunPipe, <strong>the</strong> table<br />

below shows <strong>the</strong> illuminance generated <strong>by</strong>

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