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You’ve no doubt seen plenty of fluorescent lights,

00:00:03.181 --> 00:00:05.683  
but have you ever seen one like this?

00:00:05.683 --> 00:00:08.562  
It may not seem all that strange at first glance,

00:00:08.562 --> 00:00:13.163  
after all&nbsp;there have been plenty of weird fluorescent lamp designs over the years.

00:00:13.163 --> 00:00:16.607  
But this one’s missing a&nbsp;pretty crucial part:

00:00:16.607 --> 00:00:18.964  
the electrical connections.

00:00:18.964 --> 00:00:24.934  
Your typical fluorescent tube has little wires&nbsp;attached to pins which stick out of the glass at each end,

00:00:24.934 --> 00:00:28.606  
and they connect to electrodes inside the tube.

00:00:28.606 --> 00:00:33.869  
Those wires are then connected to a ballast and starter which together place a voltage on&nbsp;
the electrodes

00:00:33.869 --> 00:00:37.654  
to pump electricity through the lamp which makes it glow.

00:00:37.654 --> 00:00:41.725  
But this… this is&nbsp;just a glass tube.

00:00:42.689 --> 00:00:44.459  
How’s that supposed to work?

00:00:44.858 --> 00:00:47.228  
Well, with these.

00:00:47.228 --> 00:00:51.341  
The tube is designed to&nbsp;be held in place by a pair of…

00:00:51.341 --> 00:00:53.752  
let’s call them electromagnets.

00:00:53.752 --> 00:00:56.809  
That’s not exactly the&nbsp;right word which will become clear in a moment

00:00:56.809 --> 00:01:03.358  
but each one of them is formed by wrapping a&nbsp;wire around a ferrite core several times.

00:01:03.358 --> 00:01:06.521  
With the help of electronics inside this driver&nbsp;unit,

00:01:06.521 --> 00:01:09.966  
a high-frequency alternating current is sent through the wires

00:01:09.966 --> 00:01:17.173  
which then causes a&nbsp;magnetic field to repeatedly form, collapse, and form again inside the ferrite cores.

00:01:17.605 --> 00:01:20.610  
Now, if&nbsp;you know a little bit about power transformers,

00:01:20.610 --> 00:01:26.395  
then if we take the tube out of the picture&nbsp;for a moment and look at a core by itself,

00:01:26.395 --> 00:01:33.228  
then what we’re looking at appears to be a toroidal&nbsp;power transformer that somebody forgot to finish.

00:01:33.228 --> 00:01:39.189  
See, usually we’d have at least two coils&nbsp;of wire wrapped around one of these cores.

00:01:39.189 --> 00:01:44.218  
When we run alternating current through the&nbsp;first coil of wire, called the primary winding,

00:01:44.218 --> 00:01:48.369  
it will induce a rapidly changing magnetic field&nbsp;through the core

00:01:48.369 --> 00:01:54.041  
which in turn induces a voltage on the other coil of wire known as the secondary&nbsp;winding.

00:01:54.407 --> 00:01:58.570  
When that secondary winding is part of a circuit, current will flow

00:01:58.570 --> 00:02:07.039  
and the upshot is that&nbsp;energy is transferred from the primary winding, through the core, and into the secondary winding.

00:02:07.039 --> 00:02:11.593  
We often do this because the secondary winding will produce a different voltage

00:02:11.593 --> 00:02:16.785  
when it has&nbsp;a different number of turns around the core compared to the primary.

00:02:16.785 --> 00:02:20.844  
But here, there isn’t&nbsp;a secondary winding!

00:02:20.844 --> 00:02:22.781  
It just doesn’t exist.

00:02:22.781 --> 00:02:25.936  
That is, until I put the tube back.

00:02:25.936 --> 00:02:31.415  
This&nbsp;lamp isn’t a literal wire, of course, but once I have it enclosed by the core

00:02:31.415 --> 00:02:38.357  
it&nbsp;does indeed form a loop in the exact same way a single turn secondary winding would.

00:02:38.357 --> 00:02:47.499  
It&nbsp;looks a little strange because it’s going way over there before looping back to the core, but&nbsp;that’s what it is.

00:02:47.499 --> 00:02:53.863  
Now, because this lamp is so large, we need a second core positioned on the other end of the tube,

00:02:53.863 --> 00:02:57.526  
but they’re wired together and so act as one.

00:02:57.526 --> 00:03:03.732  
When the alternating current being sent through the&nbsp;wires by this driver unit induces magnetic fields in the cores,

00:03:03.732 --> 00:03:08.510  
those fields then induce a voltage&nbsp;
inside the fluorescent tube.

00:03:08.510 --> 00:03:15.518  
And, because it’s formed in a loop, that results&nbsp;in current flow which causes the lamp to light.

00:03:15.518 --> 00:03:19.555  
For that reason, this is known as an&nbsp;
induction lamp.

00:03:19.555 --> 00:03:25.477  
The actual light it produces is the result of the exact same&nbsp;principle as an ordinary fluorescent tube:

00:03:25.477 --> 00:03:33.415  
a low-pressure arc discharge is produced by&nbsp;passing current through an ionized mixture of mercury vapor and a noble gas such as argon,

00:03:33.415 --> 00:03:38.279  
and&nbsp;as electrons collide with the mercury atoms the mercury emits ultraviolet light

00:03:38.279 --> 00:03:42.725  
which is then&nbsp;converted to visible light by the phosphors coating the glass.

00:03:42.725 --> 00:03:48.884  
But rather than use electrodes&nbsp;
reaching inside the tube in order to pass current through the gas,

00:03:48.884 --> 00:03:54.080  
current flow is generated&nbsp;
externally via electromagnetic induction.

00:03:54.640 --> 00:03:56.458  
Why would we want that?

00:03:56.458 --> 00:03:59.120  
Well first, it’s&nbsp;pretty cool!

00:03:59.120 --> 00:04:07.920  
But also this particular lamp has a power rating of 200W and a light output in the&nbsp;neighborhood of 16,000 lumens.

00:04:07.920 --> 00:04:15.357  
That is unusually powerful and bright for a fluorescent lamp,&nbsp;
especially given its relatively small size.

00:04:15.357 --> 00:04:22.731  
But brightness, power, and coolness weren’t really the&nbsp;main reasons these appeared - operating life was.

00:04:22.731 --> 00:04:28.185  
Getting rid of the electrodes would mean getting&nbsp;rid of the weak point of the fluorescent lamp.

00:04:28.185 --> 00:04:34.803  
In a conventional tube, the electrodes slowly&nbsp;
wear out in a process known as sputtering.

00:04:34.803 --> 00:04:40.952  
This happens the most at lamp start-up, but sputtering&nbsp;still happens throughout continued operation.

00:04:40.952 --> 00:04:44.696  
Over time this causes the ends of the tube&nbsp;to darken -

00:04:44.696 --> 00:04:53.301  
the dark spots are the material which used to be the electrodes, but as&nbsp;it sputters off it becomes deposited on the glass.

00:04:53.301 --> 00:04:58.962  
That reduces light output&nbsp;slightly 
but the bigger problem is that as they wear away

00:04:58.962 --> 00:05:03.022  
the electrodes lose&nbsp;their ability to emit electrons.

00:05:03.022 --> 00:05:08.794  
That makes it more difficult for the ballast and starter&nbsp;to initiate the arc discharge across the tube,

00:05:08.794 --> 00:05:15.956  
and eventually they will wear to the point&nbsp;the tube is no longer able to start and the lamp has failed.

00:05:15.956 --> 00:05:21.042  
As the technology developed we&nbsp;got pretty good at making electrodes which could last a good while,

00:05:21.042 --> 00:05:26.636  
and fluorescent lamps would&nbsp;
typically have a rated life of 10,000 hours.

00:05:26.636 --> 00:05:33.140  
But if we could do without the electrodes,&nbsp;
the lamp could in theory last forever.

00:05:33.140 --> 00:05:37.380  
And, well, that’s the point of this technology.

00:05:37.380 --> 00:05:42.887  
There’s nothing to the lamp 
but a phosphor-coated tube filled with some argon gas

00:05:42.887 --> 00:05:47.740  
and a pellet of&nbsp;mercury amalgam 
chilling in this little glass appendix.

00:05:47.740 --> 00:05:55.907  
It has no electrodes to wear out and&nbsp;
this means the tube itself has a theoretically unlimited lifespan.

00:05:55.907 --> 00:06:01.412  
Nothing truly lasts forever,&nbsp;of course, 
and due to phosphor wear and mercury absorption

00:06:01.412 --> 00:06:04.281  
these will lose light output over&nbsp;time,

00:06:04.281 --> 00:06:12.375  
but these lamps have a rated lifespan of 
100,000 hours - a tenfold increase over&nbsp;conventional tubes.

00:06:12.375 --> 00:06:20.144  
Operating dusk-to-dawn, that would mean this should last nearly&nbsp;23 years before requiring replacement.

00:06:20.144 --> 00:06:28.847  
Now, obviously, that’s a pretty phenomenal&nbsp;lifespan and so it might be surprising how uncommon this technology is.

00:06:28.847 --> 00:06:32.243  
I mean, there’s not&nbsp;a whole lot to this thing

00:06:32.243 --> 00:06:38.683  
and it operates on the fundamentals of electromagnetism that have been&nbsp;understood since the 19th century.

00:06:38.683 --> 00:06:45.983  
Sure enough, electrodeless lamps which operated via&nbsp;induction had been demonstrated many, many times in the past.

00:06:45.983 --> 00:06:49.297  
Nikola Tesla was&nbsp;playing with it because of course he was.

00:06:49.297 --> 00:06:55.684  
But a practical and effective application&nbsp;of the technology was surprisingly elusive.

00:06:55.684 --> 00:07:01.865  
It wasn’t until 1967 that John Anderson filed&nbsp;a patent for a lamp like this one,

00:07:01.865 --> 00:07:08.967  
and then it took until 1990 for it to actually be commercialized&nbsp;into a finished product.

00:07:08.967 --> 00:07:11.179  
What took so long?

00:07:11.179 --> 00:07:16.174  
Well, despite how simple the overall&nbsp;
idea is on the surface,

00:07:16.174 --> 00:07:23.694  
it turns out there were a LOT of different problems that needed solving&nbsp;before this could actually become a reality.

00:07:23.694 --> 00:07:32.787  
For one thing, inducing current flow in&nbsp;a loop of gas, 
even if it is conductive, is a lot harder than a solid metal wire.

00:07:32.787 --> 00:07:40.757  
To sustain the arc discharge in the tube, the magnetic field generated by the cores has to&nbsp;switch back and forth very a lot,

00:07:40.757 --> 00:07:45.712  
so the frequency at which this thing operates 
needed to be very&nbsp;high.

00:07:45.712 --> 00:07:50.788  
You’ll notice the patent 
shows the driver as “converter to radio frequency”

00:07:50.788 --> 00:07:56.132  
and Anderson&nbsp;lists a preferred 
frequency range of 100 to 500 kilocycles.

00:07:56.132 --> 00:08:00.257  
That’s almost reaching the AM radio&nbsp;broadcast band.

00:08:00.257 --> 00:08:06.901  
By 1967 it was relatively trivial to produce high-powered oscillators which ran at&nbsp;that frequency,

00:08:06.901 --> 00:08:09.395  
but that wasn’t the main issue.

00:08:09.395 --> 00:08:12.032  
Because of the required high frequency,

00:08:12.032 --> 00:08:19.486  
wrapping wire&nbsp;around an ordinary iron core 
as found in most power transformers wasn’t feasible.

00:08:19.486 --> 00:08:26.512  
At those&nbsp;frequencies, the eddy currents which form inside the cores would cause it to get extremely hot.

00:08:26.512 --> 00:08:30.272  
That’s the mechanism by which induction cooktops work.

00:08:30.272 --> 00:08:34.853  
But the problem is, that would both limit&nbsp;
the efficiency of the power coupling

00:08:34.853 --> 00:08:41.932  
and how much power you could feasibly transfer into the tube&nbsp;before the cores started to melt.

00:08:41.932 --> 00:08:48.323  
This meant ferrite compounds, which are extremely magnetically&nbsp;permeable but not electrically conductive

00:08:48.323 --> 00:08:51.656  
and therefore don’t form eddy currents inside,

00:08:51.656 --> 00:08:55.538  
were required&nbsp;for high-frequency power coupling.

00:08:55.538 --> 00:09:03.042  
They weren’t invented until the 1930’s and even though they&nbsp;were fairly common by the time Anderson filed his patent,

00:09:03.042 --> 00:09:05.953  
ferrite was still an expensive material.

00:09:05.953 --> 00:09:11.260  
In fact, that’s the main reason this lamp gets narrower where the cores attach:

00:09:11.260 --> 00:09:16.106  
making the tube diameter&nbsp;
smaller requires less material in the cores.

00:09:16.106 --> 00:09:19.211  
But here’s where the story gets a&nbsp;little weird.

00:09:19.211 --> 00:09:25.860  
Although this patent is nearly a spot-on description of&nbsp;
this lamp both in form and function,

00:09:25.860 --> 00:09:30.960  
the first commercial products using the&nbsp;technology were very different from this.

00:09:31.520 --> 00:09:37.291  
The QL line from Philips was the first 
commercial&nbsp;induction lamp and they looked…

00:09:37.291 --> 00:09:41.025  
pretty much like an ordinary incandescent light bulb.

00:09:41.025 --> 00:09:46.701  
They&nbsp;weren’t - they were in fact fluorescent lamps which worked by induction similar to this.

00:09:46.701 --> 00:09:53.923  
But compared to this tube and its external cores, 
they were constructed inside-out.

00:09:53.923 --> 00:10:00.182  
I don’t have&nbsp;one to show you, but thanks to a donation 
to the channel from Jeff, a long-time Patreon&nbsp;member,

00:10:00.182 --> 00:10:05.561  
I do have this variation which was manufactured by GE.

00:10:05.561 --> 00:10:12.418  
This Genura lamp was released&nbsp;in 1994 
and it is designed to replace a reflector flood bulb

00:10:12.418 --> 00:10:17.465  
but it works on the same basic&nbsp;principle to the original Philips QL lamps.

00:10:17.465 --> 00:10:21.794  
Here, the discharge tube isn’t so much a&nbsp;tube as it is...

00:10:21.794 --> 00:10:23.577  
a vessel.

00:10:23.577 --> 00:10:28.823  
And a single coil, once again in the form of a wire wrapped around a&nbsp;
ferrite core,

00:10:28.823 --> 00:10:35.162  
protrudes from the base of the lamp into a hollowed-out section of the glass vessel.

00:10:35.162 --> 00:10:41.071  
This evacuation stem holds the pellet of mercury amalgam which is required to produce ultraviolet&nbsp;light

00:10:41.071 --> 00:10:45.178  
and it rests inside the ferrite core when assembled.

00:10:45.178 --> 00:10:51.399  
An oscillator circuit in the base&nbsp;of the bulb sends high-frequency pulses through the wire wrapped around the ferrite core

00:10:51.399 --> 00:10:56.310  
which in&nbsp;turn creates a rapidly fluctuating magnetic field around it.

00:10:56.310 --> 00:11:00.976  
That field reaches well inside the discharge&nbsp;vessel.

00:11:00.976 --> 00:11:06.086  
As the field changes in intensity, current flows through the gas inside,

00:11:06.086 --> 00:11:09.681  
and our desired mercury discharge occurs.

00:11:09.681 --> 00:11:18.552  
In this lamp design, the single coil protruding&nbsp;into the vessel produces a magnetic field in a toroidal shape around its perimeter.

00:11:18.552 --> 00:11:23.302  
That’s why&nbsp;the QL lamps from Philips look a lot like an ordinary light bulb.

00:11:23.302 --> 00:11:31.855  
It’s not a linear discharge&nbsp;running through a tube but more of a fuzzy donut of ultraviolet light surrounding the induction&nbsp;coil,

00:11:31.855 --> 00:11:35.933  
which a bulb-shape happens to encapsulate quite well.

00:11:35.933 --> 00:11:39.626  
The phosphors on the glass convert the&nbsp;UV to visible light

00:11:39.626 --> 00:11:45.946  
and the result is a compact yet very bright light source with an extremely&nbsp;long life.

00:11:45.946 --> 00:11:52.875  
The original QL lamps ran 
at 85 watts and had a rated life of 100,000 hours.

00:11:52.875 --> 00:12:02.640  
Now,&nbsp;this GE lamp isn’t quite so optimistic but that’s likely down to the fact that its drive&nbsp;electronics are built into the lamp itself.

00:12:02.720 --> 00:12:05.842  
This was sold as a drop-in replacement light&nbsp;bulb,

00:12:05.842 --> 00:12:09.067  
so everything had to get crammed into here.

00:12:09.067 --> 00:12:12.686  
And since these are generally&nbsp;
operated with the base facing up,

00:12:12.686 --> 00:12:17.138  
heat from the discharge 
would rise right&nbsp;into the electronic components

00:12:17.138 --> 00:12:21.070  
which shortens their operating life, especially&nbsp;capacitors.

00:12:21.070 --> 00:12:25.827  
The QL line from Philips used an external driver muck like this thing does

00:12:25.827 --> 00:12:29.840  
and the lamp itself was&nbsp;little more than a glass orb on a stick.

00:12:30.400 --> 00:12:33.671  
Still, it wasn't quite as simple as it looks.

00:12:33.671 --> 00:12:39.243  
Because the induction coil was shoved up the middle of the lamp, it gets pretty hot -

00:12:39.243 --> 00:12:45.107  
particularly&nbsp;in the case of the QL lamps which operated at 85 watts.

00:12:45.107 --> 00:12:49.607  
This was a problem because as the&nbsp;
ferrite material increases in temperature,

00:12:49.607 --> 00:12:55.671  
its magnetic permeability decreases which&nbsp;
limited the strength of the magnetic fields it can produce

00:12:55.671 --> 00:12:59.699  
and thus the amount of&nbsp;power it can send into the gas discharge.

00:12:59.699 --> 00:13:04.124  
That reduces both brightness and energy&nbsp;efficiency.

00:13:04.124 --> 00:13:10.544  
Philips solved this by incorporating 
heat-conducting material into the design of&nbsp;the ferrite core’s stem,

00:13:10.544 --> 00:13:14.419  
which by the way they referred to as the antenna.

00:13:14.419 --> 00:13:19.588  
From what I can tell&nbsp;looking at patents, GE didn’t solve this at all,

00:13:19.588 --> 00:13:26.160  
but since the lamp only operates at 23 watts&nbsp;
the induction coil probably never got hot enough to matter.

00:13:26.468 --> 00:13:33.120  
But another issue with the single-coil designs is that&nbsp;
it require an even higher frequency to function:&nbsp;&nbsp;

00:13:33.120 --> 00:13:36.154  
around 2.5 megahertz.

00:13:36.154 --> 00:13:43.622  
And because these are&nbsp;operating at radio frequencies and pumping dozens of watts or more into the discharge vessel,

00:13:43.622 --> 00:13:47.779  
well radio&nbsp;frequency interference was a significant problem.

00:13:47.779 --> 00:13:55.115  
To try and help solve it, the glass is coated with a 
transparent yet&nbsp;conductive material, such as indium tin oxide,

00:13:55.115 --> 00:13:58.896  
which absorbs radio frequency energy and&nbsp;
keeps it from escaping.

00:13:58.896 --> 00:14:07.279  
And in this lamp, the underside of the discharge vessel also has a metal shield which was&nbsp;bonded to this copper ribbon

00:14:07.279 --> 00:14:11.048  
that allows the absorbed energy to return to the circuit ground.

00:14:11.048 --> 00:14:17.521  
But, it’s clear that GE at least 
wasn’t making the strongest promises about its effectiveness.

00:14:17.521 --> 00:14:24.399  
They warn specifically against using these on boats 
as they could disrupt maritime communications.

00:14:24.399 --> 00:14:28.927  
And, uh,&nbsp;given that they provided a phone number for interference complaints...

00:14:28.927 --> 00:14:32.696  
well I think it’s&nbsp;safe to say this was very much a beta test.

00:14:32.696 --> 00:14:39.960  
Now, it might seem a little odd that&nbsp;
the basic idea for this later design was patented in 1967

00:14:39.960 --> 00:14:47.930  
yet induction lighting didn’t get&nbsp;commercialized 
until after Philips and GE released their single-coil designs.

00:14:47.930 --> 00:14:53.176  
But it&nbsp;might make more sense if you consider that these external-coil lamps...

00:14:53.176 --> 00:14:56.782  
really aren't that&nbsp;different from conventional fluorescent tubes.

00:14:56.782 --> 00:15:06.714  
In fact, many lower-power versions of this design&nbsp;incorporated circular tubes which look a whole awful lot like a standard circular fluorescent&nbsp;lamp.

00:15:06.714 --> 00:15:13.133  
They did offer higher light outputs, but the form was still very familiar.

00:15:13.133 --> 00:15:23.591  
The fact that&nbsp;neither the QL lamp nor this Genura lamp look anything like a fluorescent tube is probably why&nbsp;the technology was first commercialized like this.

00:15:23.591 --> 00:15:25.783  
Consider the GE bulb:

00:15:25.783 --> 00:15:36.258  
the resulting discharge&nbsp;inside this vessel produces a compact but powerful 
ring of UV light just under a relatively&nbsp;flat piece of glass.

00:15:36.258 --> 00:15:41.462  
This meant fluorescent technology could not only 
mimic the appearance&nbsp;of an incandescent reflector

00:15:41.462 --> 00:15:49.040  
much more faithfully than sticking a coiled tube inside a&nbsp;
fake bulb but it was also much more effective.

00:15:49.600 --> 00:15:58.840  
This flavor of induction technology was able to&nbsp;create much more powerful 
yet also compact light&nbsp;sources than a linear fluorescent tube

00:15:58.840 --> 00:16:02.715  
while&nbsp;still offering similar energy-efficiency.

00:16:02.715 --> 00:16:07.771  
That was compelling enough on its own to&nbsp;
pursue not only for aesthetic purposes

00:16:07.771 --> 00:16:14.335  
but because it allowed the use of fixtures&nbsp;with 
optical systems that produced much more directional light.

00:16:15.405 --> 00:16:18.480  
To a point at&nbsp;least - I’ll touch on that more in a bit.

00:16:19.040 --> 00:16:23.680  
Induction technology also solved one of&nbsp;
fluorescent lighting’s little annoyances:

00:16:23.680 --> 00:16:25.576  
a slow warm-up.

00:16:25.576 --> 00:16:31.388  
High-efficiency fluorescent&nbsp;tubes in particular 
only produce a fraction of their light output at first

00:16:31.388 --> 00:16:37.479  
due to lower vapor pressure&nbsp;when cold 
and thus they can take several minutes to warm up.

00:16:37.479 --> 00:16:42.475  
This lamp also starts with a lower&nbsp;
vapor pressure and thus reduced light output,

00:16:42.475 --> 00:16:45.429  
but the warmup time is just a few seconds.

00:16:45.429 --> 00:16:52.135  
And the large external-coil lamp is similarly quick - 
it’s at full brightness in only&nbsp;10 seconds.

00:16:52.135 --> 00:16:59.841  
You can actually observe the mercury discharge migrating away 
from the amalgam&nbsp;pellet as the tube heats up and the pressure builds.

00:16:59.841 --> 00:17:03.153  
But… well, that was at room temperature,

00:17:03.153 --> 00:17:06.176  
and these lamps were sold to go outdoors.

00:17:06.176 --> 00:17:11.714  
In fact street lighting is one of the most likely&nbsp;
places you’re going to find these in the wild.

00:17:11.714 --> 00:17:15.818  
And I live where the outside air sometimes&nbsp;gets colder than a freezer,

00:17:15.818 --> 00:17:22.620  
so I put this whole thing inside a freezer overnight
 to see&nbsp;how quickly it would warm up from truly cold.

00:17:22.620 --> 00:17:28.258  
The lamp had no issues starting but, 
like&nbsp;most fluorescent lights in this temperature,

00:17:28.258 --> 00:17:35.455  
the mercury was barely contributing anything 
and we could&nbsp;see the purple glow of the argon starter gas.

00:17:35.455 --> 00:17:41.566  
Interestingly it initially did the same thing&nbsp;
where the light output seems to grow from the mercury pellet,

00:17:41.566 --> 00:17:48.170  
but before long that bright spot&nbsp;disappeared and it all averaged out to a very dull grey.

00:17:48.170 --> 00:17:55.880  
It took about 10 minutes to attain&nbsp;full brightness 
so it looks like cold-weather performance is only improved slightly.

00:17:55.880 --> 00:17:58.743  
But at least it had no trouble starting!

00:17:58.743 --> 00:18:03.609  
Speaking of starting, well now it’s time to&nbsp;come clean here -

00:18:03.609 --> 00:18:08.578  
I don’t really understand the mechanisms by which these lamps start.

00:18:08.578 --> 00:18:14.939  
See, the gas mixture in these tubes isn’t electrically conductive until it’s ionized.

00:18:14.939 --> 00:18:23.437  
The&nbsp;electrodes in a traditional fluorescent tube emit electrons when heated 
and/or when a sufficiently&nbsp;high voltage is placed across them,

00:18:23.437 --> 00:18:30.960  
and those electrons collide with the gas molecules inside&nbsp;
and ionize them which causes dielectric breakdown.

00:18:31.520 --> 00:18:36.139  
But with these, all we got is magnets.

00:18:36.139 --> 00:18:44.519  
The 1967 patent mentions the use of electrodes in contact with the glass that, 
when a sufficiently&nbsp;high voltage is placed across them,

00:18:44.519 --> 00:18:49.560  
will ionize enough gas inside the tube to initiate dielectric&nbsp;breakdown.

00:18:49.560 --> 00:18:53.564  
But this device has no such electrodes.

00:18:53.564 --> 00:18:59.902  
A later patent filed in 1995 describes this device&nbsp;nearly perfectly,

00:18:59.902 --> 00:19:08.159  
and it even has a diagram which more clearly illustrates the 
rather confusing&nbsp;way the wires are wrapped around the two ferrite cores.

00:19:08.159 --> 00:19:17.441  
But it also mentions a conductive strip&nbsp;in contact with the glass 
specifically for the purpose of creating ionization points for&nbsp;starting the lamp.

00:19:18.708 --> 00:19:22.103  
But again, this lamp doesn’t have those.

00:19:22.103 --> 00:19:28.389  
All the information I could find on&nbsp;how this lamp gets started was quite handwavey,

00:19:28.389 --> 00:19:36.264  
but my best understanding is that the driver&nbsp;circuitry 
initially sends a much higher than usual voltage through the wires

00:19:36.264 --> 00:19:43.093  
which produces a strong&nbsp;enough electric field 
that free electrons in the gas mixture are sort of thrown about,

00:19:43.093 --> 00:19:45.278  
causing&nbsp;some ionization.

00:19:45.278 --> 00:19:51.180  
Basically it’s the same way that fluorescent tubes 
can start glowing when you hold them near a Tesla&nbsp;coil.

00:19:51.180 --> 00:19:56.198  
And once some of that gas is ionized 
the discharge across the tube can be completed

00:19:56.198 --> 00:20:00.051  
after which the driver can switch to its normal operating voltage.

00:20:00.051 --> 00:20:05.882  
That may also further explain why the internal&nbsp;core lamps were commercialized first.

00:20:05.882 --> 00:20:12.341  
Based on readings of patents, it was initially thought&nbsp;
that a secondary winding would be needed on the ferrite core

00:20:12.341 --> 00:20:16.826  
to produce a high voltage capable of initiating a glow&nbsp;discharge,

00:20:16.826 --> 00:20:23.981  
but that feature seems to have gone away 
once it was decided to use the very&nbsp;high frequency found here.

00:20:23.981 --> 00:20:31.787  
This patent filed in 1982 seems to suggest that simply by inducing&nbsp;the magnetic field at a frequency of 3 megahertz,

00:20:31.787 --> 00:20:37.869  
a sufficiently strong electric field is produced&nbsp;
inside the vessel which can ionize the gas.

00:20:37.869 --> 00:20:43.280  
But I still haven’t gotten a truly satisfactory answer,&nbsp;
here, and would welcome one in the comments!

00:20:43.840 --> 00:20:47.683  
It might have something to do with the metal&nbsp;
mesh found here,

00:20:47.683 --> 00:20:55.298  
and a closer look up the middle of this Genura’s discharge vessel 
shows a&nbsp;piece of wire at the top of the evacuation stem.

00:20:55.298 --> 00:20:58.764  
But truthfully, I gave up trying to find an answer.

00:20:59.266 --> 00:21:07.025  
So, with their extremely long operating life&nbsp;
and newfound applications for energy-efficient&nbsp;fluorescent lighting,

00:21:07.025 --> 00:21:10.961  
it might seem strange&nbsp;that this technology is so obscure.

00:21:10.961 --> 00:21:15.209  
I mean, today we have LEDs and this technology is&nbsp;obsolete

00:21:15.209 --> 00:21:24.140  
but knowing that back in 1990 we had a lighting technology 
with a lifespan that&nbsp;essentially matches the best LEDs we have today,

00:21:24.140 --> 00:21:27.906  
you would think it would have&nbsp;taken the world by storm.

00:21:27.906 --> 00:21:29.215  
Yet it didn’t.

00:21:29.863 --> 00:21:30.926  
Why?

00:21:30.926 --> 00:21:34.411  
Was there another one&nbsp;of those light bulb conspiracies afoot?

00:21:34.411 --> 00:21:35.966  
Yeah, no.

00:21:35.966 --> 00:21:42.319  
See, here’s the thing - the tech is&nbsp;really cool and opens up some new possibilities,

00:21:42.319 --> 00:21:47.317  
but not that many and it also came with some&nbsp;significant downsides.

00:21:47.317 --> 00:21:49.866  
For one, cost.

00:21:49.866 --> 00:21:58.372  
The QL line of lighting from Philips was very much a&nbsp;specialized 
commercial product and I’ve been having a heck of a time finding original pricing,

00:21:58.372 --> 00:22:01.157  
but you can bet it was quite high.

00:22:01.157 --> 00:22:04.509  
Not only had they created a new kind of fluorescent lamp,

00:22:04.509 --> 00:22:09.853  
but&nbsp;they had to manufacture specialized electronics and the power couplers.

00:22:09.853 --> 00:22:15.428  
The lighting system really&nbsp;only made sense in 
applications where relamping was an operational headache

00:22:15.428 --> 00:22:18.904  
or its operating&nbsp;method offered improved safety -

00:22:18.904 --> 00:22:26.237  
apparently they saw success in the oil and gas industry 
due&nbsp;to regulations concerning explosion-proof lighting.

00:22:26.237 --> 00:22:31.077  
GE’s take on the technology was sort-of&nbsp;consumer focused,

00:22:31.077 --> 00:22:38.697  
and the Genura bulb retailed for about $30 in 1994, equivalent to&nbsp;$65 today.

00:22:38.697 --> 00:22:44.902  
But that’s a pricey light bulb 
especially considering its expected life&nbsp;isn’t all that great.

00:22:44.902 --> 00:22:50.829  
It’s certainly much better than the 1 or 2,000 hours 
you could&nbsp;expect out of an incandescent flood bulb,

00:22:50.829 --> 00:22:55.619  
but it was barely an improvement over existing&nbsp;fluorescent technology.

00:22:55.619 --> 00:23:01.764  
You needed to really, really want fluorescent lighting in this specific&nbsp;form-factor,

00:23:01.764 --> 00:23:09.820  
and I find it interesting that GE really didn’t bother to explain 
what’s so cool&nbsp;about this technology on the box.

00:23:09.820 --> 00:23:13.934  
They're just calling this an electronic compact fluorescent lamp.

00:23:13.934 --> 00:23:18.399  
Which is true but certainly underselling it.

00:23:18.399 --> 00:23:25.039  
But the biggest issue, and what I think is likely&nbsp;
the main reason this technology never took the world by storm,

00:23:25.039 --> 00:23:29.345  
is that it’s still fundamentally&nbsp;fluorescent lighting.

00:23:29.345 --> 00:23:34.997  
Yes it was longer-lived, but it still had kinda meh light quality.

00:23:34.997 --> 00:23:39.715  
And,&nbsp;because fluorescent lights are very much not point-sources of light,

00:23:39.715 --> 00:23:42.925  
it was hard to direct&nbsp;the light these emitted.

00:23:42.925 --> 00:23:46.876  
This 200W lamp was originally housed in this flood fixture,

00:23:46.876 --> 00:23:53.882  
and while you could point this in a direction, it still casts a very wide beam of light.

00:23:53.882 --> 00:23:57.512  
I don’t&nbsp;even think you could describe it as a beam.

00:23:57.512 --> 00:24:04.945  
The QL lamps were more compact, 
but they still emitted&nbsp;diffused light which is difficult to control.

00:24:05.040 --> 00:24:07.527  
Take street lighting as an example.

00:24:07.527 --> 00:24:10.961  
I've&nbsp;encountered a few induction street lamps in the wild,

00:24:10.961 --> 00:24:17.827  
but they all have about as much beam&nbsp;control as a circline
 fluorescent light stuck in the middle of the kitchen ceiling.

00:24:17.827 --> 00:24:20.134  
Because that’s&nbsp;pretty much what they are.

00:24:20.134 --> 00:24:28.632  
And the inverse square law means that you can’t place the lamps too&nbsp;high 
above the street or they just won’t offer effective light output.

00:24:28.632 --> 00:24:33.528  
This ultimately means you&nbsp;need many more of them placed closer together.

00:24:33.528 --> 00:24:40.980  
High-intensity discharge lamps like high pressure&nbsp;
sodium and metal halide produce all their light in a small arc tube

00:24:40.980 --> 00:24:46.792  
which allows fixtures&nbsp;with optical systems 
to focus the light they produce into a narrow beam,

00:24:46.792 --> 00:24:51.715  
permitting the use of&nbsp;fewer fixtures by placing them higher in the air.

00:24:51.715 --> 00:24:56.457  
And actually, the Genura lamp demonstrates&nbsp;this downside quite well.

00:24:56.457 --> 00:25:02.360  
While it mimics the basic appearance of an incandescent BR flood very&nbsp;faithfully...

00:25:02.360 --> 00:25:03.978  
at least from the face of it,

00:25:03.978 --> 00:25:08.241  
there’s no directionality to the light it produces.

00:25:08.241 --> 00:25:16.654  
Even a&nbsp;frosted lamp like this produces a somewhat narrow beam of light 
thanks to fact that the filament is placed far down the reflector

00:25:16.654 --> 00:25:22.642  
and that is very important to both the 
character and effectiveness of the light it produces,

00:25:22.642 --> 00:25:25.920  
especially when recessed in ceiling can fixtures.

00:25:26.560 --> 00:25:30.103  
This lamp simply cannot recreate&nbsp;that directional light,

00:25:30.103 --> 00:25:36.817  
and I would imagine that presented problems from both an&nbsp;
aesthetic perspective and a functional one,&nbsp;too.

00:25:36.817 --> 00:25:43.455  
It may be the same number of lumens,&nbsp;
but when fired in all directions and not mostly downward,

00:25:43.455 --> 00:25:46.897  
the room might&nbsp;be underlit compared to before.

00:25:46.897 --> 00:25:52.781  
And let’s not forget that 
conventional fluorescent&nbsp;technology saw lots of innovation, too.

00:25:52.781 --> 00:26:01.329  
If any of the lighting nerds out there have been&nbsp;wondering why I never touted the flicker-free light output created by the high-frequency drivers&nbsp;in these things,

00:26:01.329 --> 00:26:06.913  
that’s because electronic ballasts for traditional tubes did the same thing.

00:26:06.913 --> 00:26:09.991  
They&nbsp;didn’t operate anywhere near these frequencies,

00:26:09.991 --> 00:26:16.494  
but they were fast enough for the persistence&nbsp;
of the phosphors to produce truly continuous light output.

00:26:16.494 --> 00:26:20.730  
That also increased the&nbsp;energy-efficiency of fluorescent lighting.

00:26:20.730 --> 00:26:28.119  
As a matter of fact, a bog-standard T8 tube is&nbsp;
more energy-efficient than either of these induction lamps.

00:26:28.119 --> 00:26:30.370  
And then of course there’s the CFL.

00:26:30.370 --> 00:26:34.088  
Those, too, got&nbsp;electronic ballasts and all the benefits thereof

00:26:34.088 --> 00:26:39.605  
and they were available in much more modest&nbsp;
power outputs than induction lamps.

00:26:39.605 --> 00:26:44.994  
Sure, the Genura lamp is a more elegant solution&nbsp;
than sticking a coil in a fake bulb,

00:26:44.994 --> 00:26:49.983  
but… is its elegance worth the extra cost?

00:26:49.983 --> 00:26:53.616  
The&nbsp;market clearly decided no it wasn’t.

00:26:53.616 --> 00:26:59.795  
I mean, this lamp was sold long before the old curly-q&nbsp;CFL went mainstream.

00:26:59.795 --> 00:27:07.189  
Once we figured out how to make those cheaply, 
small induction lamps&nbsp;like this just hardly made any sense at all.

00:27:07.189 --> 00:27:11.925  
And when ordinary fluorescent lights already had a&nbsp;10,000 hour lifespan,

00:27:11.925 --> 00:27:18.880  
well frankly you just had to be extremely committed to the idea of a lamp&nbsp;which could last 20 years without being touched.

00:27:19.534 --> 00:27:22.826  
That is, if it makes it that long.

00:27:22.826 --> 00:27:29.993  
The&nbsp;weak point in the induction lamp 
isn't the discharge tube, it's the electronics inside this box.

00:27:29.993 --> 00:27:35.812  
And while it certainly is possible to produce
electronic circuitry which lasts&nbsp;100,000 hours,

00:27:35.812 --> 00:27:39.354  
well let’s just say there are never any guarantees.

00:27:39.354 --> 00:27:44.366  
Honestly props to&nbsp;GE for being so realistic with these lamps.

00:27:44.366 --> 00:27:49.831  
The QL line from Philips probably had the best&nbsp;
quality drivers of any commercial system

00:27:49.831 --> 00:27:53.791  
and since they were separated from the lamp they didn’t have&nbsp;
to deal with heat.

00:27:53.791 --> 00:28:02.070  
But had this tech gone mainstream, we’d no doubt have the same race to&nbsp;the bottom that plagues so many things.

00:28:02.070 --> 00:28:04.970  
But of course now this is all moot.

00:28:04.970 --> 00:28:13.360  
The&nbsp;LED has trounced every lighting technology 
that we’ve ever made on energy efficiency,&nbsp;quality of light, and flexibility.

00:28:14.240 --> 00:28:18.173  
We still have the same race-to-the-bottom nonsense&nbsp;going on, unfortunately,

00:28:18.173 --> 00:28:25.108  
and it’s not like there haven’t been some high-profile 
issues with LEDs (such as purple&nbsp;streetlights)

00:28:25.108 --> 00:28:29.450  
but in general lighting is now just solved.

00:28:29.450 --> 00:28:30.889  
We’re there.

00:28:30.889 --> 00:28:34.763  
Aside from some cheap&nbsp;builder-grade light bulbs I still have kicking around,

00:28:34.763 --> 00:28:39.745  
I personally haven’t needed to replace a light&nbsp;bulb in several years.

00:28:39.745 --> 00:28:44.122  
That’s no doubt helped by the fact that I 
generally only buy high-quality&nbsp;bulbs

00:28:44.122 --> 00:28:49.840  
and I use dimmers nearly everywhere 
so rarely are any of my lights at full-brightness,

00:28:49.840 --> 00:28:50.654  
but yeah.

00:28:50.654 --> 00:28:53.935  
I’m certainly not pining for the days of old.

00:28:53.935 --> 00:28:59.246  
But luckily our path to get here was&nbsp;
filled with all sorts of wacky nonsense like this.

00:29:00.260 --> 00:29:02.855  
♫ electromagnetically smooth jazz ♫

00:29:03.728 --> 00:29:05.859  
And because it’s formed in a loop,

00:29:05.859 --> 00:29:12.036  
that&nbsp;induced voltage results in current flow which causes the lamp to light.

00:29:12.036 --> 00:29:13.416  
Except it&nbsp;didn’t.

00:29:14.571 --> 00:29:19.596  
Probably because… you need to be secured in place.

00:29:19.596 --> 00:29:22.982  
Hopefully I didn’t just&nbsp;kill ya, that would be very problematic.

00:29:22.982 --> 00:29:25.683  
For that reason, this is known as&nbsp;an induction lamp.

00:29:25.683 --> 00:29:28.867  
And I cannot be sitting here with this in front of my eyes.

00:29:28.867 --> 00:29:30.887  
…chilling in this little glass appendage.

00:29:30.887 --> 00:29:33.247  
Is that the right one? Nope. I pointed at the wrong one.

00:29:33.247 --> 00:29:36.926  
I mean, there’s not a not… not a… dada da!

00:29:37.520 --> 00:29:43.040  
And in this lamp, [glass scraping sounds] 
the&nbsp;underside… that I’m sure sounded horrible.&nbsp;

00:29:43.040 --> 00:29:46.394  
…have been demonstrated many many&nbsp;times over the past.

00:29:46.394 --> 00:29:48.285  
In the… in… ugh.

00:29:50.000 --> 00:29:52.499  
One would have to call this technology...

00:29:52.499 --> 00:29:55.307  
totally tubular, amirite?

00:29:55.730 --> 00:29:57.309  
That one hurt to the core.

00:29:58.126 --> 00:29:59.175  
Both of them, actually.

00:29:59.175 --> 00:30:03.046  
Hey did you know that Michael used to be a taxi driver?

00:30:03.046 --> 00:30:05.403  
He switched to a career in science since he only got one fare a day.

