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Internet FOCUS ON MYSPACE in Malaysiakini

Internet users who upload video pirated from the television may no longer find the clips being taken down or find themselves in trouble. Instead they may become an important part in helping broadcasters make money from the web.

MySpace, the social networking site owned by Rupert Murdoch’s News Corporation, says it will start using new technology that will identified pirated material and insert an advert along the bottom of the video.

The sale of that advert will generate revenue that is then shared between MySpace and the TV company that created the clip.

“This is a game-changer,” said Jeff Berman, president of sales and marketing at MySpace. “We’re going from a world of no to a world of yes while protecting the rights of the copyright holder.”

MySpace is using a digital fingerprinting technology created by Auditude, a company led by a former MTV executive, and will trial it first in partnership with MTV’s parent company, Viacom. Auditude is able to index and scan hours of TV and online footage in a split second, and will be searching for clips from popular Viacom shows such as Comedy Central’s The Daily Show with Jon Stewart and MTV’s Punk’d.

Clips from Viacom shows, many of which are popular among young viewers, have been among those most often pirated and uploaded by the mainly young users of social networking and video sharing sites – much to the fury of Viacom.

The company is currently pursuing a $1bn lawsuit against Google’s YouTube over what it says are millions of incidences of copyright infringement by users who uploaded clips of its shows to the video sharing website. It has held out against revenue sharing deals that other broadcasters have signed with YouTube, saying the site does not do enough to identify and take down copyrighted material. YouTube says it has implemented video identification technology similar to Auditude’s.

Mika Salmi, president of global digital media at MTV Networks, lavished praise on what he said is News Corp’s more accommodating attitude.

“This deal with MySpace is quite different,” he said. “MySpace has always respected copyright and is more progressive about copyright in our mind. The way we’re pushing this out with Auditude and MySpace is different than with YouTube or our past associations there.”

News Corp is also a major broadcaster and producer in its own right, owning the Fox television network that makes The Simpsons, Family Guy and American Idol.

The ads served through Auditude are called “attribution overlay,” a semitransparent strip that covers the lower third of the video player. Although the exact formatting of the overlay will vary as the companies experiment, it will identify the channel that provides the program as well as links to either see a full-length episode or purchase a download. In addition, the overlay can convey a separate brand message from an advertiser that could trigger a second video within the player.

Ultraviolet ANSWER

Ultraviolet (UV) light has shorter wavelengths than visible light. Though these waves are invisible to the human eye, some insects, like bumblebees, can see them! (Image of the bumblebee is courtesty of Mark Cassino.)     An image of a bumblebee.

Scientists have divided the ultraviolet part of the spectrum into three regions: the near ultraviolet, the far ultraviolet, and the extreme ultraviolet. The three regions are distinguished by how energetic the ultraviolet radiation is, and by the “wavelength” of the ultraviolet light, which is related to energy.

The near ultraviolet, abbreviated NUV, is the light closest to optical or visible light. The extreme ultraviolet, abbreviated EUV, is the ultraviolet light closest to X-rays, and is the most energetic of the three types. The far ultraviolet, abbreviated FUV, lies between the near and extreme ultraviolet regions. It is the least explored of the three regions.

The Extreme Ultraviolet Sun.     Our Sun emits light at all the different wavelengths in electromagnetic spectrum, but it is ultraviolet waves that are responsible for causing our sunburns. To the left is an image of the Sun taken at an Extreme Ultraviolet wavelength - 171 Angstroms to be exact. (An Angstrom is a unit length equal to 10-10 meters.) This image was taken by a satellite named SOHO and it shows what the Sun looked like on April 24, 2000.

Though some ultraviolet waves from the Sun penetrate Earth’s atmosphere, most of them are blocked from entering by various gases like Ozone. Some days, more ultraviolet waves get through our atmosphere. Scientists have developed a UV index to help people protect themselves from these harmful ultraviolet waves.

How do we “see” using Ultraviolet light?

It is good for humans that we are protected from getting too much ultraviolet radiation, but it is bad for scientists! Astronomers have to put ultraviolet telescopes on satellites to measure the ultraviolet light from stars and galaxies - and even closer things like the Sun!

There are many different satellites that help us study ultraviolet astronomy. Many of them only detect a small portion of UV light. For example, the Hubble Space Telescope observes stars and galaxies mostly in near ultraviolet light. NASA’s Extreme Ultraviolet Explorer satellite is currently exploring the extreme ultraviolet universe. The International Ultraviolet Explorer (IUE) satellite has observed in the far and near ultraviolet regions for over 17 years.     The International Ultraviolet Explorer

What does Ultraviolet light show us?

We can study stars and galaxies by studying the UV light they give off - but did you know we can even study the Earth? Below is an unusual image - it is a picture of Earth taken from a lunar observatory! This false-color picture shows how the Earth glows in ultraviolet (UV) light.

The Far UV Camera/Spectrograph deployed and left on the Moon by the crew of Apollo 16 took this picture. The part of the Earth facing the Sun reflects much UV light. Even more interesting is the side facing away from the Sun. Here, bands of UV emission are also apparent. These bands are the result of aurora caused by charged particles given off by the Sun. They spiral towards the Earth along Earth’s magnetic field lines.     The UV Earth D

Many scientists are interested in studying the invisible universe of ultraviolet light, since the hottest and the most active objects in the cosmos give off large amounts of ultraviolet energy.

The image below shows three different galaxies taken in visible light (bottom three images) and ultraviolet light (top row) taken by NASA’s Ultraviolet Imaging Telescope (UIT) on the Astro-2 mission.

UV and Visible images of 3 galaxiesD

The difference in how the galaxies appear is due to which type of stars shine brightest in the optical and ultraviolet wavelengths. Pictures of galaxies like the ones below show mainly clouds of gas containing newly formed stars many times more massive than the sun, which glow strongly in ultraviolet light. In contrast, visible light pictures of galaxies show mostly the yellow and red light of older stars. By comparing these types of data, astronomers can learn about the structure and evolution of galaxies.

The story about Subsidy

A man called Razak owns a farm which can produce 10 apples every day.
He has 5 workers to operate the farm.
Each of them eats 1 apple daily and it is enough to keep them operating the farm normally.
The remaining 4 apples, the landlord sells them at RM10 each and he earns RM40.
He uses the RM25 to improve the farm operation and facilities.
He gives RM2.00 to each of his workers and he keeps the remaining RM5.00 as profit.
Day by day, the farm is well developed and all of the 5 workers are happy with the money they can save.

When Razak passed away and there is a new landlord, PokLeh comes to continue the farm operation.
He says to the workers: “We need to improve the farm quality and redefine our way of thinking.
>From now on all of you only need to pay RM1.00 for each apple you eat.
It is very cheap as the price is RM10 each outside the farm.”

The workers have no choice but to pay RM1.00 for the apple they eat daily.
Their earning decrease from RM2.00 to RM1.00 per person.
As usual, PokLeh sells the 4 apples and he gets RM40.
He uses RM25 for farm improvement and pays RM10 to his 5 workers.
He gets RM5.00 as profit. On top of that, he gets another RM5.00 from the apples that he sells to his workers.
In total, he gets RM10 as profit every day.

Soon, the apple price increases to RM20 each.
The new landlord gets a higher profit as he gets RM80 for the 4 apples he sells daily.
Then, he decides to give the farming improvement contract to one of his close friend, Samy..
Samy says:”Apple cost naik, improvement cost also misti naik.”
So, the farm improvement cost increases from RM25 to RM50.
In actual, the improvement only cost RM30.
The remaining RM20, PokLeh and Samy share evenly among themselves.

Let’s calculate how much PokLeh gets daily:

RM10 (from farm improvement cost)
RM20 (Net profit by selling 4 apples: [Gross profit, RM80] ?
[Improvement cost, RM50] ? [Wages RM10] = RM20)
RM5 (from selling apples to his workers)

In total, PokLeh gets RM35 daily compare to RM10 initially when he takes
over the farm from Razak.
His profit increases RM25 and the workers are still getting RM1.00 daily
per person.

The greedy PokLeh does not want to stop there.
One day, he says to his fellow workers:” You see ah, the current
market price for one apple is RM20 and you are only paying RM1.
See how lucky you are! I have to SUBSIDY RM19.00 for each of the apple
you buy and total I need to SUBSIDY RM95.00.
This will greatly burden the farm and we might get bankrupt if we continue like this.
In order to avoid bankruptcy, I need to increase the apple price that you
buy from RM1.00 to RM1.50 and I will bare the remaining RM18.50 per apple as my subsidy to you all. ”

So, greedy PokLeh adds RM2.50 to his current profit and the number
becomes RM37.50.


After you have read the story, I am sure you have already understood
the meaning of a ‘SUBSIDY’ given by the government.
The RM95 subsidy was never existed in the first place and so was the
RM52 billion fuel subsidy generously ‘given’ by the government..

Cutting fuel subsidy is actually just a reason to steal money from your
pocket. Are you gonna stand there and let them rob you???

Petroleum business

check.gifI don’t know what you guys are paying for petrol… but here in Durban , we are also paying higher, up to 47.35 per litre. But my line of work is in petroleum for about 31 years now, so here are some tricks to get more of your money’s worth for every litre. Here at the Marian Hill Pipeline, where I work in Durban , we deliver about 4 million litres in a 24-hour period thru the pipeline. One day is diesel; the next day is jet fuel, and petrol, LRP and Unleaded. We have 34-storage tanks here with a total capacity of 16,800,000 litres.

ONLY BUY OR FILL UP YOUR CAR OR BIKKIE IN THE EARLY MORNING WHEN THE GROUND TEMPERATURE IS STILL COLD. Remember that all service stations have their storage tanks buried below ground. The colder the ground, the denser the fuel, when it gets warmer petrol expands, so buying in the afternoon or in the evening…. your litre is not exactly a litre.

In the petroleum business, the specific gravity and the temperature of the petrol, diesel and jet fuel, ethanol and other petroleum products play an important role. A 1degree rise in temperature is a big deal for this business. But the service stations do not have temperature compensation at the pumps.

WHEN YOU’RE FILLING UP, DO NOT SQUEEZE THE TRIGGER OF THE NOZZLE TO A FAST MODE. If you look, you will see that the trigger has three (3) stages: low, middle, and high. In slow mode, you should be pumping on low speed, thereby minimizing the vapours that are created, while you are pumping. All hoses at the pump have a vapour return. If you are pumping on the fast rate, some of the liquid that goes to your tank becomes vapour. Those vapours are being sucked up and back into the underground storage tank so you’re getting less worth for your money.

ONE OF THE MOST IMPORTANT TIPS IS TO FILL UP WHEN YOUR TANK IS HALF FULL. The reason for this is, the more fuel you have in your tank, the less air occupying its empty space. Petrol evaporates faster than you can imagine. Petroleum storage tanks have an internal floating roof. This roof serves as zero clearance between the petrol and the atmosphere, so it minimizes the evaporation.

Unlike service stations, here where I work, every truck that we load is temperature compensated, so that every litre is actually the exact amount.

ANOTHER REMINDER, IF THERE IS A FUEL TRUCK PUMPING INTO THE STORAGE TANKS, WHEN YOU STOP TO BUY, DO NOT FILL UP - most likely the petrol/diesel is being stirred up as the fuel is being delivered, and you might pick up some of the dirt that normally settles on the bottom.

Hope, this will help you get the maximum value for your money.

DO SHARE THESE TIPS WITH OTHERS! LET’S SHARE INFORMATION AND BENEFIT ALL, FOR THE BETTER OF MANKIND.

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Resistors

A LITTLE THEORY

Resistors, next to wire, are the simplest of the electronic devices. They resist the flow of current, both A.C. and D.C. Theoretically, the resistance to A.C. is linear. In either case, the resistance is proportional to the ratio of voltage to current. R=E/I. This equation is derived from Ohms law, E=IR. This states that the voltage across the resistor is the resistance times the current through it. Ohm most likely measured it before he formulated it. This is one rule of thumb, namely “Why calculate what you can meaure?” What he did was put one volt across a resistance. His finding on the ammeter was that one amp flowed. He therefore, I guess wanting to make a baseline standard, declared it one unit of resistance. We call it after him, an Ohm. If one put two of these exact same resistances together and put one volt across them, one would read 0.5 amp on the ammeter Why is voltage the deciding factor? In this experiment it is the constant. So the change in resistance made a change in current, while voltage remained the same.

So he could logically conclude that two units of resistance made the current lower by 1/2, but voltage remained the same. So if I multiply 2 by 0.5 I get one, just like the voltage. E=IR or 1 = 2 X 0.5!

Resistors are generally made with carbon. The molecular structure of carbon makes it conductive but with a little resistance. The less carbon electricity must flow through, the higher the resistance. It really doesn’t take much carbon, that is why resistors are so small. A copper wire with the resistance of a 1000 ohms would likely have to be miles long and very thin. However, carbon makes for noisy audio components. The noise is due to the electrons having to bounce around those nasty little carbon molecules.

Metal film is the higher quality version and the resistor of choice for audio amps. There is less noise because the metal film is more conducive to conduction. More free electrons, therefore less noise. However, there is a floor to how much lower one can go before one can’t eliminate any more noise. This is known as Johnson noise. It will be the same level for any component one uses.

Metal film resistors are accused of making an amp sound “metallic”. I believe that this has nothing to do with the resistor being metal and more to do with the noise level. A friend of mine told me that with amps of a curve where frequencies higher than 15 kilohertz are about 1 to 2 decibels higher than flat tend to sound mettalic. The noise content of carbon resistors tends to mask the high frequency boost, hence sounding less mettalic. It’s a psychoacoustic thing.

Resistors come in a variety of tolerance values. The tolerance in this case is how much from the “advertised” value the resistor is off. If I have a resistor of 1000 ohms and the tolerance is 10 percent, then the value could range from 900 ohms to 1100 ohms. Resistors used to be had with 20% tolerance. I doubt that anyone could even find a ten percenter nowadays, let alone 20. The tolerance can go as low as 0.1%. They are pretty expensive though. 1%ers go for about 25 cents US each, where the 0.1%er will go for $2.50 or more! I would be satisfied with the 1% ones.

How do they get such tight tolerances? “Modern technology, Ted.” No, laser trimming. ;-)

But as for the psychoacoustic effects, does replacing resistors in an amplifier make a difference? Absolutely. If an engineer designs an amplifier, in this case a tube amplifier, he designs it with the specifications of the tube in mind. Any variation from the design will result in, even if subtle, a difference in the overall response of the amplifier.

According to “The Psychology of Music”, our ears can detect from five to seven harmonics in a tone. If there is a variation of amplitude by a small amount of any of the harmonics, we can detect it. This effect is more sensitivve than phase changes in harmonics. According to the book, a room is likely to smear the phase relationship of the harmonics, yet we know the difference between a guitar and a violin playing the same note. This is based on the timber which is dictated by the amplitude relationship of the harmonics.

There are some who actually have compared the “sound” of different resistors. This to me is somewhat absurd. There are claims that tantalum resistors (no longer manufactured except in Japan. Why? They cost up to 10 bucks apiece!) offer the warmth of carbon composition with the low noise and precision of metal film. I think that there is either something in the amp that is amiss or the person listening has super-duper absolutely perfect wide range hearing ears and can discern even the most minutest variation in response. I can’t (yet I can hear a difference in the sound of wire. Well, jumping from 28 gauge to 20 there is a difference anyway). I have used both types in the exact same amp and they both sound equal. The only reason I would go with metal film over carbon is the precision values one can get. In high gain applications the low noise is a plus. But that is it. There is no reactive component in a resistor that causes it to affect the frequency response of an amplifier (except maybe at RF frequencies where skin effect is the greatest). Therefore they are linear.

In a tube amplifer, the tube has several different response curves for different settings of bias. I have noticed that the closer to zero the tube is biased the more linear the curve. This changes dramatically as the tube’s curve gets closer to cut-off.

If the cathode resistor that determines the bias setting in most triode applications was to vary by 10 percent, the voltage drop across the resistor will also change. This is because more or less current will flow. If I have a 1000 ohm resistor dropping 1 volt, and it changes or actually has 900 ohms resistance, then the voltage will be .9 volts for the same current, or less for a larger current. In a tube, the closer one gets to a bias of zero volts, the more current flows, so the voltage drop across the resistor of 900 ohms could actually be .75 volts, depending on the tube. But that is the subject for the tube psych page. This would, if you take a look at a triode curve sheet, make enough of a difference that it will sound different to us.

A similar effect would be had by changing the type or make of tube. Again, the subject for the tube page.

So, in conclusion, if you just bought your first or fifth ST-70 or Conrad-Johnson or whatever, along with replacing the capacitors, invest the five or six bucks and extra hours and replace those resistors too.

My first experience with this was an old 1961 Magnavox console stereo. I replaced the capacitors, the tubes, the wires and even the tube sockets, but the most dramatic change I got was when I replaced all of the resistors. The sound was fat and lower midrange-upper bass strong. Afterwards the response “flattened” to give less fatness and lots of deeeep bass. My father ran out of his room and asked “What did you DO!?! It hasn’t sounded like that since it was new!” Well, at first I didn’t like it, but then I got used to it.

BACKGROUND OF THE INVENTION

An improvement in the processing of bituminous sands is described, whereby the concentration of bitumen in tar sand feed is measured by infrared light reflected from the tar sand surface. Near infrared is shone onto the surface of the incoming tar sand and reflected light is collected and passed through two parallel filters, one being a measuring filter having a wavelength range of 2180 to 2260 nm and the other being a reference filter having a wavelength range of 2270 to 2350 nm. The beams emerging from the filters are measured electronically and the resulting signals are separately integrated and amplified by electronic means. The ratio of the amplified signals is used to provide a read-out signal responsive to the bitumen concentration. The results may be used to adjust processing conditions in the extraction process to allow for the variations of bitumen in the feed.

1. A method for monitoring the bitumen content trends of an advancing layer of tar sand, comprising:

shining an uninterrupted beam of near infrared radiation onto the surface of said advancing tar sand to produce reflected radiation;

filtering a first portion of the reflected radiation through a first filter which passes only wavelengths of about 2180 to about 2260 nm;

filtering a second portion of reflected radiation through a second filter which passes only wavelengths of about 2270 to about 2350 nm;

sensing the radiation passed by the first filter and producing an electrical signal indicative of its intensity;

sensing the radiation passed by the second filter and producing an electrical signal indicative of its intensity;

establishing a ratio of said signals and producing an electrical output indicative of said ratio and which is indicative of the bitumen content of the tar sand; and

continuing the foregoing steps sufficiently frequently to give a reading representative of the bitumen content of the tar sand.

2. An infrared reflectance monitor, for indicating the bitumen content trend in a layer of tar sand feed being advanced past the monitor, comprising:

means for beaming infrared radiation at the tar sand;

means for focusing radiation reflected by the tar sand;

a first filter for passing only wavelengths of about 2180 to about 2260 nm;

a second filter for passing only wavelengths of about 2270 to about 2350 nm;

means for alternately positioning the filters in the path of the focused reflected radiation; and

means for sensing the intensity of each radiation species alternately passed by the filters and producing a signal indicative of the bitumen content.
Description:
FIELD OF THE INVENTION

This invention relates to an infrared reflectance monitor for indicating the bitumen content trend in tar sand feed.

BACKGROUND OF THE INVENTION

Bitumen is today being commercially extracted from tar sand using a recovery process commonly known as the hot water process.

In general, this process involves: mixing the mined tar sand with hot water, steam and sodium hydroxide in a tumbler; diluting the produced slurry with additional hot water; retaining the diluted slurry under quiescent conditions in an open-topped primary separation vessel having an outlet in its conical base, whereby aerated bitumen rises to form a primary froth, which is collected, and solids settle and are removed through the outlet; withdrawing a dragstream from the middle of the vessel, said dragstream containing non-rising bitumen and clay particles; and subjecting said dragstream to induced air flotation to recover a secondary froth.

The tar sand is a complex material. More particularly, it comprises: sand-size solid grains; connate water sheathing the grains; fine clay-like solids (-325 mesh) which appear appear to be concentrated in the water; and bitumen filling the interstices between the water-sheathed sand grains.

The concentrations of these various components, which make up the tar sand, vary throughout the deposit and hence in the feed led to the extraction plant. These variations in concentration have a marked effect on the efficiency of the recovery process.

The component whose concentration variations can most deleteriously affect the hot water process is the fine solids (hereinafter termed “fines”). The solids component of a low fines tar sand may contain in the order of 5% by weight fines, while the solids component of a high fines tar sand may contain in the order of 20% by weight fines.

Operators of the process can react to the presence of higher levels of fines in the feed by increasing the sodium hydroxide and water additions to the process; these increases will reduce the deleterious effects of the high fines on the efficiency of the bitumen recovery process.

To date, the practice used for monitoring the tar sand composition has involved sampling the feed and subjecting the samples to laboratory analysis. However, this is a time-consuming process and thus the implementation of changes in water and sodium hydroxide addition is late, with the result that the hot water process is rarely operated at optimum conditions.

There has thus existed a long-standing need for an on-line analysing means which would monitor and indicate tar sand feed grade trends accurately and quickly.

It needs to be noted that there is an inverse proportional relationship between bitumen and fines concentrations in tar sand. Therefore the development of an accurate indicator of bitumen content would provide the industry with a means for monitoring fines content.

SUMMARY OF THE INVENTION

In accordance with the invention, tar sand feed grade trends are monitored by:

(a) shining near infrared radiation onto the surface of advancing tar sand;

(b) filtering a first portion of reflected radiation through a first filter which is adapted to pass only radiation of a wavelength range absorbed to a significant extent by bitumen alone among the components of tar sand;

(c) filtering a second portion of reflected radiation through a second filter which is adapted to pass only radiation not absorbed to a significant extent by any component of the tar sand and which has a wavelength close to the first wavelength range;

(d) sensing the radiation passed by the first filter and producing an electrical signal indicative of its intensity;

(e) sensing the radiation passed by the second filter and producing an electrical signal indicative of its intensity;

(f) establishing a ratio of said signals and producing an electrical output indicative of said ratio and which is indicative of the bitumen content of the tar sand;

(g) continuing the foregoing steps sufficiently frequently to give a reading representative of the bitumen content of the tar sand.

In a preferred embodiment of the invention, the first filter is adapted to pass only radiation having a wavelength of about 2180 to about 2260 nm and the second filter is adapted to pass only radiation having a wavelength of about 2270 to about 2350 nm.

It is necessary to have two filters, adapted to pass different wavelengths (a measure and a reference), due to variations in intensity of the incident radiation and to variations in the nature of the reflective surface. Incident radiation can be affected by extraneous sources of light, alterations in electrical supply to the near infrared lamps, or deterioration of those lamps. At the same time, the tar sand reflective surface may vary according to its roughness or smoothness, the quantity of bitumen, or such properties as dryness and degree of oxidation. Before absorption of the near infrared due to bitumen can be determined, it is necessary to compensate for the extent to which the reflected rays are affected by the other properties of the tar sand or the incident radiation. It is thus the purpose of the reference filter to determine those effects on the reflected radiation due to variations of tar sand or incident radiation which are distinct from absorption by bitumen. With this compensating means present, absorption due to bitumen alone is successfully isolated from ancillary variations in reflected radiation. The wavelength range of the reference filter should be close to that of the measure filter, because the extent to which ancillary variations affect reflectance is wavelength-dependent.

The development of the present invention involved some surprising discoveries. Previous uses of reflexive infrared in connection with oil monitoring had been limited to recording oil layers having a thickness in the order of 10.mu.. This is the thickness of, for instance, oil spills on bodies of water. However, penetration to this order of depth would not be useful in tar sand monitoring, as the individual sand particles are commonly thicker than 10.mu.. It follows that one would question whether the infrared would reach interior bitumen. Surprisingly, the infrared appears to penetrate between 1 and 3 mm. into the tar sand. Also, tar sand contains variations in concentration of bitumen and there was concern that these localized rich and lean zones would deleteriously affect the desired performance of the instrument. It was found that manageable absorptions were obtained in both low and high bitumen content zones. Finally, the bituminous component, at the surface of the tar sand mass (such as a layer of tar sand on a conveyor belt), quickly becomes dry and oxidized. Its chemical nature changes significantly from the bitumen present further into the layer. There was therefore concern that this surface effect would affect the reliability of the measurement. However, bitumen readings taken at the surface of a pile have been found to be essentially the same as those obtained after the surface layer is removed.

In addition, the present inventor had to conduct extensive experimentation involving over 130 spectra and many analyses to discover the proper wavelength requirements of the filters.

Broadly stated, the invention is a method for monitoring the bitumen content trends of a layer of tar sand being advanced by a conveyor, comprising: shining an uninterrupted beam of near infrared radiation onto the surface of said advancing tar sand to produce reflected radiation; filtering a first portion of the reflected radiation through a first filter which is adapted to pass only radiation of a wavelength absorbed to a significant extent by bitumen alone among the components of tar sand; filtering a second portion of reflected radiation through a second filter which is adapted to pass only radiation not absorbed to a significant extent by any component of the tar sand and which has a wavelength close to the first wavelength range; sensing the radiation passed by the first filter and producing an electrical signal indicate of its intensity; sensing the radiation passed by the second filter and producing an electrical signal indicative of its intensity; establishing a ratio of said signals and producing an electrical output indicative of said ratio, and which is indicative of the bitumen content of the tar sand; and continuing the foregoing steps sufficiently frequently to give a reading representative of the bitumen content of the tar sand.

In another aspect of the invention, there is provided an infrared reflectance monitor for indicating the bitumen content trend in a layer of tar sand feed being advanced by a conveyor, said monitor comprising: a source of infrared radiation, which radiation may be directly shone at the tar sand; means for focusing radiation reflected by the tar sand; first and second filters that may be alternately positioned in the path of the focused reflected radiation, the first such filter being adapted to pass only wavelengths of about 2180 to about 2260 nm, absorbed by bitumen alone among the components of the tar sand, the second such filter being adapted to pass only wavelengths of about 2270 to about 2350 nm, not absorbed by any of the tar sand components; and means for sensing the intensity of each passed radiation species and producing a signal indicative of the bitumen content.

DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic showing the interrelationship of the principal elements of the instrument up to the photodetector;

FIG. 2 is a schematic showing a known instrument incorporated into the invention;

FIG. 3 is a plot showing a typical relationship between bitumen content in tar sand as determined by reflective infrared and as determined by laboratory analysis.

DESCRIPTION OF THE PREFERRED EMBODIMENT

The present tar sand monitor is an instrument which, when suspended about 40 to 60 inches above the tar sand, provides a remote indication of the bitumen concentration (weight percent) in the surface layer of said tar sand. When the tar sand is on a moving conveyor belt, the instrument continuously produces a measurement which is an averaging of the bitumen content of a strip observed over a period of approximately 30 seconds. The strip typically has a width of approximately 6 inches and a length of approximately 250 feet.

A greatly simplified layout is given in FIG. 1 to show the interrelationship of the optical and electronic elements. For greater detail, refer to FIG. 2. The monitor comprises a source of infrared radiation, more particularly a Tungsten-halogen lamp 1, mounted at the focal point of an aluminum parabolic reflector 1a. The lamp 1 is used in conjunction with a focusing lens 1b. Preferably, dual transmitters (not shown) are used, to ensure continuous operation if one lamp burns out. As stated, the lamp 1 beams radiation at the tar sand surface, which radiation is partly reflected.

A receiver lens 2 is suitably mounted in the path of the reflected radiation. The lens 2 functions to focus the incoming radiation to a small point. An arsenic trisulfide lens is suitable for this purpose.

A filter wheel 3 is positioned between the lens 2 and the latter’s focal point. The wheel 3 carries a pair of filters of the following specification:

______________________________________
Filter No. 1
center wavelength
2.22 .mu.m .+-. 0.01 .mu.m
half-band width
0.08 .mu.m .+-. 0.11 .mu.m
transmission on
50% peak or greater
wavelength
transmission off
0.1% absolute or less at all
wavelength     wavelengths out of band to 5 .mu.m
Filter No. 2
Center wavelength
2.33 .mu.m .+-. 0.02 .mu.m
half-band width
0.08 .mu.m .+-. 0.11 .mu.m
transmission on
50% peak or greater
wavelength
transmission off
0.1% absolute or less at all
wavelength     wavelengths out of band to 5 .mu.m
______________________________________

Filter No. 1 passes only radiation of a wavelength absorbed to a significant extent by bitumen alone among the components of the tar sand. The beam passed by this filter is termed the measure beam. Filter No. 2 passes only radiation of a wavelength not absorbed by any of the components of tar sand; this radiation has a wavelength close to the measuring wavelength. The beam passed by filter No. 2 is termed the reference beam.

The lamp 1, receiver lens 2, filter wheel 3, and most of the electronic equipment shown schematically in FIG. 2 and briefly described below are commercially available from Wright and Wright Inc., Oak Bluffs, Mass., in the form of a monitor designated Model E 250.

Continuing now with such description, a photodetector 5 is provided at the focal point of the receiver lens 2. This photodetector senses each of the alternately passed measure and reference beams and emits electrical signals proportional to their intensities. An indium arsenide photodetector is suitable for this purpose.

With reference now to FIG. 2, the photodetector signals are transmitted to and amplified by a preamplifier 6. The preamplifier output is fed to an AGC amplifier 16 and thence to a multiplexer 7.

A sync pick-off 8 is provided to sense and indicate when each filter is directing a beam at the photodetector 5. This sync pick-off 8 comprises a U-shaped optical switch straddling the filter wheel 3 and employing a light source and a silicon photodetector at opposite ends of the switch. Light emitted by the sync pick-off passes through slots in the outer edge of the filter wheel and thus periodically transmits a signal determined by the filter wheel position.

The pick-off signals are transmitted to a logic circuit 9 which functions to switch the multiplexer 7 to transmit the detected and amplified signal to either the measuring signal amplifier 10 or reference signal amplifier 11, depending on which filter is sensed to be in front of the photodetector 5.

There are provided measure and reference signal processing means comprising amplifiers 10, 11, synchronous demodulators 12, 13 and integrators 14, 15. The multiplexer 7 alternately shorts to ground that amplifier 12 or 13 not passing the detected and amplified signal. The synchronous demodulators 12,13 allow only signals of the frequency corresponding to the rotational speed of the filter wheel to be passed, with other frequencies being rejected. They thus reduce the electronic noise in the signal.

Each amplifier 10, 11 has adjustable gain from approximately .times.1.0 to .times.10.0, as well as zero adjustment. The amplified measure or reference signals are detected by the synchronous demodulators 12, 13 respectively. The demodulators 12, 13 are operative to pass signals at exactly the same frequency as the chopped frequency of light detected by the photodetector 5. The chopped frequency is of course set by the rotational frequency of the filter wheel 3. The sync pick-off 8 senses this chopped frequency and feeds this frequency to each of the synchronous demodulators 12, 13 through the logic circuit 9. The demodulators 12, 13 reject all detected analog signals other than this chopped frequency to thereby increase the signal-to-noise ratio.

The detected signals from demodulators 12, 13 are fed to integrators 14, 15 respectively. The integrators 14, 15 average the signal strength over a preset interval of time to compensate for signal variations due to rocks, clay lumps and variations in the tar sand oil content. A 30-second time constant has been found suitable.

An automatic gain control circuit 16 referred to as the AGC amplifier is provided to control the strength of the signals fed to the amplifiers 10, 11. The gain control circuit 16 senses the output voltage from the integrator 14, and if low, increases the gain of the AGC amplifier. Conversely, when the output voltage of the integrator 14 is high, the gain control circuit 16 reduces the gain of the AGC amplifier to prevent saturation of the amplifiers 10, 11.

The averaged signals from the integrators 14, 15 (v.sub.integrator 14 and v.sub.integrator 15) respectively are fed to a ratiometer 17. The ratiometer 17 calculates a voltage output ratio (v.sub.out) of the two signal strengths according to the equation 1 below: ##EQU1## The ratiometer 17 operates with a conventional logrithm, summation, antilog method to obtain the ratio (v.sub.out).

The output (v.sub.out) from the ratiometer 17 is fed through an output amplifier 18 and a current driver 19, and finally to an output meter (not shown). The output signal I.sub.out is also run to an external potentiometer (not shown) which returns an adjustable feedback signal to the input of the output amplifier 18 to provide current gain control. Also provided externally is a zero control (not shown). The zero and current gain controls allow adjustment such that a standard 4 to 20 mA current signal represents the desired range of bitumen content (5 to 15% bitumen).

The output signals from the integrators 14, 15 are also fed to threshold detectors 20, 21 respectively. Each of the threshold detectors 20, 21 is in turn connected to an instrument status alarm relay 22, 23 respectively. The threshold detector 20, 21 activates when the voltage level of integrator 14 or 15 output approaches zero. Activation causes the contacts of the alarm relay 22 or 23 to open, thereby indicating a monitor malfunction. Further, loss of power to the monitor de-energizes and opens the alarm relays 22,23 to indicate failure. Opening of the relay 22 or 23 forces the current output of the current driver 19 to zero.

The output meter (not shown) is a digital voltmeter which displays the amplified output signal from the current driver 19.

The monitor as described above operates off 115 V AC (60 Hz) line power and thus is provided with a low voltage power supply 24 to convert this power to .+-.15 V DC. The .+-.15 V DC is further converted to 5 V DC through a zener network 25. The monitor components operate from the 5 V or .+-.15 V DC power supply.

The AC input to the monitor is internally fused at 26 to prevent short circuit damage to the monitor. The AC input is also passed through a voltage transient suppressor 27 to suppress high voltage spikes.

FIG. 3 shows that, over the range of bitumen values of interest in various tar sand feeds, there is a linear relationship between the bitumen contents determined by chemical analysis and those determined by the infrared reflectance monitor.

While the present invention has been disclosed in connection with the preferred embodiment thereof, it should be understood that there may be other embodiments which fall within the spirit and scope of the invention as defined by the following claims.

Thyristors - SCRs and Triacs

What are Thyristors
Thyristors are used to control power in numerous applications including light dimmers and motor speed controls, solid state relays, some microwave ovens, photocopiers, traction motors for electric locomotives and electric cars, power inverters for transmission of electric power over long distances, frequency converters, other DC-DC or DC-AC or AC-AC inverters, AC-DC regulated power supplies, and many other applications where efficient power control is required.

A Silicon Controlled Rectifier is one type of thyristor used where the power to be controlled is unidirectional. The Triac is a thyristor used where AC power is to be controlled. (There are exceptions in both cases but for this simple discussion these can be ignored).

Both types are normally off but may be triggered on by a low current pulse to an input called the Gate. Once triggered on, they remain on until the current flowing through the main terminals of the device drops below a hold value which is very close to zero. It is usually not possible (at least not easy) to turn thyristors off while current is flowing. However, there are special types called Gate Turnoff Thyristors which enable this type of control as well.

Both SCRs and Triacs are 4 layer PNPN structures.
How Does a Thyristor Work?
The usual way an SCR is described is with an analogy to a pair of cross connected transistors - one is NPN and the other is PNP. The base of the NPN is connected to the collector of the PNP and the base of the PNP is connected to the collector of the NPN.

If we connect the positive terminal of a supply to say, a light bulb, and then to the emitter of the PNP transistor and its return to the emitter of the NPN transistor, no current will flow as long as the breakdown voltage ratings of the transistor are not exceeded because there is no base current to either transistor. However, if we provide some current to the base of the NPN (IG(+).)ransistor, it will turn on and provide current to the base of the PNP transistor which will turn on providing more current to the NPN transistor. The entire structure is now in the solid on state and will stay that way even when the input to the NPN’s base is removed - until the power supply goes to zero and the load current goes below the hold value.

The same scenario is true if we reverse the power supply and use the IG(-) input for the trigger.

+——+
+ >————+ LOAD +—————-+
+——+                |
|
E \|
PNP    |—+——-< IG(-)
C /|   |
|     |
|   |/ C
Gate IG(+)  >—–+—|    NPN
|\ E
|
|
- >——————————————+

A Triac works in a basically similar manner except that the polarity of the Gate can be either + or - during either half cycle of an AC cycle.

For a light dimmer or motor speed control, for example, the exact time when the thyristor is triggered relative to the zero crossings of the AC power is used to determine the power level. Trigger the thyristor early in the cycle and the load is driver an high power. Trigger the thyristor late in the cycle and there is only a small amount of power delivered to the load. The thermal or mechanical inertia is generally counted to smooth out the power and results in smooth continuous operation (i.e., a light bulb controlled by a dimmer does not flicker.)

The advantage of thyristors over simple variable resistors is that they (ideally) dissipate very little power as they are either fully on or fully off.

There are a wide variety of other types of thyristor and thyristor-like devices. In particular, are diacs and sidacs which have no gate input but simply turn on when a specified threshold voltage is exceeded across their main terminals. See the section: Testing Diacs and Sidacs. These are often used to trigger other thyristors in phase control applications.

For more information on thyristors, see Horowitz and Hill or any thyristor databook.

Testing SCRs and Triacs

* For SCRs, the gate to cathode should test like a diode (which it is) on a multimeter. The anode to cathode and gate to anode junctions should read open in both directions.

* For triacs, the gate to main terminal 1 (MT1) should test like a diode junction in both directions. MT1 to MT2 and gate to MT2 junctions should read open in both directions. (CAUTION: I’m not sure the MT1 and MT2 designations are universal - check the datasheet to be sure!)

* For diacs and sidacs, there is no gate terminal - resistance should be infinite in both directions. For more complete testing, see the section: Testing Diacs and Sidacs.

Note: Some thyristors will have a low G-K/MT1 resistance but it should not read as a short.

The real test is quite simple but will require a low voltage DC power supply and two resistors. For triacs, a negative output from the supply is desireable as well to test the triggering when the gate is negative).

R1 will be used to limit current through the device and R2 will be used to limit current to the gate. A 12 VDC supply of at least 200 mA capacity with a 100 ohm 2 W resistor for R1 and 1 K 1/4 W resistor for R2 should work for most small to medium power SCRs. Check the ‘minimum gate current’ and ‘holding current’ specs to be sure. For larger devices, R1 and/or R2 may need to be smaller.

R1
+ o—-+—–/\/\———+—–o Test+
|   100, 2W      __|__
|                _\/\_ Device Under Test - DUT
12 VDC   |    R2          / |   (SCR or triac).
+—/\/\—o < --'  |
1K     o      |
|      |
- o----------------+------+-----o Test-

1. Connect the supply as shown.

2. Trigger the gate from the positive of the supply through the current limiting resistor (R2) and see that the DUT turns on stays on when the gate is disconnected.

3. Open the circuit to the anode (with the gate connected to the cathode) and again reconnect the anode resistor. The DUT should now be off again.

* For triacs, repeat steps (2) and (3) with R2 supplied from a negative voltage.
* For diacs, testing must be at full rated voltage. See the section: Testing Diacs and Sidacs.

If the device passes these tests, it is behaving properly and is probably functional. However, without applying full voltage or current, there is no way of knowing if it will meet all specifications.

You can replace the DC supply with a low voltage power transformer (say, 12 VAC). Use a scope to monitor the voltage across the DUT or R1. Then, when the gate is connected to R2, you should see the voltage across the DUT drop to nearly zero when it switches on part way through the positive cycle. This phase will be determined by the voltage and value of R2. It should remain off for the entire negative cycle (SCRs only) with the gate connected and remain off all the time with the gate connected to the cathode.

(From: T. O. Prellwitz (timilen@halcyon.com).)

If you have a semiconductor curve tracer you can configure a small audio transformer circuit to drive the gate. I did this with my B&K and it works well. The secondary should provide enough voltage to drive the gate of the SCR and the negative swing of the AC will cycle the scr off while the positive phase turns it on. I drive the transformer with an audio generator. Hope this offers some ideas.
Testing Diacs and Sidacs
Diacs and Sidacs are thyristors without any gate terminal. They depend on the leakage current to switch them on once the voltage across the device exceeds their specified ratings. With an ohmmeter, they can be tested only for shorts. Resistance should be infinite in both directions.

However, you can test a diac or sidac with a resistor, variable power supply (you will need at least the rating of the device), and a DMM. Hook them in series and monitor across the device. With care, your variable supply can be a Variac, 1N4007, and 1 uF, 200 V capacitor. Use a 47 K resistor to limit the current:

D1            R1
~ o----|>|—-+—–/\/\———+——o Test+
1N4007   |      47K         |
_|_ C1            __|__
Variable AC     — 1 uF          _\/\_ Device Under Test - DUT
0 to 140 VRMS    |                  |
|                  |
~ o———–+——————+——o Test-

CAUTION: this is not isolated from the power line. Use an isolation transformer for safety. If the DUT is rated more than about 180 V, you will need to use a doubler and higher voltage capacitor but testing is otherwise similar.

As you increase the input, the voltage on the DUT will track it until the rated voltage at which point it will drop abruptly to zero and stay there until the voltage is reduced below its holding current. Repeat with the opposite polarity.

With a scope it is even easier as you can use an AC supply directly (remove D1 and C1) and observe that the DUT will turn on at the proper voltage on both polarities of the AC waveform and stay on until the voltage crosses 0.

Use an isolation transformer for safey.
Thyristors Driving Inductive Loads

“I am trying to turn on a triac which is driving an inductive load (solenoid) using a digital signal without using an opto triac. I get limited success.”

(From: Jeroen Stessen (Jeroen.Stessen@philips.com).)

It is soooo easy: just use a DC current to drive the gate of the triac. Even the polarity of the current doesn’t matter, although most triacs are more sensitive for a negative input current (flowing out of the gate to a negative supply). A large triac may require some 50 mA.

There will be some applications where there is no 50 mA supply available. That’s where you would want to drive with short pulses. But these pulses would have to occur around the expected instant of the zero-crossing of the load current, which is a bit tricky with an inductive load.

As an alternative you could look for a more sensitive triac, for not too large load currents there are types down to 5 mA or so. If you have 50 mA of DC to spare, go for it, it will work.

By the way, never switch an inductive load like a power transformer ON at the zero crossing of the mains voltage. That’s guaranteed to drive the transformer into saturation and create the worst possible current transient. Try and switch on at maximum mains voltage, at +/- 90 degrees delay. Do not use a voltage differentiator to generate +90 degrees phase shift, as it will be too sensitive to mains disturbances. Instead, use a double integrator to give 2 * -45 degrees and a low-pass filter. Using only 1 integrator to approach -90 degrees gives too much attenuation of the voltage, hence 2 are recommended.
Burning Up of Thyristors
(From: Neill Means (means@expert.cc.purdue.edu).)

Any thyristor will have a maximum change in current vs change in time dI/dt. If this is exceeded, then current flowing through the thyristor will find the path of least resistance through the silicon. Unfortunately, for us, this can be thought of as a molecular sized lightning bolt streaking through the doped layers of silicon - finding the path of least resistance from individual molecule to individual molecule. This soon results in an ‘avalanche’ of electrons streaming through a very small path and this process feeds on itself until the thyristor dies. This whole process probably takes only microseconds to happen.

I don’t know if fast blow fuses will help this situation if the current changes too rapidly. A fuse is a very analog device with mass and it seems like it would be a slow, lumbering giant compared to almost instantaneous current change.

The solution for this problem? I am guessing putting an appropriately sized inductor in series with the light bulb, but just be sure to add the correct over voltage snubbing network. The inductor will keep the current from changing too rapidly

Testing Semiconductor Devices with a VOM or DMM

Testing Semiconductor Devices with a VOM or DMM
VOMs and DMMs
Analog and Digital meters behave quite differently when testing nonlinear devices like diodes and transistors. It is recommended that you read through this document in its entirety.

Caution: An analog VOM on the lowest resistance range may put out too much current for smaller devices possibly damaging them. Ironically, this is more likely with better meters like the Simpson 260 which can test to lower ohms (X1 scale). Use the next higher resistance range in this case or a DMM as these never drive the device under test with significant current. However, this can result in false readings as the current may be too low to adequately bias the junctions of some power devices or devices with built in resistors.
Testing Diode Junctions with a Multimeter
On an (analog) VOM, use the low ohms scale. A regular signal diode or rectifier should read a low resistance (typically 2/3 scale or a couple hundred ohms) in the forward direction and infinite (nearly) resistance in the reverse direction. It should not read near 0 ohms (shorted) or open in both directions. A germanium diode will result in a higher scale reading (lower resistance) due to its lower voltage drop.

For the VOM, you are measuring the resistance at a particular (low current) operating point - this is not the actual resistance that you will see in a power rectifier circuit, for example.

On a (digital) DMM, there will usually be a diode test mode. Using this, a silicon diode should read between .5 to .8 V in the forward direction and open in reverse. For a germanium diode, it will be lower, perhaps .2 to .4 V or so in the forward direction. Using the normal resistance ranges - any of them - will usually show open for any semiconductor junction since the meter does not apply enough voltage to reach the value of the forward drop. Note, however, that a defective diode may indeed indicate a resistance lower than infinity especially on the highest ohms range. So, any reading of this sort would be an indication of a bad device but the opposite is not guaranteed.

Note: For a VOM, the polarity of the probes is often reversed from what you would expect from the color coding - the red lead is negative with respect to the black one. DMMs usually have the polarity as you would expect it. Confirm this using a known diode as a reference. Also, ‘calibrate’ your meter with both silicon and germanium semiconductors so you will know what to expect with an unknown device.
Transistor Testing Methodology
As with diode junctions, most digital meters show infinite resistance for all 6 combinations of junction measurements since their effective resistance test voltage is less than a junction diode drop (if you accidentally get your skin involved it will show something between 200K and 2M Ohms). The best way to test transistors with a DMM is to make use of the “diode test” function which will be described after the analog test. For both methods, if you read a short circuit (0 Ohms or voltage drop of 0) or the transistor fails any of the readings, it is bad and must be replaced. This discussion is for OUT OF CIRCUIT transistors *ONLY*.

One exception to this occurs with some power transistors which have built in diodes (damper diodes reversed connected across C-E) and resistors (B-E, around 50 ohms) which will confuse these readings. If you are testing a transistor of this type - horizontal output transistors are the most common example - you will need to compare with a known good transistor or check the specifications to be sure. There are some other cases as well. So, if you get readings that do not make sense, try to confirm with a known good transistors of the same type or with a spec sheet.

Before testing an unknown device, it is best to confirm and label lead polarity (of voltage provided in resistance or diode test mode) of your meter whether it be an analog VOM or digital DMM using a known good diode (e.g., 1N4007 rectifier or 1N4148 signal diode) as discussed below. This will also show you what to expect for a reading of a forward biased junction. If you expect any Germanium devices, you should do this with a Ge diode as well (e.g., 1N34).

The assumption made here is that a transistor can be tested for shorts, opens, or leakage, as though it is just a pair of connected diodes.

C                                    C
o                                    o
|           +–|>|—o C             |           +–|< |---o C
|/            |                      |/            |
B o---|    =  B o---+                B o---|    =  B o---+
|>            |                      |<             |
|           +--|>|—o E             |           +–|<|—o E
o                                    o
E                                    E

NPN Transistor                       PNP Transistor

Obviously, simple diodes can be tested as well using the this technique. However, LEDs (forward drop too high more most meters) and Zeners (reverse breakdown - zener voltage - too large for most meters) cannot be fully tested in this manner (see the specific sections on these devices).
Testing with a (Analog) VOM
For NPN transistors, lead “A” is black and lead “B” is red; for PNP transistors, lead “A” is red and lead “B” is black (NOTE: this is the standard polarity for resistance but many multi-meters have the colors reversed since this makes the internal circuitry easier to design; if the readings don’t jive this way, switch the leads and try it again). Start with lead “A” of your multi-meter on the base and lead “B” on the emitter. You should get a reasonable low resistance reading. Depending on scale, this could be anywhere from 100 ohms to several K. The actual value is not critical as long as it is similar to the reading you got with your ‘known good diode test’, above. All Silicon devices will produce somewhat similar readings and all Germanium devices will result in similar but lower resistance readings.

Now move lead “B” to the collector. You should get nearly the same reading. Now try the other 4 combinations and you should get a reading of infinite Ohms (open circuit). If any of these resistances is wrong, replace the transistor. Only 2 of the 6 possible combinations should show a low resistance; none of the resistances should be near 0 Ohms (shorted).

As noted above, some types of devices include built in diodes or resistors which can confuse these measurements.
Testing with a (Digital) DMM
Set your meter to the diode test. Connect the red meter lead to the base of the transistor. Connect the black meter lead to the emitter. A good NPN transistor will read a JUNCTION DROP voltage of between .45v and .9v. A good PNP transistor will read OPEN. Leave the red meter lead on the base and move the black lead to the collector. The reading should be the same as the previous test. Reverse the meter leads in your hands and repeat the test. This time, connect the black meter lead to the base of the transistor. Connect the red meter lead to the emitter. A good PNP transistor will read a JUNCTION DROP voltage of between .45v and .9v. A good NPN transistor will read OPEN. Leave the black meter lead on the base and move the red lead to the collector. The reading should be the same as the previous test. Place one meter lead on the collector, the other on the emitter. The meter should read OPEN. Reverse your meter leads. The meter should read OPEN. This is the same for both NPN and PNP transistors.

As noted, some transistors will have built in diodes or resistors which can confuse these readings.
Testing Power Transistors
Power transistors without internal damper diodes test just about like small signal transistors using the dual diode model, high in one direction B-E or B-C. If there is a built in damper diode, it is across C-E back biased under normal operating conditions. Therefore, a reading between C-E will also test low in one direction and B-C will show a double diode drop in the reverse direction. Also, there is often a low value resistor - about 50 ohms - between B-E when there is a built in damper. This will show up as a nearly zero volt junction drop on the diode test scale of a DMM but such a reading does not indicate a bad part. Use the resistance scale to confirm.
Testing Darlington Transistors
A Darlington is a special type of configuration usually consisting of 2 transistors fabricated on the same chip or at least mounted in the same package. Discrete implementations as well as Darlingtons with more than 2 transistors are also possible.

In many ways, a Darlington configuration behaves like a single transistor where:

* the current gains (Hfe) of the individual transistors it is composed of are multiplied together and,

* the B-E voltage drops of the individual transistors it is composed of are added together.

Darlingtons are used where drive is limited and the high gain - typically over 1,000 - is needed. Frequency response is not usually that great, however.

C
o
|
+——-+
|       |
B1 |/ C1     |
B o—–|         |
|\ E1     |
|  B2 |/ C2
+—–|
|\ E2
|
o
E

Testing with a VOM or DMM is basically similar to that of normal bipolar transistors except that in the forward direction, B-E will measure higher than a normal transistor on a VOM (but not open and 1.2 to 1.4 V on a DMM’s diode test range due to the pair of junctions in series. Note, 1.2 V may be too high for some DMMs and thus a good Darlington may test open - confirm that the open circuit reading on your DMM is higher than 1.4 V or check with a known good Darlington.
Testing Digital or Bias Resistor Transistors
Occasionally you may find a transistor that includes an internal bias resistor network attached to the base and emitter so that it can be driven directly from a digital (e.g., TTL) source. These may be used in consumer electronic equipment where space is critical or for no good reason other than to make it difficult to locate a suitable replacement device!

C
o
|
R1         |/
B o—/\/\—+—-|     Typical R1, R1: 47K.
|    |\
/      |
R2 \      |
/      |
|      |
+——+
|
o
E

The addition of R1 makes testing with a multimeter other than for shorts more difficult. With a VOM, you should see a difference in the B-E and B-C junctions in the forward and reverse directions. However, a DMM will probably read open across all pairs of terminals.
Testing Unijunction and Programmable Unijunction Transistors
Unijunction Transistors (UJTs) and Programmable Unijunction Transistors (PUTs) are used in similar sorts of circuits though the UJT is all but extinct. They both exhibit a negative resistance characteristic and can be used easily in low to medium frequency free running relaxation oscillators and other trigger type circuits.

* The UJT goes into heavy conduction from E to B1 when E becomes more positive than a critical trigger voltage, Vt = n * Vbb + .6. (n, the ‘intrinsic standoff voltage’ is typically about .6). It continues to conduct until the emitter current drops below some minimum ‘valley current’ value. Sounds sort of like a thyristor, right? :)

* The PUT is even more like a thyristor: The PUT in that the triggering takes place when the G becomes more positive than the A (probably plus a diode drop, .6 V) so that the threshold voltage can now be set with a voltage divider feeding the anode. Then, current flows from the G to the K terminal. Note that its leads are even labeled like an SCR but it behaves sort of backwards!

For an initial test, check between B1 and B2 (UJT) or A and K (PUT) with an ohmmeter. The resistance should be the same in both directions and typically a few K ohms or more. A short or wildly different readings would indicate a bad device.

This doesn’t prove that the device is good - only that it isn’t blown up. A more complete test requires a simple circuit and some means of detecting an audio output signal.

For the UJT:

+5 VDC o——–+———+
|         |
/         |
R1 \         |
100K /         |
\         |
|         |B2
+—–. |-+
|      \|   Q1 UJT
|      E|-+——–o
|         |B1
C1 _|_        /      To scope or
.01uF —     R3 \      audio amp
|      1K /      ~1K Hz
|         \
|         |
Gnd o———+———+——–o

For the PUT (Programmable Unijunction Transistor), an additional voltage divider (R3 and R4) is needed to set the threshold:

+10 VDC o——–+—————–+
|                 |
/                 /
R1 \              R3 \
100K /              1K /
\                 \
|                 |
|             +—+
+———+   |   |
|         |A  .G  |
|    Q1 __|__/    |
|   PUT _\_/_     |
|         |K      |
|         +——-|——o
|         |       |
C1 _|_        /       /   To scope or
.01uF —     R2 \    R4 \   audio amp
|      1K /    1K /   ~1K Hz
|         \       \
|         |       |
Gnd o———+———+——-+——o

(From: Spehro Pefhany (speff@interlog.com).)

A PUT is essentially an SCR with a large reverse gate breakdown voltage (G can be more positive than A by maybe 40 V) and a sensitive gate. When the voltage at A exceeds the voltage at G by a diode drop, and assuming enough voltage from A to K, the SCR turns on (conducts from A to K) and stays that way until the current drops below the holding current (typically around 100 uA, but it drops with increasing resistance in series with the gate).

Symbol and example:

_
/   \
A   G              —–
| /               |     |
—–               |     |
\ /    PUT          —–  2N6028
—–                | | |
| K                A G K

If you connect your meter from A to K, it should measure open both ways. If you connect the positive lead (which may be red or black, depending on the meter design) to A and the negative lead to K, and then momentarily short G to K it should change to a relatively low resistance reading (meter dependent). It will most likely stay latched when the G lead is returned to being open, because the meter measuring current will exceed the “holding current” of the PUT (called “valley current” in PUT specs).

If your meter has a “diode” range (in the ohms group), using that would assure there is enough open-circuit voltage to make this work, but it works this way in the half-dozen or so meters I have checked, using reasonable ohms ranges.

Measurements between A and G, with K open, should be similar to a silicon diode (fairly low in one direction, open in the other). Between G and K, with A open, should be open in both directions.

PUTs are pretty sensitive (less than 1 uA trigger current) so be sure to keep fingers away from the G lead.
Testing a Photodiode
Photodiodes are used in all sorts of equipment from PC mice (those with a ball) to high power lasers (for monitoring the output power). They are generally very reliable and rarely fail on their own. However, some types are susceptible to damage from ESD and other abuse.

The following assumes a silicon photodiode which is the most common type with a useful spectral range from near-UV to near-IR, typically from 400 to 1,150 nm at the 10 percent response points. See the chart in: Typical Silicon Photodiode Spectral Response.

The simplest electrical test is to check it like a normal diode. The results should be similar - a forward voltage drop of 0.5 to 0.7 V, and open in the reverse direction. For GaAs and other types, the forward voltage drop will differ.

To test for functionality, connect the photodiode to a multimeter set to its mA current range (1 mA full scale optimal). This is operating the photodiode in photovoltaic mode - like a solar cell. A laser pointer or helium-neon laser is the ideal light source to use for testing, but the Sun, a light bulb, a flashlight, or even an LED will work fine as well but will not provide any useful sensitivity information. For the laser source, the sensitivity should be between 0.2 and 0.5 mA/mW of laser power depending on wavelength. So, using a typical cheap Far East import red laser pointer (typically 3 mW at 650 nm), the current will be about 1 mA.

For a more accurate measurement, reverse bias the photodiode with a few volts with a current limiting resistor (for protection) and repeat the light measurement. This is operating the photodiode in photoconductive mode, which is probably the way it is used in your equipment. The results should be similar but the response is more linear at higher current than in photovoltaic mode.

For most applications, photodiodes either work or they don’t. But in some cases, performance degradation may occur from age or abuse. Substitution of a known good device is the easiest confirmation where the photodiode appears to behave properly based on the tests above, but doesn’t perform properly in-circuit.

All about Resistor

How do you know if a resistor is correctly restricting the flow of electricity? Using a multimeter is an obvious answer. However, there is more to it than meets the eye. This article will explain what you need to know.

When a PC stops working, it’s often cheaper and easier to replace it than to repair it. After all, why repair a computer that your company bought two years ago when you can buy a new one that’s twice as powerful for half the cost of your original machine? However, for many IT support technicians today, the time and energy spent repairing electronic equipment is still necessary because of budget constraints or because of the sensitive nature of data kept on many desktops. Fortunately, there are quite a few tools at the technician’s disposal. And when it comes to repairing electronics, few tools are as handy as a multimeter. In this article, I’ll show you how to use a multimeter to troubleshoot some basic electronic components, such as resistors.
Before we begin
Every multimeter is different, so the instructions that I give you may not exactly match up with your multimeter. Therefore, make sure you understand how to use your specific model of multimeter before you try any of these techniques. Failure to do so could result in injury or damage to the components that you are testing.
Resistor ratings
Resistors are probably the easiest component to test with a multimeter. Resistors are designed to decrease electrical current. For example, if a circuit required the use of a transistor, but the amount of electricity being used was sufficiently high enough to damage the transistor, then one way of being able to use the transistor is to place a resistor in front of it.

Color band
Before you can test a resistor, you need to know its strength and tolerance. Resistors are color-coded. If you look at a resistor, one end should have a gold, silver, or white band. Turn the resistor so that this band is to your right. That band represents the resistor’s tolerance. Before I discuss tolerances, you need to know how to read a resistor’s values. You begin by translating the colored bands into numbers and recording those numbers. For the first and second colored bands, the values are as follows:

* Black = 0
* Brown = 1
* Red = 2
* Orange = 3
* Yellow = 4
* Green = 5
* Blue = 6
* Violet = 7
* Grey = 8
* White = 9

Multiplier band
Once you find the values for the first two bands, write them down. For example, if you have a red band and a black band, then the values will be 2 and 0. Put these two numbers together and you’ll get the number 20. The third band is the multiplier band. This is the number you’ll multiply the first two bands by to get the resistor’s value. The color scheme for the third band is as follows:

* Black = 1
* Brown = 10
* Red = 100
* Orange = 1000 (or 1 K)
* Yellow = 10,000 (or 10 K)
* Green = 100,000 (or 100 K)
* Blue = 1,000,000 (or 1 M)

Pretend that a resistor had red, black, yellow, and silver bands. I already explained that the red and black bands in the first two positions would translate into 2 and 0, which are joined to read as 20. The yellow band in the third position is a multiplier. The multiplication value is 10,000 (or 10 K). Now, multiply 20 by 10,000 and you’ll get 200,000. This means that the resistor is rated at 200,000 ohms, more commonly expressed as 200 K ohms.

Tolerance band
Let’s take a look at the tolerance band. The reason for having a tolerance band is that no resistor performs at exactly its rated value. The tolerance band is there to let you know how much the resistor could potentially be off by. A gold resistor means that the rated value is within plus or minus 5 percent of being accurate. A silver band means that the resistor’s actual value may be within plus or minus 10 percent of the rated value. If there is no tolerance band, it means that the resistor has an actual value within plus or minus 20 percent of the rated value.

Now we’ll go back to our 200,000 ohm resistor. This resistor had a silver tolerance band, meaning that it is accurate within plus or minus 10 percent of the rated value, with 10 percent of 200,000 equaling 20,000. If we add 20,000 to 200,000, we determine that the resistor’s actual measurement could be as high as 220,000 ohms. Likewise, if we subtract 20,000 from 200,000, the resistor could have a resistance of as low as 180,000 ohms.

Testing resistors
Now that you know how to read a resistor’s estimated values and potential values, let’s take a look at how to check for a bad resistor. Generally, resistors are pretty durable, but they can be cooked by excessive amounts of electricity. Back in my college electronics class, I remember more than one classmate cooking resistors with too much juice. Usually, the resistor gets hot, starts smoking, and makes a strange high-pitched squeal.

Once a resistor has been blown, often no electricity can pass through it. Such resistors are said to have infinite resistance. At the same time, if the resistor was damaged by excessive voltage but not destroyed, the resistor may allow some electricity to pass but have an incorrect level of resistance. This is why it is so important to know about tolerances. For example, if you knew that a resistor was supposed to have a value of 200,000 ohms but tested the resistor at 180,000, you might assume that the resistor was bad.

When testing a resistor, the multimeter is passing a known amount of electrical current through the resistor and then measuring the amount of current that actually makes it through. Since the multimeter is passing current through the resistor, you want to ensure that the device containing the resistor you are testing is unplugged and turned off. If a normal amount of current were flowing through the resistor and you tried to test the resistor, not only will your reading be inaccurate, but you could damage the resistor and other components. You could also damage your multimeter or receive a nasty electrical shock.

With that said, multimeters are designed to use scales. These scales determine how much current the multimeter will use during the test. For example, my multimeter has scales for 200 ohms, 2 K ohms, 200 K ohms, 2 M ohms, and 20 M ohms. If I were to test our fictitious 200 K ohm resistor with this particular meter, I would set the scale at 200 K ohms. However, it’s purely a coincidence that my meter has a setting for 200 K ohms. Normally, there won’t be a scale setting that matches the value of the resistor. In such situations, you’ll want to go to the nearest scale value above the resistor’s rating. For example, if you had a 100 K ohm resistor, you would use the 200 K ohm scale. If you had a 300 K ohm resistor, you’d use the 2 M ohm scale. The available scales will differ among brands and models of multimeters, but the concept remains the same.

Once you’ve verified that the device is unplugged and powered off and that your meter is set to the correct scale, it’s time to take a measurement. Resistors aren’t polarized, so it doesn’t matter which side of the resistor you place the meter’s red or black probes on. Once you place the probes against the resistor’s leads, you should receive a value for the resistor.

For demonstration purposes, I decided to use my meter to actually test a 200 K ohm resistor. The resistor tested at 197.6 ohms. This was well within the 180 K to 220 K range allowed by the resistor’s 10 percent tolerance. Had the resistor tested outside of this range, the resistor would have been bad and would have needed to be replaced.

Guidelines for Testing Components

Guidelines for Testing Components

Test Situation Considerations
Testing resistors With the right tester you can easily verify a resistor’s value. However, when there are other resistors in parallel with the resistor being tested, the measured value will be lower as defined by the formula Rmeasured = R1*R2/(R1+R2).

If the tester self-learns the assembly you’ll notice the resistance values automatically account for the parallel effects. If you are creating a test program, you will need to adjust the resistance values for the parallel effects. MDA testers may use point guarding to eliminate the effects of parallel components.

Testing electrolytic and tantalum capacitor polarity Detecting reverse polarity of electrolytic and tantalum capacitors usually requires visual inspection since the capacitance value will appear correct during a brief electrical test.
Testing more than just capacitors, diodes, and resistors When a tester self-learns it might not identify all the components in the assembly. Many testers allow you to add instructions to test various components. You can check the resistance of inductors, thermocouples, MOV’s (Metal Oxide Varistors), switches, relays, proximity switches, high voltage zener diodes, “Transorbs”, serial EEPROM’s (including programming), transistors, orientation of IC’s and open pins to IC’s, opto-couplers, LED’s and more. It can be a challange to verify certain components using resistance, capacitance, or voltage-drop measurements. Let us know about your applications and we’ll help you come up with an appropriate testing solution.
Testing twisted-pairs To check twisted-pair cabling, continuity testing alone is not sufficient. It is possible to have proper point-to-point continuity and still have split-pairs. A tester with sensitive capacitance measurement capability can detect split-pairs. If your application also requires near-end/far-end crosstalk and attenuation tests you’ll need to select a tester with those capabilities.
Components effect on test speed Assemblies with wires only (no components) are tested very quickly (hundreds of points per second). Assemblies with lots of passive components, especially if these components have many common connections, slow down the test rate dramatically. With slower testing it gets harder to find intermittent errors.
Damage to components with high voltage tests Hipot testing verifies proper electrical isolation between circuits. It is safe to perform hipot tests on assemblies with embedded components as long as no voltage drop occurs across any component. It is okay for both ends of a component to be raised to a high voltage with respect to other points in an assembly. Many testers self-learn the test program and might not properly learn all components. You can assure no damage to components during hipot testing by closely checking the test program to make sure all components are included