Fiber Optic Speed of Light Apparatus
Contents
1. 19 REFERENCES ae 20 GLOSSARY ise eee 22 INTRODUCTION Welcome to the fascinating world of fiber optics technology We believe you will find the instructions and exercises in this science curriculum not only educational but challenging and enjoyable as well This manual is an essential component of the Speed of Light Apparatus which is designed for use in science physics industrial technology and vocational education classrooms grades 10 12 Physics fans and other science oriented individuals including those who are just intellectually curious about how things work may also obtain the apparatus for studies in home or workshop Your particular apparatus may have been purchased either fully assembled at our factory or in kit form which you can assemble on your own Easy to follow instructions for this kit are contained in the Assembly portion of this manual The manual is intended to guide both instructors and students through a basic introduction to the principles of fiber optics and the measurement of the speed of light The apparatus includes one experiment along with descriptions of components a glossary of terms commonly encountered in fiber optics and a list of optional reading references which discuss fiber optics theory and development Everything is here for you to get in on the ground floor of fiber optics to develop an understanding of emerging technology in this vast new field of potential applicat2. amp LED Sources ANSI Standard Z136 2 LIA 12424 Research Parkway Suite 130 Orlando FL 32826 A User s Manual for Optical Waveguide Communications Gallawa U S Department of Commerce Monthly publications The first two items are journals which are available to members of the respective professional societies The last four are trade magazines available free of charge to qualified readers Applied Optics Optical Society of America 1816 Jefferson Place NW Washington DC 20036 Optical Engineering SPIE P O Box 10 Bellingham WA 98227 Fiberoptic Product News Gordon Publications Inc Box 1952 Dover NJ 07801 Laser Focus World PenWell Publishing Co 1421 S Sheridan Tulsa OK 74112 Lightwave Magazine PenWell Publishing Co 1421 S Sheridan Tulsa OK 74112 Photonics Spectra The Optical Publishing Co Berkshire Common Pittsfield MA 01202 4949 Fiber Optic Buyers Guides Fiberoptic Product News Buying Guide Gordon Publications Inc Box 1952 Dover NJ 07801 Lightwave Buyer s Guide PenWell Publishing Co 1421 S Sheridan Tulsa OK 74112 Organizations Optical Society of America 1816 Jefferson Place NW Washington DC 20036 Society of Photo Optical Instrumentation Engineers SPIE P O Box 10 Bellingham WA 98227 Laser Institute of America 12424 Research Parkway Suite 130 Orlando FL 32826 21 GLOSSARY Abso rption In an optical fiber the loss of optical power resulting from conversion of that powe
3. apparatus Connect the ground lead from Channel 2 s probe to the ground test point just below the Delay white test point Move Channel 2 s input selector to the ground position Plug the connector of the 110 VAC to DC power adapter into the receptacle on the left side of the apparatus Plug the AC adapter into a 110 VAC 60 Hz receptacle As soon as the AC adapter supplies power to the apparatus the yellow LED should light up D3 the fiber optic LED should also be visible if you lean down to look sideways into the front of the blue fiber optic housing Turn the Calibration Delay knob on the apparatus to the 12 o clock position Loosen the fiber optic cinch nuts on the fiber optic LED D3 and detector D8 Select the 15 cm length of plastic fiber and insert one end of it into LED D3 until it is seated then ightly tighten the fiber optic cinch nut Insert the other end of the optical fiber into detector D8 until seated then tighten its fiber optic locking nut Calibration It is important to calibrate this apparatus to ensure accurate results for the remainder of the activity The calibration will be done with 15 cm of optical fiber installed to simulate a distance of zero Admittedly 15 cm is not zero range but the time delay in 15 cm of fiber is less than one nanosecond not enough to affect the accuracy of this apparatus and test equipment If at any time your results differ from those we describe you should go back and
4. be completed on the opposite side Avoid applying prolonged heat to any part of the board or component to prevent damage After soldering each component trim its lead length flush with the solder copy of the printed wiring board s legend is shown in Figure 8 Use it to properly place the components on the board A copy of the circuit schematic is also included as Figure 9 1 10 up Identify pin 1 of U2 and U3 the lower left pin of the integrated circuit IC when viewed from above Insert the ICs into designated spots marked on the printed circuit board with pin 1 to your lower left The lettering on the ICs will face the same direction as the markings on the board Solder in place Identify the plus and minus signs on U4 and match them to the same signs on the printed circuit board Insert resistors R1 through R7 and R9 through R16 one at a time into the printed wiring board and solder Do not install the potentiometer R8 yet Orientation of diodes D2 and D4 through D7 is critical Line up the bar markings on the diode with the bar on the printed circuit board diode positional indicators Insert and solder C1 and C2 are capacitors which are sensitive to the direction in which they are installed Identify the wire lead marked with minuses then the round pad on the printed wiring board corresponding to that capacitor Match up the two insert the leads properly into the board and solder each capacitor into plac
5. disprove old beliefs to overcome the challenges of the unknown and to master the mysteries of science with innovation and determination ACTIVITY Using the Speed of Light Apparatus and a dual channel oscilloscope you will be able to measure the speed of light in a transparent medium In this case the medium is plastic optical fiber The transmitter portion of the apparatus generates more than 500 000 light pulses per second which appear as a cone of red light leaving the red LED When one end of the fiber is connected to an LED and the other end to a detector or receiver our red light will make a circular trip through the fiber The time required for these red pulses to travel through a 20 meter long fiber is about 100 billionths of asecond or 100 nanoseconds A bit on the quick side Rather However with the aid of an oscilloscope this becomes a straightforward practical and visually rewarding demonstration of how an elusive natural phenomenon such as light can be captured briefly and measured by people who put their minds to work Materials Required for the Project Speed of Light Module which includes Speed of Light Apparatus 110 VAC to DC power adapter use only the one provided 15 centimeters of plastic fiber 20 meters of plastic fiber Required but not included Dual channel oscilloscope 20 MHz bandwidth or greater time base measurement capability of 0 1 micro seconds or less 2 oscilloscope probes f
6. its start back in the days when tinkerers and scientists were trying their best to bend light around corners It isn t exactly clear why anyone would want to do that but a lot of people even a hundred years ago were unwilling to accept that light travel was confined to straight lines They tried hundreds of schemes many involving intricate arrangements of mirrors but no one scored big until 1870 when English physicist John Tyndall 1820 1893 demonstrated a most impressive principle to members of the British Royal Society With a simple apparatus whose major components included a light source a slender stream of falling water and a bucket Tyndall demonstrated that light could be guided inside a most definitely un straight arc of water His equipment is represented in Figure 2 rays gradually leak out Figure 2 John Tyndall s demonstration Guiding light in water 4 Good show Good show Tyndall depicted for the first time what now occurs millions of times a day in our high tech communications industry Light is guided inside some curving medium and very little is allowed to escape until we re ready to let it go He used astream of water We use slender fibers of glass and plastic Sixty five years after Tyndall s water light and bucket demo Norman R French a scientist with American Telephone and Telegraph AT amp T conceived of and demonstrated the use of light guiding fibers as communica
7. materials at a 90 degree angle most of that light is going to penetrate the materials and keep on going The same will be true if the incident angle is very small say on the order of a few degrees away from the perpendicular However as Snell s law tells us there is a point otherwise known as the critical angle when the incident light ray is leaning well away from the perpendicular when the incoming light will be totally reflected off the boundary between the two materials as in optical fiber Stated another way If light traveling through one material encounters another material having a lower index of refraction and if that light strikes the boundary between the materials at a low enough or glancing angle it cannot escape from the first material This is where we get the term total internal reflection which explains how light is guided in an optical fiber There is Always a New Frontier We ve come quite a distance in time and technology since the days when Galileo grappled with the awesome speed of luminous energy Today knowing the speed of light isn t so important to us as our ability to control way in which light travels Through the marvels of fiber optics we have achieved partial control but we are only on the threshold of new discovery Just as people in John Tyndall s day wanted to throw a few curves into the flight path of light you can bet that people today perhaps even you are thinking of ways to
8. you purchased your Speed of Light Apparatus as a kit you must first assemble it following the instructions in the Assembly portion of this manual If the kit was assembled at the factory you may proceed with Equiprnent Setup following t Check the ends of the fiber to see if they are polished and flat If not go to the Fiber Preparation section and polish the ends of the fiber cable before going further Equipment Setup if 2 Turn on the oscilloscope On the oscilloscope make the following settings e Set the Horizontal Mode Switch on A e Set the Triggering Mode on Auto e Set the Trigger Source Switch on Channel 1 e Set Triggering on Positive Slope e Set the voltage control of input Channel 1 on 1 volt per division e Set the voltage control of input Channel 2 on 0 5 volt per division e Set the input coupling of both channels on AC e Set the Timebase on 50 nanoseconds per division e Set Verticle Mode to ALT Connect the probe of Channel 1 to the blue test point marked Reference on the Speed of Light Apparatus Connect the Ground lead of Channel 1 s probe to the ground test point just below the Reference test point It is not essential to use probes with ground leads but the waveforms on the oscilloscope screen will have better shapes from which measurements can be made If your probes do not have ground leads use the ground on the oscilloscope Connect the probe of Channel 2 to the Delay blue test point on the
9. 4 sheet metal screws provided fasten the printed circuit board onto the raised supports of the chassis Do not overtighten the screws or you could crack the chassis Remove the adhesive backing from the four rubber feet provided and attach one to each corner of the chassis base Proceed to the Fiber Preparation section to finish the ends of the fiber cable 18 FIBER PREPARATION Cutting and polishing the ends of plastic fiber cable is easy In addition to the items contained in your kit you need only a polishing liquid water glycerin or light oil a sharp knife or single edge razor blade and a wire stripper The 600 grit paper included in the kit for polishing fiber can be reused by rinsing it under tap water to remove any polishing residue To polish the two fiber optic cables complete Steps 1 and 2 below for both ends of each fiber 1 Cut 1 to 2 mm off the end of the fiber cable with the razor blade or sharp knife trying to get as square a cut as possible Wet the 600 grit polishing paper with water or light oil and place the paper abrasive side facing up on any hard flat surface Polish the end of the fiber by moving it in a Figure 8 pattern against the paper while holding the fiber perpendicular to the polishing surface Supporting the fiber against a flat perpendicular object during polishing will help support the flexible fiber and result in better flatter termination After 20 Figure 8s examine the en
10. Fiber Optic Speed of Light Apparatus Instruction Manual INDUSTRIAL FIBER OPTICS Copyright 2010 Previous Printings 2001 2004 by Industrial Fiber Optics Inc 12 0225 IF SL Rev G Printed in the United States of America All rights reserved No part of this publication may be reproduced stored in a retrieval system or transmitted in any form or by any means electronic mechanical photocopying recording or otherwise without prior written permission from Industrial Fiber Optics Inc INDUSTRIAL FIBER OPTICS 1725 West 15 Street Tempe AZ 85281 7622 USA TABLE OF CONTENTS INTRODUCTION s 1 BACKGROUND INFORMATION cene 2 THE SPEED OF LIGHT A CENTURIES LONG QUEST 2 SPEED ZONES OCCUR WHEN LIGHT MEETS MATTER 3 FIBER OPTICS LIGHT MEETS ITS MASTER 4 OPTICAL FIBER THE WORKHORSE TODAY 5 THERE IS ALWAYS A NEW FRONTIER 22 7 AG TV i eee ee 8 MATERIALS REQUIRED FOR THE 8 EQUIPMENT SETUP oai cicadas cele ede oo edese 9 en NnCuis 10 MEASUREMEN pg 11 SPEED OF LIGHT CALGULATIGON etit 11 APPENDIX 13 5 13 FIBER PREPARATION 2 E i rtetu
11. al form usable by other devices See also Transmitter Responsivity The ratio of detector output to input usually specified in amperes watt or microamperes per microwatt for photodiodes photodarlingtons and phototransistors Rise time The time required for an output to rise from a low level to peak value Typically specified as the time to rise from 10 percent to 90 percent of its final steady state value See also Fall time Scatte ring The changes in direction of light confined within an optical fiber occurring due to imperfections in the core and cladding Scattering causes no changes in the wavelengths of radiation See also Absorption Splice A permanent junction between two optical fiber ends Step index fiber An optical fiber in which the refractive index changes abruptly at the boundary between core and cladding Transmitter A device that converts an electrical signal into an optical signal for transmission through a fiber cable See also Receiver 208
12. c or glass Plastic fibers cost less than glass but they lose light more readily Both consist of two essential layers of transparent optical materials core and cladding Viewed from one end as in Figure 3 the fiber materials appear in m cross section as concentric circles Strenath with a common center or axis members thus the term coaxial The outer layer is called cladding the inner Buffer layer which carries the light is s called the core What makes this ng little combination workable is the Core concept we discussed earlier called the refractive index The Figure 3 Cross section of a typical optical cable cladding of an optical fiber has a lower refractive index than that of the core and that simple difference helps trap light rays within the core rather than allowing them to wander off into space When light enters an optical fiber it travels in a straight line until it strikes the boundary between core and cladding At that point light is deflected back into the core and proceeds once again in a straight line until it strikes the core cladding boundary again The process repeats itself time and again and it permits light to negotiate curves in the fiber by sort of ricocheting its way around the turns Whether we re talking glass or plastic however one principle works the same for both and that s a little jewel known as Snell s Law the thing that explains the ricochet around the turns process we described abo
13. d of the fiber A microscope or magnifying glass is helpful but not required If the end is cloudy not flat or has scratches repeat Step 2 E w m FX 7 y ee Tem FIBER OPTIC V m M d P M 7 uc MMC d 7 is fee j i j PAPER Y du gy e 7 gt a PB UC E gt uL lt ae o P d See ee SS a bcd FIGURE g MOTION Figure 10 Figure 9 pattern used for polishing the fiber ends 5 Your Speed of Light Apparatus is now ready for operation Turn to the ACTIVITY section of this manual for step by step instructions on how to operate the apparatus 19 REFERENCES Following is a list of books magazines and other publications which may be useful in the study of fiber optics If the title does not mention fiber optics please still consider it a worthwhile source of information since fiber optic systems span multiple technologies BOOKS INTRODUCTORY Fiber Optics A Bright New Way to Communicate Billings Dodd Mead amp Company New York NY 1986 The Rewiring of America The Fiber Revolution David Chaffee Academic Press Inc Orlando FL 32887 1988 Understanding Fiber Optics Second Edition Hecht Howard W Sams 201 West 103rd Street Indianapolis IN 46290 1989 Fiber Optics Communications Experiments amp Projects Boyd Howard W Sams 4300 West 62nd Stre
14. double check your measurements A pulse should now be observed as Channel 1 on the oscilloscope CRT screen It should be approximately 3 5 volts in amplitude and 35 nanoseconds in pulse width The pulse width is measured at 50 amplitude of the pulse See Figure 5 This is the calibration pulse which will serve as a reference pulse for subsequent measurements Turn the input selector of Channel 2 from ground to AC coupling A second pulse from 1 to 1 5 volts in amplitude and 75 nanoseconds wide should also now be visible This is the pulse received through the 15 cm fiber optic cable Using the vertical positioning knobs align the bases of Channel 1 and Channel 2 traces with the second grid line above the bottom of the CRT screen Using the horizontal positioning Figure 5 o of the oscilloscope screen knob align Channel 1 with the with the Reference pulse displayed as Channel 1 second grid line from the left of the CRT screen Rotate the Calibration Delay knob on the until the EE of the received pulse coincides with the peak of the reference pulse as shown in Figure 6 Readjust the oscilloscope s sweeptime timebase scale to 20 nanoseconds per division This scale may be available only by using the 10X magnification knob on the oscilloscope Consult the oscilloscope operator s manual if you are uncertain about how to locate the proper scale Fine tune the Calibration Delay Adjustment knob on th
15. e There is no positive negative orientation of capacitors C3 through C8 Identify each insert leads through the board and solder in place O1 is the only 3 lead metal can transistor in your kit Align the metal tab protruding from the can with the white ink tab on the printed wiring board and solder O2 and Q4 are 4 lead metal can transistors Align the metal tab protruding from the can with the white ink tab on the printed wiring board then solder all leads into place Locate the square pad within the area on the wiring board designated for placement of D1 the yellow LED Insert the shortest leg of D1 the cathode into the square pad on the printed wiring board and solder into place U1 will be installed with the flat metal tab contacting the board Use needle nose pliers to grip the three leads approximately 0 3 inch 7 5 mm out from the square black base and bend them downward at a 90 angle to penetrate the board Insert the 4 40 screw through the metal tab and the wiring board and fasten it in place using the nut provided Solder the three leads onto the board Install the two white test points H2 at the locations on the wiring board marked as GND connections then solder 17 12 13 14 15 16 17 18 19 Install the two blue test points that are marked as Reference and Delay and solder to the wiring board Clean the printed circuit board with soap and warm water to remove solder r
16. e D6 13914 1 4148 Switching diode D7 1 1 914 1 4148 Switching diode D8 IF D91 Fiber optic photo diode Black housing orange dot Ci 1 uf 50 V Electrolytic capacitor C2 0pf16V Electrolytic capacitor C3 150 pf Axial ceramic capacitor Brown green brown silver or 151 C4 150 pf Axial ceramic capacitor Brown green brown silver or 151 C5 047 uf Axial ceramic capacitor Yellow violet orange silver 473 C6 150 pf Axial ceramic capacitor Brown green brown silver 151 C7 150 pf Axial ceramic capacitor Brown green brown silver 151 C8 047 uf Axial ceramic capacitor Yellow violet orange white 473 Ri 1k 1 4 watt carbon film resistor Brown black red R2 22k 1 4 watt carbon film resistor Red red red R3 270 ohms 1 4 watt carbon film resistor Red violet brown R4 22k 1 4 watt carbon film resistor Red red red R5 47 ohms 1 4 watt carbon film resistor Yellow violet black R6 22k 1 4 watt carbon film resistor Red red red H7 22k 1 4 watt carbon film resistor Red red red R8 10k Linear potentiometer Not applicable R9 47 ohms 1 4 watt carbon film resistor Yellow violet black R10 220 ohms 1 4 watt carbon film resistor Red red brown R11 10k 1 4 watt carbon film resistor Brown black orange R12 22 ohms 1 4 watt carbon film resistor Red red black R13 1k 1 4 watt carbon film resistor Brown black red R14 47 1 4 watt carbon film resistor Yellow violet red R15 22k 1 4 watt carbon film resistor Red red red R16 10k 1 4 watt carbon film resistor Brown black orange Ul 17805 Linear vol
17. e apparatus to Lj achieve best overlap coincidence of Figure 6 Correct alignment of Channel 1 and 2 the reference and received pulses oscilloscope traces for proper Speed of Light Apparatus calibration 10 9 Carefully loosen the fiber cinch nuts on LED D3 and Detector D8 and remove the 15 cm length of fiber Measurement Finally we are going to make our speed of light measurement Using the oscilloscope we will measure the time required for the red LED light pulses to travel through 20 meters of plastic fiber 1 Insert one end of the 20 meter plastic fiber gently but firmly into LED D3 until the fiber is seated Lightly finger tighten the fiber optic cinch nut on the LED 2 Insert the other end of the fiber into Detector D8 and lightly tighten the fiber optic cinch nut 3 Observe the display on the CRT screen of the oscilloscope The received pulse should now have moved to the right of the reference pulse with a reduced amplitude of approximately 50 See Figure 7 4 Very carefully measure the time difference between the reference pulse and the delay pulse in nanoseconds ins a E Make the measurement from the Figure 7 Oscilloscope display showing second vertical graticule used in your approximate positions of the reference pulse and initial calibration to the peak of the the received pulse delayed through 20 meters of relocated received pulse that is the Jiber received pulse generated w
18. esidue Soapy water will not harm the components as long as electrical power is not being applied in which case you don t want to get anywhere near water anyway for safety s sake If you used a rosin core solder clean the board with flux remover before washing in soap and water Rinse thoroughly Shake the board to remove water from under the ICs Wipe everything dry with paper towels and let it air dry for 30 minutes Insert D3 and D8 in designated areas on the printed circuit board and secure in place with the 2 56 screws and nuts provided Solder each lead Remove the nut and washer from the potentiometer R8 Insert the shaft of the potentiometer through the bottom of the board aligning the tab on the pot with the hole on the board Use the washer and nut to tighten R8 securely to the board Turn the board over to expose its bottom with the fiber optic emitter D3 and detector D8 pointing away from you Solder a 5 cm 1 5 24 gauge jumper wire from the left pin of the pot to the solder pad just underneath it Solder another jumper of the same length between the pot s middle and right pins then to the open solder pad that is connected to R7 Place the power supply jack onto the printed wiring board and solder all three of its leads into place Apply heat and solder sparingly to prevent the solder from flowing down into the jack The printed wiring board is now assembled and ready for installation in the chassis provided Using the six
19. et Indianapolis IN 1982 Technician s Guide to Fiber Optics Sterling AMP Incorporated Harrisburg PA 17105 1987 Paperback Delmar Publishers 2 Computer Drive West Box 15 015 Albany New York 12212 9985 Hardbound version Fiber Optics Handbook Second Edition Hentschel Hewlett Packard 1988 ADVANCED Fiber Optic Communications Fourth Edition Palais Prentice Hall Publishing 1998 Optical Fiber Transmission Basch Howard W Sams 4300 West 62nd Street Indianapolis IN 1986 COLLEGE LEVEL An Introduction to Optical Fibers Cherin McGraw Hill Book Company 1983 Fiber Optic Handbook for Engineers and Scientists Allard McGraw Hill Publishing New York NY 1990 Fiber Optics James C Daly CRC Press Inc 2000 Corporate Blvd N W Boca Raton FL 1986 Fiber Optics in Communication Systems Elion and Elion Marcel Dekker Inc 1978 Pulse Code Formats for Fiber Optic Communications Morris Marcel Dekker Inc 1983 Optical Fibre Sensing and Signal Processing Culshaw Peter Peregrinus LTD 1984 Principles of Optical Fiber Measurements Marcuse Academic Press 1974 Semiconductor Devices for Optical Communications Kressel Springer Verlag Inc 1980 20 SAFETY Safety with Lasers and Other Optical Sources Stiney and Wolbarsht Plenum Press 1980 Safe Use of Lasers ANSI Standard Z136 1 LIA 12424 Research Parkway Suite 130 Orlando FL 32826 Safe Use of Optical Fiber Communications Systems Utilizing Laser Diodes
20. h greater distance if he hoped to get a second grip on that speeding luminous energy He decided that hilltop to hilltop was a good starting point and that s where he began with himself on one hill and his trusty assistant on another well after the sun had set Each man carried an oil burning lamp with a cover so he could shield the light until needed Galileo uncovered his lamp briefly sending a flash of light over to his assistant The assistant replied with his own quick flash of light back to the boss The exchanges continued that night and many nights more from hilltops increasingly further apart Galileo had hoped to measure the time which elapsed from the moment the lamp shields were uncovered until the light was perceived by his eye Rotten luck He finally decided rightfully that he and his assistant weren t physically up to the challenge of grappling with an item we now know to travel at 186 000 miles per second Incorrectly he determined that light travels at infinite speed Figure 1 Galileo Galilei 1564 1642 The next recorded method of measuring light was that of Frenchman Armande L Fizeau 1819 1896 in 1849 Try to visualize his elaborate apparently unwieldy array of mirrors lenses and a huge rotating cogwheel with 720 teeth designed to measure the speed of light over a distance of 5 39 count em miles But the thing worked Pretty much Fizeau and his apparatus computed
21. hen using the 20 meter optical fiber 5 Write down the result of your measurements from Step 4 It should be between 90 and 110 nanoseconds Speed of Light Calculation We now have just about all the information we need to calculate the speed of light Because the light in our demonstration is traveling through a plastic fiber which is not a vacuum we need to know the index of refraction of the plastic fiber to compensate for the slower light speed As you will recall or at least we hope you recall heh heh from the preceding Background Information sections here the index of refraction of a particular medium equals the speed of light in a vacuum divided by the speed of light in the medium n c v Ahhh you re probably saying to yourself It s all coming back to me now Sure zil Today we won t attempt to measure the index of refraction of the plastic fiber That s a project for another day For now we ll rely on the manufacturer s specifications which say our fiber s refractive index is 1 5 Use the familiar equation nel where c the speed of light in a vacuum n the index of refraction of the plastic fiber l the length of the plastic fiber in meters t the travel time of light through the 20 meter fiber in nanoseconds Now take the measurement number you wrote down and substitute it for t in the equation If the results of your measurement resembled 100 nanoseconds your numbers should
22. ight is impeded less by solid airborne particles light speed increases For most practical purposes we can rate light speed in air versus light speed in a vacuum the same In water however things get relatively sluggish The speed of light is about 25 percent less than in a vacuum n glass light has even a tougher time Its speed drops by about 33 percent compared to its rate in a vacuum To put these relationships into some form of mathematical perspective we utilize the term refractive index or index of refraction which refers to the ratio between the speed of light in a vacuum and its speed in some other medium Here s the equation Light speed in a vacuum Refractive index Light speed in another medium Or massaging things down into more manageable symbols C n V Substituting the numerical values of light speed in air water and glass we would obtain the following refractive indices For air n 1 000 For water n 1 333 For glass 1 50 If we went to five decimal places instead of three we would find the refractive index for air is actually 1 00029 Precise Definitely much more so than in the days of Fizeau not to mention Galileo You ll soon learn how we can measure the speed of light with accuracy that would have astounded those well intentioned gentlemen with their lamps cogwheels and mirrors Fiber Optics Light Meets its Master at Last The modern day technology of fiber optics got
23. ing diode Lig ht Strictly speaking electromagnetic radiation visible to the human eye Commonly the term is applied to electromagnetic radiation with properties similar to those of visible light including the invisible near infrared radiation used in fiber optic systems See also Infrared Lig ht Emitting Diode LED A P N junction semiconductor device that emits incoherent optical radiation when biased in the forward direction Numerical Ape NA The numerical aperture of an optical fiber defines the characteristic of a fiber in terms of its acceptance of impinging light The larger the numerical aperture the greater the ability of a fiber to accept light See also Acceptance angle Critical angle Optoelectronics The field of electronics that deals with LEDs lasers and photodetectors or any other electronic devices that produce respond to or utilize optical radiation Photodetector light detector Photon A unit of electromagnetic radiation Light can be viewed as either a wave or a series of photons Phototransistor transistor that detects light and amplifies the resulting electrical signal Light falling on the base emitter junction generates a current which is amplified internally Simple but slow Refractive index The ratio of the speed of light in a vacuum to the speed of light in a material Abbreviated n Receiver A device that detects an optical signal and converts it into an electric
24. inished soldering Parts Identification All the components required for this apparatus are listed in Table 1 Compare the contents of the kit to the list in the table before you start assembly to ensure all components are present 1 2 Identify all the resistors using the color codes in Table 1 This kit contains six axial leaded ceramic capacitors The values of these capacitors may be denoted by a three digit code or by color bands similar to those on the resistors Two of the capacitors have values of 047 uF They are identified by the code 473 or color bands of yellow violet orange white The other four capacitors have values of 150 pF They are identified by the code 151 or color bands of brown green brown silver 5 Identify all the resistors using the color codes in Table 1 6 Locate diodes D2 D4 D5 D6 and D7 They are the red glass components with a black cathode marking on one end and wire leads protruding from both ends Identify the remaining components shown in Table 1 13 Table 1 Speed of Light Apparatus Parts List Value Description Color Code Q 2N2369 NPN switching transistor 2 205179 NPN wide bandwidth transistor 2 5179 NPN wide bandwidth transistor Q4 2 5179 NPN wide bandwidth transistor D1 Yellow LED D2 1 914 1 4148 Switching diode D3 IF E96 Fiber optic red LED Blue housing pink dot D4 1 1 914 1 4148 Switching diode D5 1 914 1 4148 Switching diod
25. ions and to ready yourself for more advanced studies When you are ready to move on to more sophisticated discussions look for our other study materials and kits specifically designed to make learning both fun and rewarding BACKGROUND INFORMATION The miracles of modern day fiber optic technology didn t simply show up on someone s door step Centuries of curiosity experimentation frustration and perspiration passed before pure science won out over superstition and guesswork A small Italian gentleman was among the first to seek enlightenment about the speed of light The Speed of Light A Centuries Long Quest Scientists and probably even more casual thinkers began speculating about the speed of light centuries ago When you consider that early civilizations often made gods and goddesses out of suns planets and moons it isn t hard to understand their fascination and wonder about one of the most powerful forms of energy in their world One of the first that we know of to ask himself Hmmm wonder how fast that stuff travels was Galileo Galilei 1564 1642 Italian astronomer and physicist the same fellow who dropped objects off the now Leaning Tower of Pisa trying to calculate their rates of fall Galileo scored with the tower business in calculating the fall rates of items as varied as feathers and cannonballs Light was another matter however and he knew he had to attempt his measurements of light speed over a muc
26. light speed at 194 000 miles per second Not bad when you consider the scientific tools available at that time plus the difficulty of the experiment In the years that followed investigators steadily improved on Fizeau s equipment and methods of observation Most notable was the work of American physicist Albert Michelson 1852 1931 who replaced Fizeau s 720 tooth wheel with an eight sided mirror He also increased the measurement distance to 44 miles In 1926 Michelson got a grip on light computed at 299 796 kilometers per second or 186 284 miles per second The quest for precision and the continued refinement of the measurement continued until today really only hard core mathematicians quibble about the number of decimal places we should assign to the speed of light The speed of light in a vacuum is now listed as 299 792 4562 kilometers per second For the purposes of everyday discussion we generally suffice with a figure of 300 million meters per second or 186 000 miles per second Speed Zones Occur When Light Meets Matter Up to this point we ve talked primarily about light traveling through a vacuum such as outer space When light passes through some medium other than a vacuum such as a gas solid or liquid it slows down But often not by much e At sea level light speed through air is only about 70 kilometers less per second than it is in a vacuum At higher altitudes where the air is less dense and where l
27. look something like this E 15 20 m 100 x 10 seconds 3x103 meters second In other words the speed of light Just to make sure you understand why you feel proud about yourself rightfully so for having arrived at the right numbers run back through the preceding Background Information sections If you begin with people s initial curiosity about the speed of light more than 500 years ago you probably can appreciate how far that curiosity and determination and scientific dedication and sudden inspiration have changed our world The demonstration you completed so simply with your Speed of Light Apparatus was founded upon the ae endless questions and eventually scientific explorations of thousands of adventurous people who dared to ask Why KIT ASSEMBLY If you obtained your ndustrial Fiber Optics Speed of Light Apparatus in kit form rather than already assembled at the factory these instructions will explain how to get everything together and ready for operation Tools and equipment required for assembly 25 watt soldering iron Needle nose pliers Single edge razor blade or sharp knife Small standard blade screwdriver Small Phillips screwdriver Small adjustable wrench Solder Water glycerin or light oil Wire cutters Solid core solder is recommended for assembly If rosin core solder is used you may wish to purchase flux remover to make cleaning the board easier after you have f
28. r into heat See also Scattering Acceptance Angle The angle within which an optical fiber will accept light for transmission along its core This angle is measured from the centerline of the core Ang le of Incidence The angle formed between a ray of light striking a surface and a line drawn perpendicular to that surface at the point of incidence the point at which the light ray strikes the surface Angstrom A A unit of length often used to characterize light An Angstrom is equal to 0 1 nm or 10 meters The word is often spelled out as Angstrom s because the special symbol is not available on typewriters and older printers Attenuation Reduction of signal magnitude or loss normally measured in decibels Fiber attenuation normally is measured per unit length in decibels per kilometer Cable single fiber or a bundle sometimes including strengthening strands of opaque material covered by a protective jacket Cladding The layer of glass or other transparent material surrounding the light carrying core of an optical fiber It has a lower refractive index than the core Coatings may be applied over the cladding Connector A device mounted at the end of a fiber optic cable light source receiver or housing that mates to a similar device to couple light optically into and out of optical fibers A connector joins two fiber ends or one fiber end and a light source or detector Core The central part of an optical fiber that ca
29. rries the light Cou pler A device which connects three or more fiber ends dividing one input between two or more outputs or combining two or more inputs into one output Critical Angle The smallest angle of incidence at which light will undergo total internal reflection Detector A device that generates an electrical signal when illuminated by light or infrared radiation The most common in fiber optics are photodiodes photodarlingtons and phototransistors Fall time Typically specified as the time required for a signal to fall from 90 percent to 10 percent of i original negative or positive amplitude See also Rise time ct S Fiber The optical wave guide or light carrying core or conductor Generally refers to the combination of optical core and cladding See also Core Cladding Fiber buffer buffering material that is used to protect an optical fiber s core and cladding from physical damage Fiber optics A branch of optical technology that deals with the transmission of radiant energy through optical waveguides generally made of glass or plastic 22 Infrared Wavelengths of light longer than 750 nm and shorter than 1 mm Infrared radiation cannot be seen but can be felt as heat Transmission of light through glass fibers is best in the region of 800 1600 nm and through plastic fiber in the region of 640 900 nm Jacket layer of material surrounding an optical fiber but not bonded to it LED Light emitt
30. tage regulator 02 TLC555CP CMOS timer U3 7415221 TTL dual monostable 04 DB101 Bridge rectifier H1 2 1 mm power jack H2 Test point white 2 H3 Test point blue 2 H4 Printed wiring board H5 Six inches 24 gauge wire H6 Chassis H7 110 VAC to DC power adapter H8 Knob H9 2 56 machine screw with nut 2 H10 4 40 machine screw with nut H11 4 3 8 sheet metal screws 6 H12 Rubber feet 4 H13 Polishing paper F1 20 meter fiber F2 15 centimeter fiber 14 LHET 2 ide 2015 diio HTS g ar Sere SSeS css T samdo jeujsnpuy snjeseddy jybrq jo paads Figure 8 Printed wiring board legend showing the correct parts placement for assembly of the Speed of Light Apparatus 15 eye odo 109 0001 US 4 td vu 2a TEE 371250 Ziy OSL 4 161 20 m XOL LLY 8 OSL d 92 12251 sen 101 8y AZ a z NS ZH 09 DVA 021 ND 00 1 4 NIH 202v 10180 ht Apparatus i Figure 9 Circuit schematic of the Speed of L 16 Assembly Procedure All components are to be mounted on the side of the blue printed wiring board with the white printing except for R8 All soldering is to
31. tions device Proof of the pudding He was granted a patent for optical telephone system which transmitted voice signals on beams of light through a network of light pipes By the early 1960s scientists most working for the phone companies were right on the doorstep of creating the first fiber optic telephone networks Three components in particular were proving to be increasingly compatible e Small compact Light Emitting Diodes LEDs e asers e Glass optical fibers Researchers from throughout the world put those items through assorted scientific hoops day after day year after year until they arrived at the basis for the largest and most efficient fiber optic telephone communications in existence today In 1976 the Bell System installed a trial fiber optic telephone system and one year later had a commercial system in operation near Chicago The phenomenal reliability of that system was in large part responsible for the rapid acceptance of fiber optic networks today Bell s acceptable percentage of outages or out of operation due to failure time for its existing wire and microwave carrier system was 02 percent The new fiber optic set up even while the bugs were still being removed had a downtime average of 0001 percent Small wonder that engineers and financiers alike started thinking Fiber optics hmmm sound good sound very good Optical Fiber The Workhorse Today Optic fibers are usually made of plasti
32. ve The amount that light bends depends partly on two materials having different refractive indices as in optical fiber but it also depends on the angle at which the light ray strikes the boundary between the two materials That incoming light ray is known as the incident ray and the outgoing light ray which bounces off the surface is known as the reflected ray Mr Snell his full name was Willebrod Snell van Royen a Dutch mathematician birth date unknown explained in 1621 how light is bent by explaining the relationship between angles of incidence and angles of transmission Figure 4 depicts these two angles Note that both angles are measured from a line drawn perpendicular to the surface at the point where the incident ray strikes Here s the equation 1 sin 0 1 sin 0 The 7 and 1 are the respective refractive indices of the two materials involved in an optical fiber these would be the refractive indices of the core and cladding 0 is the angle of incidence is the angle of transmission Snell s Law isn t limited to the bending of light though It also helps explain Figure 4 Ray of light traveling through two materials how light can be reflected from surface That s handy for us because if light couldn t be reflected our optical fiber would be just so much excess hose rather than the communications wonder it is When an incident light ray strikes the boundary surface between our two
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