PASCO scientific 080187 Gun Diode Microwave Transmitter User Manual 012 04630G cov p65

PASCO scientific Gun Diode Microwave Transmitter 012 04630G cov p65

Users Manual

012-04630GMICROWAVE OPTICSInstruction Manual andExperiment Guide forthe PASCO scientificModel WA-9314BIncludesTeacher's NotesandTypicalExperiment ResultsPhone (916) 786-3800  FAX (916) 786-8905  web: www.pasco.com10101 Foothills Blvd.  Roseville, CA 95678-9011 USA®betterteach scienceways to
i012-04630G Microwave OpticsTable of ContentsSection PageCopyright, Warranty, and Equipment Return ................................................... iiIntroduction ...................................................................................................... 1Equipment......................................................................................................... 1Initial Setup ...................................................................................................... 3Accessory Equipment ....................................................................................... 3Assembling Equipment for Experiments.......................................................... 5ExperimentsExperiment 1: Introduction to the System ............................................ 7Experiment 2: Reflection ................................................................... 11Experiment 3: Standing Waves - Measuring Wavelengths ............... 13Experiment 4: Refraction Through a Prism ....................................... 17Experiment 5: Polarization ................................................................ 19Experiment 6: Double-Slit Interference ............................................ 21Experiment 7: Lloyds Mirror............................................................. 23Experiment 8: Fabry-Perot Interferometer ........................................ 25Experiment 9: Michelson Interferometer .......................................... 27Experiment 10: Fiber Optics.............................................................. 29Experiment 11: Brewster's Angle ...................................................... 31Experiment 12: Bragg Diffraction ..................................................... 33Teacher's Guide .............................................................................................. 35Appendix ........................................................................................................ 45Schematic Diagrams ....................................................................................... 46Replacement Parts List ................................................................................... 47➤➤➤➤➤ This device complies with Part 15 of the FCC Rules. Operation is subject to thefollowing two conditions:1. this device may not cause harmful interference. 2. this device must accept any interference received, including interference that maycause undesired operation.Changes or modifications not expressly approved by Pasco Scientific could void the user's author-ity to operate the equipment.
iiMicrowave Optics 012-04630GCopyright NoticeThe PASCO scientific 012-04630E Model WA-9314BMicrowave Optics manual is copyrighted and all rightsreserved. However, permission is granted to non-profiteducational institutions for reproduction of any part of themanual providing the reproductions are used only for theirlaboratories and are not sold for profit. Reproductionunder any other circumstances, without the writtenconsent of PASCO scientific, is prohibited.Limited WarrantyPASCO scientific warrants the product to be free fromdefects in materials and workmanship for a period of oneyear from the date of shipment to the customer. PASCOwill repair or replace at its option any part of the productwhich is deemed to be defective in material or workman-ship. The warranty does not cover damage to the productcaused by abuse or improper use. Determination ofwhether a product failure is the result of a manufacturingdefect or improper use by the customer shall be madesolely by PASCO scientific. Responsibility for the returnof equipment for warranty repair belongs to the customer.Equipment must be properly packed to prevent damageand shipped postage or freight prepaid. (Damage causedby improper packing of the equipment for return shipmentwill not be covered by the warranty.) Shipping costs forreturning the equipment after repair will be paid byPASCO scientific.Copyright, Warranty, and Equipment ReturnPlease—Feel free to duplicate this manualsubject to the copyright restrictions below.Equipment ReturnShould the product have to be returned to PASCOscientific for any reason, notify PASCO scientific byletter, phone, or fax BEFORE returning the product. Uponnotification, the return authorization and shippinginstructions will be promptly issued. ➤ ➤ ➤ ➤ ➤ NOTE: NO EQUIPMENT WILL BE ACCEPTED FOR RETURN WITHOUT AN AUTHORIZATION FROM PASCO.When returning equipment for repair, the units must bepacked properly. Carriers will not accept responsibility fordamage caused by improper packing. To be certain theunit will not be damaged in shipment, observe the follow-ing rules:➀The packing carton must be strong enough for theitem shipped.➁Make certain there are at least two inches ofpacking material between any point on theapparatus and the inside walls of the carton.➂Make certain that the packing material cannot shiftin the box or become compressed, allowing theinstrument come in contact with the packingcarton.Address: PASCO scientific10101 Foothills Blvd.Roseville, CA 95747-7100Phone: (916) 786-3800FAX: (916) 786-3292email: techsupp@pasco.comweb: www.pasco.comCreditsThis manual edited by: Dave GriffithTeacher’s guide written by: Eric Ayars
1012-04630G Microwave OpticsMicrowave Transmitter with Power SupplyIntroductionGUNN DIODEMICROWAVETRANSMITTERPAS CO scientificGunn Diode TransmitterThe Gunn Diode Microwave Transmitter provides 15 mWof coherent, linearly polarized microwave output at awavelength of 2.85 cm. The unit consists of a Gunn di-ode in a 10.525 GHz resonant cavity, a microwave hornto direct the output, and an 18 cm stand to help reducetable top reflections. The Transmitter may be powereddirectly from a standard 115 or 220/240 VAC, 50/60 Hzoutlet by using the provided power supply. Other featuresinclude an LED power-indicator light and a rotationalscale that allows easy measurement of the angle of po-larization.The Gunn diode acts as a non-linear resistor that oscillatesin the microwave band. The output is linearly polarizedalong the axis of the diode and the attached horn radiatesa strong beam of microwave radiation centered along theaxis of the horn.To Operate the Microwave TransmitterSimply plug the power supply into the jack on theTransmitter's bottom panel and plug the power supply intoa standard 115 or 220/240 VAC, 50/60 Hz outlet. TheLED will light indicating the unit is on.➤➤➤➤➤ CAUTION: The output power of the MicrowaveTransmitter is well within standard safety levels.Nevertheless, one should never look directly into themicrowave horn at close range when the Transmit-ter is on.Power Supply Specifications:9 Volt DC, 500 mA;Miniature Phone Jack Connector (the tip is positive)EquipmentThere are many advantages to studying optical phenom-ena at microwave frequencies. Using a 2.85 centimetermicrowave wavelength transforms the scale of the experi-ment. Microns become centimeters and variables ob-scured by the small scale of traditional optics experimentsare easily seen and manipulated. The PASCO scientificModel WA-9314B Basic Microwave Optics System isdesigned to take full advantage of these educational ben-efits. The Basic Microwave Optics System comes with a2.85 centimeter wavelength microwave transmitter and areceiver with variable amplification (from 1X to 30X).All the accessory equipment needed to investigate a vari-ety of wave phenomena is also included.This manual describes the operation and maintenance ofthe microwave equipment and also gives detailed instruc-tions for many experiments. These experiments rangefrom quantitative investigations of reflection and refrac-tion to microwave models of the Michelson and Fabry-Perot interferometers. For those who have either theComplete Microwave Optics System (WA-9316) or theMicrowave Accessory Package (WA-9315), the manualdescribes experiments for investigating Bragg diffractionand Brewster's angle.
2012-04630GMicrowave OpticsMicrowave ReceiverMicrowave ReceiverThe Microwave Receiver provides a meter reading that,for low amplitude signals, is approximately proportionalto the intensity of the incident microwave signal. A mi-crowave horn identical to that of the Transmitter's collectsthe microwave signal and channels it to a Schottky diodein a 10.525 GHz resonant cavity. The diode respondsonly to the component of a microwave signal that is polar-ized along the diode axis, producing a DC voltage thatvaries with the magnitude of the microwave signal.Special features of the Receiver include four amplificationranges—from one to thirty—with a variable sensitivityknob that allows fine tuning of the amplification in eachrange. For convenience in class demonstrations, bananaplug connectors provide for an output signal via hookupto a projection meter (such as PASCO Model ES-9065Projection Meter or SE-9617 DC Voltmeter). This outputcan also be used for close examination of the signal usingan oscilloscope. The receiver is battery powered and hasan LED battery indicator; if the LED lights when you turnon the Receiver , the battery is working. As with theTransmitter, an 18 cm high mount minimizes table topreflections, and a rotational scale allows convenient mea-surements of polarization angle.The female audio connector on the side of the Receiver isfor an optional Microwave Detector Probe ( PASCOModel WA-9319). The probe works the same as the Re-ceiver except it has no horn or resonant cavity. The Probeis particularly convenient for examining wave patterns inwhich the horn could get in the way, such as the standingwave pattern described in Experiment 3 of this manual.➤➤➤➤➤NOTE: The detector diodes in the Receiver (andthe Probe) are non-linear devices. This non-linear-ity will provide no problem in most experiments. Itis important however, to realize that the meter read-ing is not directly proportional to either the electricfield (E) or the intensity (I) of the incident micro-wave. Instead, it generally reflects some intermedi-ate value.To Operate The Microwave Receiver:➤➤➤➤➤NOTE: Before using the Receiver, you will needto install the two 9-volt transistor batteries—they areincluded with the system. See the instructions in theMaintenance section at the end of this manual.①Turn the INTENSITY selection switch from OFF to30X, the lowest amplification level. The battery indi-cator LED should light, indicating that the battery isokay. If it does not, replace the battery following theprocedures in the Maintenance section of this manual.➤➤➤➤➤NOTE: The INTENSITY selection settings (30X,10X, 3X, 1X) are the values you must multiply themeter reading by to normalize your measurements.30X, for example, means that you must multiply themeter reading by 30 to get the same value youwould measure for the same signal with the INTEN-SITY selection set to 1X. Of course, this is trueonly if you do not change the position of the VARI-ABLE SENSITIVITY knob between measurements.②Point the microwave horn toward the incident micro-wave signal. Unless polarization effects are under in-vestigation, adjust the polarization angles of the Trans-mitter and Receiver to the same orientation (e.g., bothhorns vertically, or both horns horizontally).③Adjust the VARIABLE SENSITIVITY knob to attaina meter reading near midscale. If no deflection of themeter occurs, increase the amplification by turning theINTENSITY selection switch clockwise. Remember,always multiply your meter reading by the appropriateINTENSITY selection (30X, 10X, 3X, or 1X) if youwant to make a quantitative comparison of measure-ments taken at different INTENSITY settings.
3012-04630G Microwave OpticsInitial SetupAttaching the Transmitter and Receiver StandsHand ScrewWashersFixed Arm Assembly (1)Goniometer (1)Accessory equipment for the Basic Microwave OpticsSystem includes:Rotating Component Holder (1)Component Holder (2)ROTATING TABLERotating Table (1)Accessory EquipmentTo attach the microwave Transmitter and Receiver to theirrespective stands prior to performing experiments, pro-ceed as follows:①Remove the black hand screw from the back panel ofboth the Transmitter and the Receiver.②Attach both units to the stands as shown below. Ob-serve the location of the washers.③To adjust the polarization angle of the Transmitteror Receiver, loosen the hand screw, rotate the unit,and tighten the hand screw at the desired orientation.Notice the rotational scale on the back of each unit formeasuring the angle of polarization. Be aware, how-ever, that since the Transmitter and Receiver face eachother in most experiments it is important to match theirpolarization angle. If you rotate one unit to an angle of10-degrees, you must rotate the other to -10-degrees(350-degrees) to achieve the proper polar alignment.
4012-04630GMicrowave OpticsWide Slit Spacer (1)Narrow Slit Spacer (1) Slit Extender Arm (1)Metal Reflector (2)Partial Reflector (2)Polarizers (2)TubularPlastic Bags (4)Ethafoam Prism Mold w/Styrene Pellets (1)Polyethylene Panel (1)Cubic Lattice with 100 metalspheres—5x5x4 array (1)The WA-9315 Microwave Accessory Package (which ispart of the Complete Microwave Optics System ModelWA-9316) includes the following:The following components, compatible with the WA-9314B Basic Microwave Optics System, are availablefrom PASCO scientific:Model WA-9319 Microwave Detector Probe plugs di-rectly into the Microwave Receiver. The probe is essen-tial for experiments in which the horn of the Receivermight otherwise interfere with the wave pattern beingmeasured.Model WA-9318 Microwave Modulation Kit includes amodulator and microphone. With this kit, you can useyour Transmitter and Receiver as a microwave communi-cations system.
5012-04630G Microwave OpticsAssembling Equipment for ExperimentsThe arms of the Goniometer slide through the holes in theComponent Holders as shown. Make sure the magneticstrip on the bottom of the arm grips the base of the car-riage. To adjust the position of the holders, just slidethem along the Goniometer arms. Attach the mountingstands of the microwave Transmitter and Receiver to thearms of the Goniometer in the same manner.For most experiments it is advantageous to attach theTransmitter to the long arm of the Goniometer and theReceiver to the shorter, rotatable arm. This maintains afixed relationship between the microwave beam and com-ponents mounted on the long arm (or on the degree plate)of the Goniometer. In turn the Receiver moves easily tosample the output.Reflectors, Partial Reflectors, Polarizers, Slit Spacers, andthe Slit Extender Arm all attach magnetically to the Com-ponent Holders. The metric scale along the Goniometerarms and the degree plate at the junction of the arms al-low easy measurement of component placement. Whenrotating the rotatable arm, hold the degree plate firmly tothe table so that it does not move.➤➤➤➤➤IMPORTANT NOTES:1. CAUTION—Under some circumstances, microwaves can interfere with elec-tronic medical devices. If you use a pacemaker, or other electronic medicaldevice, check with your doctor or the manufacturer to be certain that low powermicrowaves at a frequency of 10.525 GHz will not interfere with its operation.2. Always mount the apparatus on a CLEAN, SMOOTH table. Before setting upthe equipment, brush off any material—particularly metal chips—that mighthave adhered to the magnetic strips on the bottom of the Goniometer arms.Mounting the Component Holder
6012-04630GMicrowave OpticsCopy-Ready ExperimentsThe following Experiments provide a thorough introduction to wave theory usingthe microwave system. We expect that the student approaches each experimentwith the appropriate theoretical background, therefore, basic principles are onlybriefly discussed in each experiment.The experiments are written in worksheet format. Feel free to photocopy them foruse in your lab.
7012-04630G Microwave OpticsEQUIPMENT NEEDED:– Transmitter – Goniometer– Receiver – Reflector (1)PurposeThis experiment gives a systematic introduction to the Microwave Optics System. This mayprove helpful in learning to use the equipment effectively and in understanding the significance ofmeasurements made with this equipment. It is however not a prerequisite to the following experi-ments.Procedure①Arrange the Transmitter and Receiver on the Goni-ometer as shown in Figure 1.1 with the Transmitterattached to the fixed arm. Be sure to adjust bothTransmitter and Receiver to the same polarity—thehorns should have the same orientation, as shown.②Plug in the Transmitter and turn the INTENSITYselection switch on the Receiver from OFF to 10X.(The LEDs should light up on both units.)③ Adjust the Transmitter and Receiver so the distancebetween the source diode in theTransmitter and the detector diodein the Receiver (the distance la-beled R in Figure 1.1) is 40 cm(see Figure 1.2 for location ofpoints of transmission and recep-tion). The diodes are at the loca-tions marked "T" and "R" on thebases. Adjust the INTENSITY andVARIABLE SENSITIVITY dialson the Receiver so that the meterreads 1.0 (full scale).④Set the distance R to each of thevalues shown in Table 1.1. For eachvalue of R, record the meter reading.(Do not adjust the Receiver controlsbetween measurements.) After mak-ing the measurements, perform thecalculations shown in the table.⑤Set R to some value between 70 and90 cm. While watching the meter,slowly decrease the distance betweenthe Transmitter and Receiver. Doesthe meter deflection increase steadilyas the distance decreases?Experiment 1: Introduction to the SystemRFigure 1.1 Equipment Setup5 cm 5 cmTransmitter ReceiverEffective Point of Reception ofTransmitter SignalEffective Point of Emission ofTransmitter SignalFigure 1.2 Equipment SetupR(cm) Meter Reading (M) M X R(cm)M X R2(cm2)4050607080901001.0 40 1600Table 1.1
8012-04630GMicrowave Optics⑥Set R to between 50 and 90 cm. Move a Reflector, its plane parallel to the axis of the microwavebeam, toward and away from the beam axis, as shown in Figure 1.3. Observe the meter read-ings. Can you explain your observations in steps 5 and 6? Don’t worry if you can’t; you willhave a chance to investigate these phenomena moreclosely in Experiments 3 and 8, later in this manual. Fornow just be aware of the following:➤➤➤➤➤IMPORTANT: Reflections from nearby objects, in-cluding the table top, can affect the results of your mi-crowave experiments. To reduce the effects of extrane-ous reflections, keep your experiment table clear of allobjects, especially metal objects, other than those com-ponents required for the current experiment.⑦Loosen the hand screw on the back of the Receiver androtate the Receiver as shown in Figure 1.4. This variesthe polarity of maximum detection. (Look into thereceiver horn and notice the alignment of the detectordiode.) Observe the meter readings through a full 360degree rotation of the horn. A small mirror may behelpful to view the meter reading as the receiver isturned. At what polarity does the Receiver detect nosignal?Try rotating the Transmitter horn as well. When fin-ished, reset the Transmitter and Receiver so their polari-ties match (e.g., both horns are horizontal or both hornsare vertical).⑧Position the Transmitter so the output surface of the hornis centered directly over the center of the Degree Plate ofthe Goniometer arm (see Figure 1.5). With the Receiverdirectly facing the Transmitter and as far back on theGoniometer arm as possible, adjust the Receiver controlsfor a meter reading of 1.0. Then rotate the rotatable armof the Goniometer as shown in the figure. Set the angleof rotation (measured relative to the 180-degree point onthe degree scale) to each ofthe values shown in Table1.2, and record the meterreading at each setting.Figure 1.5 Signal DistributionFigure 1.3 ReflectionsReflectorFigure 1.4 PolarizationHandscrewTable 1.2MeterReadingAngle ofReceiver0°10°20°30°40°50°MeterReadingAngle ofReceiver70°80°90°100°110°120°MeterReadingAngle ofReceiver140°150°160°170°180°60° 130°
9012-04630G Microwave OpticsQuestions①The electric field of an electromagnetic wave is inversely proportional to the distance fromthe wave source(i.e., E = 1/R). Use your data from step 4 of the experiment to determine if the meter read-ing of the Receiver is directly proportional to the electric field of the wave.②The intensity of an electromagnetic wave is inversely proportional to the square of the distancefrom the wave source (i.e., I = 1/R2). Use your data from step 4 of the experiment to determineif the meter reading of the Receiver is directly proportional to the intensity of the wave.③Considering your results in step 7, to what extent can the Transmitter output be considered aspherical wave? - A plane wave?
10012-04630GMicrowave OpticsNotes
11012-04630G Microwave OpticsExperiment 2: ReflectionEQUIPMENT NEEDED:– Transmitter – Goniometer– Receiver – Metal Reflector– Rotating Component HolderProcedure①Arrange the equipment as shown in figure 2.1with the Transmitter attached to the fixed armof the Goniometer. Be sure to adjust the Trans-mitter and Receiver to the same polarity; thehorns should have the same orientation asshown.②Plug in the Transmitter and turn the ReceiverINTENSITY selection switch to 30X.③The angle between the incident wave from theTransmitter and a line normal to the plane ofthe Reflector is called the Angle of Incidence(see Figure 2.2). Adjust the Rotating Compo-nent Holder so that the Angle of Incidenceequals 45-degrees.④Without moving the Transmitter or the Reflec-tor, rotate the movable arm of the Goniometeruntil the meter reading is a maximum. Theangle between the axis of the Receiver horn anda line normal to the plane of the Reflector iscalled the Angle of Reflection.⑤Measure and record the angle of reflection foreach of the angles of incidence shown in Table 2.1.➤NOTE: At various angle settings the Receiver willdetect both the reflected wave and the wave comingdirectly from the Transmitter, thus giving misleadingresults. Determine the angles for which this is trueand mark the data collected at these angles with anasterisk "*".Figure 2.1 Equipment SetupFigure 2.2 Angles of Incidence and ReflectionAngle ofIncidenceAngle ofReflectionReflectorAngle ofIncidence20°30°40°50°60°Angle ofReflection70°80°90°Table 2.1
12012-04630GMicrowave OpticsQuestions①What relationship holds between the angle of incidence and the angle of reflection? Does this rela-tionship hold for all angles of incidence?②In measuring the angle of reflection, you measured the angle at which a maximum meter readingwas found. Can you explain why some of the wave reflected into different angles? How does thisaffect your answer to question 1?③Ideally you would perform this experiment with a perfect plane wave, so that all the Transmitterradiation strikes the Reflector at the same angle of incidence. Is the microwave from the Transmittera perfect plane wave (see Experiment 1, step 7)? Would you expect different results if it were aperfect plane wave? Explain.Questions for Additional Experimentation①How does reflection affect the intensity of the microwave? Is all the energy of the wave striking theReflector reflected? Does the intensity of the reflected signal vary with the angle of incidence?②Metal is a good reflector of microwaves. Investigate the reflective properties of other materials.How well do they reflect? Does some of the energy pass through the material? Does the materialabsorb some of it? Compare the reflective properties of conductive and non-conductive materials.
13012-04630G Microwave OpticsExperiment 3: Standing Waves - Measuring Wavelengths➤➤➤➤➤ NOTE: This experiment is best performed using the PASCO Microwave Detector Probe(Model ME-9319), as described in Method A below. However, for those without aprobe, Method B may be used, although in this Method λ can not be measured directlyfrom the standing wave pattern.EQUIPMENT NEEDED:– Transmitter – Goniometer– Receiver – Reflector (1)– Component Holder (2) – Microwave Detector Probe (ME-9319 )IntroductionWhen two electromagnetic waves meet in space, they superpose. Therefore, the total electricfield at any point is the sum of the electric fields created by both waves at that point. If thetwo waves travel at the same frequency but in opposite direction they form a standing wave.Nodes appear where the fields of the two waves cancel and antinodes where the superposedfield oscillates between a maximum and a minimum. The distance between nodes in thestanding wave pattern is just 1/2 the wavelength (λ) of the two waves.ProcedureMethod AIn this experiment, you will reflect the wavefrom the Transmitter back upon itself, creatinga standing wave pattern. By measuring thedistance between nodes in the pattern and mul-tiplying by two, you can determine the wave-length of the microwave radiation.①Arrange the equipment as shown in Figure 3.1.②Plug the Detector Probe into the side connectoron the Receiver. Face the Receiver horn di-rectly away from the Transmitter so that noneof the microwave signal enters the horn. Adjustthe Receiver controls as needed to get a strongmeter reading.③Slide the Probe along the Goniometer arm (no more than a centimeter or two) until the metershows a maximum reading. Then slide the Reflector (again, no more than a centimeter ortwo) to find a maximum meter reading. Continue making slight adjustments to the Probeand Reflector positions until the meter reading is as high as possible.④Now find a node of the standing wave pattern by adjusting the Probe until the meter readingis a minimum. Record the Probe Position along the metric scale on the Goniometer arm.Initial Probe Position = _____________________.Figure 3.1 Equipment SetupReceiverReflectorDetector Probe
14012-04630GMicrowave Optics⑤While watching the meter, slide the Probe along the Goniometer arm until the Probehas passed through at least 10 antinodes and returned to a node. Record the newposition of the Probe and the number of antinodes that were traversed.Antinodes Traversed= __________________________.Final Probe Position = _________________________.⑥Use your data to calculate λ, the wavelength of the microwave radiation.λ =_________________________.⑦Repeat your measurements and recalculate λ.Initial Probe Position =_________________________.Antinodes Traversed =_________________________.Final Probe Position =_________________________.λ =_________________________.Questions①Use the relationship velocity = λν to calculate the frequency of the microwave signal(assuming velocity of propagation in air is 3x108 m/sec).(ν = the expected frequency of the microwave radiation -10.525 GHz).Method B①Set up the equipment as shown in Figure 3.2. Adjust the Receiver controls to get afull-scale meter reading with the Transmitter and Receiver as close together as pos-sible. Slowly move the Receiver along the Goniometer arm, away from the Trans-mitter. How does this motion effect the meter reading?The microwave horns are not perfect collectors of microwave radiation. Instead, theyact as partial reflectors, so that the radiation from the Transmitter reflects back andforth between the Transmitter and Reflector horns, diminishing in amplitude at eachpass. However, if the distance between the Transmitter and Receiver diodes is equalto nλλλλλ/2, (where n is an integer and λ is the wavelength of the radiation) then all themultiply-reflected waves entering the Receiver horn will be in phase with the primarytransmitted wave. When this occurs, the meter reading will be a maximum. (Thedistance between adjacent positions in order to see a maximum is therefore λλλλλ/2.)②Slide the Receiver one or two centime-ters along the Goniometer arm to ob-tain a maximum meter reading.Record the Receiver position along themetric scale of the Goniometer arm.Initial Position of Receiver =_________________________.Figure 3.2 Equipment Setup
15012-04630G Microwave Optics③While watching the meter, slide the Receiver away from the Transmitter. Do not stopuntil the Receiver passed through at least 10 positions at which you see a minimum meterreading and it returned to a position where the reading is a maximum. Record the newposition of the Receiver and the number of minima that were traversed.Minima Traversed= _________________________.Final Receiver Position = _________________________.④Use the data you have collected to calculate the wavelength of the microwave radiation.λ = _________________________.⑤Repeat your measurements and recalculate λ.Initial Position of Receiver = _________________________.Minima Traversed = _________________________.Final Receiver Position = _________________________.λ = _________________________.Questions①Use the relationship velocity = λν to calculate the frequency of the microwave signal(assuming velocity of propagation in air is 3x108 m/sec).(ν = the expected frequency of the microwave radiation -10.525 GHz).
16012-04630GMicrowave OpticsNotes
17012-04630G Microwave OpticsExperiment 4: Refraction Through a PrismEQUIPMENT NEEDED:– Transmitter– Goniometer– Receiver– Rotating Table– Ethafoam Prism mold with styrene pellets– ProtractorIntroductionAn electromagnetic wave usually travels in astraight line. As it crosses a boundary betweentwo different media, however, the direction ofpropagation of the wave changes. This changein direction is called Refraction, and it is sum-marized by a mathematical relationship knownas the Law of Refraction (otherwise known asSnell’s Law):n1sinθθθθθ1 = n2sinθθθθθ2;where θθθθθ1 is the angle between the direction of propagation of the incident wave and thenormal to the boundary between the two media, and θ2 is the corresponding angle for therefracted wave (see Figure 4.1). Every material can be described by a number n, calledits Index of Refraction. This number indicates the ratio between the speed ofelectromegnetic waves in vacuum and the speed of electromagnetic waves in the material,also called the medium. In general, the media on either side of a boundary will have dif-ferent indeces of refraction. Here they are labeled n1 and n2. It is the difference betweenindeces of refraction (and the difference between wave velocities this implies) whichcauses “bending”, or refraction of a wave as it crosses the boundary between two distinctmedia.In this experiment, you will use the law of refraction to measure the index of refrac-tion for styrene pellets.Procedure①Arrange the equipment as shown in Figure 4.2. Rotate the empty prism mold and seehow it effects the incident wave. Does itreflect, refract, or absorb the wave?②Fill the prism mold with the styrene pellets.To simplify the calculations, align the face ofthe prism that is nearest to the Transmitterperpendicular to the incident microwavebeam.③Rotate the movable arm of the Goniometerand locate the angle θ at which the refractedsignal is a maximum.n1 n2Boundary betweenmediaRefractedWaveIncidentWaveθ1θ2Figure 4.1 Angles of Incidence and RefractionEthafoam PrismRotating TableFigure 4.2 Equipment Setup
18012-04630GMicrowave OpticsRefractedBeamNormal toBoundary ofRefractionθ2θθ1Figure 4.3 Geometry of Prism RefractionIncidentBeam➤ NOTE: θ is just the angle that you read directlyfrom the Degree Scale of the Goniometer.θ = _________________________.④Using the diagram shown in Figure 4.3, determine θ1and use your value of θ to determine θ2. (You willneed to use a protractor to measure the Prism angles.)θ1 = _________________________.θ2 = _________________________.⑤Plug these values into the Law of Refraction todetermine the value of n1/n2.n1/n2 = _________________________.⑥The index of refraction for air is equal to 1.00. Use this fact to determine n1, the index ofrefraction for the styrene pellets.Questions①In the diagram of Figure 4.3, the assumption is made that the wave is unrefracted when itstrikes the first side of the prism (at an angle of incidence of 0°). Is this a valid assumption?②Using this apparatus, how might you verify that the index of refraction for air is equal to one.③Would you expect the refraction index of the styrene pellets in the prism mold to be the same asfor a solid styrene prism?
19012-04630G Microwave OpticsExperiment 5: PolarizationEQUIPMENT NEEDED:-Transmitter -Receiver-Goniometer -Component Holder (1)-Polarizer (1).IntroductionThe microwave radiation from the Transmitter is linearlypolarized along the Transmitter diode axis (i.e., as theradiation propagates through space, its electric field re-mains aligned with the axis of the diode). If the Trans-mitter diode were aligned vertically, the electric field ofthe transmitted wave would be vertically polarized, asshown in Figure 5.1. If the detector diode were at anangle θ to the Transmitter diode, as shown in Figure 5.2,it would only detect the component of the incident elec-tric field that was aligned along its axis. In this experi-ment you will investigate the phenomenon of polariza-tion and discover how a polarizer can be used to alter thepolarization of microwave radiation.Procedure①Arrange the equipment as shown in Figure 5.3 andadjust the Receiver controls for nearly full-scalemeter deflection.②Loosen the hand screw on the back of the Receiverand rotate the Receiver in increments of ten de-grees. At each rotational position, record the meterreading in Table 5.1.③What happens to the meter readings if you continueto rotate the Receiver beyond 180-degrees?Figure 5.2 Detecting Polarized RadiationComponentDetectedθVerticallyPolarizedMicrowaveDetectorDiodeFigure 5.1 Vertical PolarizationTransmitterDiodeVerticallyPolarizedMicrowaves(E field)Figure 5.3 Equipment SetupMeterReadingAngle ofReceiver0°10°20°30°40°50°MeterReadingAngle ofReceiver70°80°90°100°110°120°MeterReadingAngle ofReceiver140°150°160°170°180°60° 130°Table 5.1
20012-04630GMicrowave Optics④Set up the equipment as shown in Figure 5.4. Resetthe Receivers angle to 0-degrees (the horns shouldbe oriented as shown with the longer side horizon-tal).⑤Record the meter reading when the Polarizer is alignedat 0, 22.5, 45, 67.5 and 90-degrees with respect to thehorizontal.⑥Remove the Polarizer slits. Rotate the Receiver so theaxis of its horn is at right angles to that of the Transmit-ter. Record the meter reading. Then replace the Polar-izer slits and record the meter readings with the Polarizer slits horizontal, vertical, and at 45-Figure 5.4 Equipment SetupAngle ofSlitsHorizontalVertical45°Meter ReadingAngle ofPolarizer0° (Horiz.)22.5°45°67.5°90° (Vert.)Meter Readingdegrees.Questions①If the Receiver meter reading (M) were directly proportional to the electric field component(E) along its axis, the meter would read the relationship M = Mocosθθθθθ (where θθθθθ is the anglebetween the detector and Transmitter diodes and Mo is the meter reading when θθθθθ = 0). (SeeFigure 5.2). Graph your data from step 2 of the experiment. On the same graph, plot therelationship Mo cosθθθθθ. Compare the two graphs.②The intensity of a linearly polarized electromagnetic wave is directly proportional to the square ofthe electric field (e.g., I = kE2 ). If the Receiver’s meter reading was directly proportional to theincident microwave’s intensity, the meter would read the relationship M = Mocos2θθθθθ. Plot this rela-tionship on your graph from question 1. Based on your graphs, discuss the relationship between themeter reading of the Receiver and the polarization and magnitude of the incident microwave.③Based on your data from step 5, how does the Polarizer affect the incident microwave?④Can you explain the results of step 6 of the experiment. How can the insertion of an additional po-larizer increase the signal level at the detector? ( HINT: Construct a diagram like that shown inFigure 5.2 showing (1) the wave from the Transmitter; (2) the wave after it passes through the Polar-izer; and (3) the component detected at the detector diode.)
21012-04630G Microwave OpticsExperiment 6: Double-Slit InterferenceEQUIPMENT NEEDED:- Transmitter, Receiver - Goniometer, Rotating- Component Holder - Metal Reflectors (2)- Slit Extender Arm - Narrow Slit Spacer- Wide Slit SpacerIntroductionIn Experiment 3, you saw how two waves moving inopposite directions can superpose to create a standingwave pattern. A somewhat similar phenomenonoccurs when an electromagnetic wave passes througha two-slit aperture. The wave diffracts into twowaves which superpose in the space beyond the aper-tures. Similar to the standing wave pattern, there arepoints in space where maxima are formed and otherswhere minima are formed.With a double slit aperture, the intensity of the wavebeyond the aperture will vary depending on the angleof detection. For two thin slits separated by a dis-tance d, maxima will be found at angles such thatd sinθθθθθ = nλλλλλ. (Where θθθθθ = the angle of detection, λλλλλ = the wavelength of the incident radiation,and n is any integer) (See Figure 6.1). Refer to a textbook for more information about the natureof the double-slit diffraction pattern.Procedure①Arrange the equipment as shown in Figure 6.2. Usethe Slit Extender Arm, two Reflectors, and the Nar-row Slit Spacer to construct the double slit. (Werecommend a slit width of about 1.5 cm.) Be precisewith the alignment of the slit and make the setup assymmetrical as possible.②Adjust the Transmitter and Receiver for vertical po-larization (0°) and adjust the Receiver controls to givea full-scale reading at the lowest possible amplifica-tion.③Rotate the rotatable Goniometer arm (on which theReceiver rests) slowly about its axis. Observe the meter readings.④Reset the Goniometer arm so the Receiver directly faces the Transmitter. Adjust the Receivercontrols to obtain a meter reading of 1.0. Now set the angle θθθθθ to each of the values shown inTable 6.1. At each setting record the meter reading in the table. (In places where the meter read-ing changes significantly between angle settings, you may find it useful to investigate the signallevel at intermediate angles.)Figure 6.1 Double-Slit InterferencedθFigure 6.2 Equipment Setup
22012-04630GMicrowave Optics⑤Keep the slit widths the same, but changethe distance between the slits by using theWide Slit Spacer instead of the NarrowSlit Spacer. Because the Wide Slit Spaceis 50% wider than the Narrow Slit Spacer(90mm vs 60mm) move the Transmitterback 50% so that the microwave radiationat the slits will have the same relativeintensity. Repeat the measurements.(You may want to try other slit spacings aswell.)Questions①From your data, plot a graph of meterreading versus θθθθθ. Identify the angles atwhich the maxima and minima of theinterference pattern occur.②Calculate the angles at which you would expect the maxima and minima to occur in a standard two-slit diffraction pattern—maxima occur wherever d sinθθθθθ = nλλλλλ, minima occur whereverd sinθθθθθ = nλλλλλ/2. (Check your textbook for the derivation of these equations, and use the wavelengthmeasured in experiment 3.) How does this compare with the locations of your observed maxima andminima? Can you explain any discrepancies? (What assumptions are made in the derivations of theformulas and to what extent are they met in this experiment?)③Can you explain the relative drop in intensity for higher order maxima? Consider the single-slit dif-fraction pattern created by each slit. How do these single slit patterns affect the overall interferencepattern?➤➤➤➤➤NOTE:① Wavelength at 10.525 GHz = 2.85 cm.② The experimenter’s body position may affect the results.Angle Meter Reading45°50°55°60°65°Angle Meter Reading0°5°10°15°20°25°30°35°40°70°75°80°85°Table 6.1
23012-04630G Microwave OpticsExperiment 7: Lloyd's MirrorEQUIPMENT NEEDED:- Transmitter - Receiver- Goniometer - Fixed Arm Assembly- Component Holder - Reflector (1)- Meter StickIntroductionIn earlier experiments, such as 3 and 6, you observedhow a single electromagnetic wave can be diffractedinto two waves and, when the two components joinback together, they form an interference pattern.Lloyd’s Mirror is another example of this phenom-enon. Just as with the other interference patterns youhave seen, this interference pattern provides a conve-nient method for measuring the wavelength of theradiation.Figure 7.1 is a diagram for Lloyd’s mirror. An elec-tromagnetic wave from point source A is detected atpoint C. Some of the electromagnetic wave, ofcourse, propagates directly between point A and C,but some reaches C after being reflected at point B. A maximum signal will be detected whenthe two waves reach the detector in phase. Assuming that the diagram shows a setup for a maxi-mum signal, another maximum will be found when the Reflector is moved back so the pathlength of the reflected beam is AB + BC + λ λ λ λ λ.Procedure①Arrange the equipment as shown in Figure 7.2. For best results, the Transmitter and Receivershould be as far apart as possible. Be sure the Receiver and Transmitter are equidistant (d1) fromthe center of the Goniometer degree plate and that the horns are directly facing each other. (SeeFigure 7.3 for location of effective points of transmission and reception). Also be sure that thesurface of the Reflector is parallel to the axis of theTransmitter and Receiver horns.②While watching the meter on the Receiver, slowly slidethe Reflector away from the Degree Plate. Notice howthe meter reading passes through a series of minimaand maxima.③Find the Reflector position closest to the degree platewhich produces a minimum meter reading.④Measure and record h1, the distance between the centerof the degree plate and the surface of the Reflector.h1 = _________________________.Figure 7.1 Lloyd's MirrorBACd1d1hFigure 7.2 Equipment Setup1.0 meter or more
24012-04630GMicrowave Optics⑤Slowly slide the Reflector away from the degree plate until the meter reading passes through a maxi-mum and returns to a new minimum. Measure and record h2, the new distance between the centerof the degree plate and the surface of the Reflector.h2 = _________________________.⑥Measure d1 the distance between the center of the degree scale and the Transmitter diode.d1 = _________________________.⑦Use your collected data to calculate λλλλλ, the wavelength of the microwave radiation.λ = _________________________.⑧Change the distance between the Transmitter and Receiver and repeat your measurements.h1 = _________________________.h2 = _________________________.d1 = _________________________.λ = _________________________.Questions①What is the advantage in having the effective transmission and reception points equidistant from thecenter of the degree plate in this experiment?➤➤➤➤➤ NOTE: Don’t stand in front of the apparatus while conducting the experiment. Your body acts asa reflector. Therefore, try to stand to one side behind the plane of the antenna horn.5 cm 5 cmFigure 7.3 Transmission and Reception PointsReceiverTransmitterEffective Point of Emission ofTransmitter Signal ReceiverEffective Point of Reception ofTransmitter Signal
25012-04630G Microwave OpticsExperiment 8: Fabry-Perot InterferometerEQUIPMENT NEEDED:- Transmitter - Receiver- Goniometer - Component Holders (2)- Partial Reflectors (2)IntroductionWhen an electromagnetic wave encounters a partial reflector, part of the wave reflects and part ofthe wave transmits through the partial reflector. A Fabry-Perot Interferometer consists of twoparallel partial reflectors positioned between a wave source and a detector (see Figure 8.1).The wave from the source reflects back and forth between the two partial reflectors. However,with each pass, some of the radiation passes through to the detector. If the distance between thepartial reflectors is equal to nλλλλλ/2, where λλλλλ is the wavelength of the radiation and n is an integer,then all the waves passing through to the detector at any instant will be in phase. In this case, amaximum signal will be detected by the Receiver. If the distance between the partial reflectors isnot a multiple of λλλλλ/2, then some degree of destructive interference will occur, and the signal willnot be a maximum.Procedure①Arrange the equipment as shown in Figure 8.1. Plug inthe Transmitter and adjust the Receiver controls for aneasily readable signal.②Adjust the distance between the Partial Reflectors andobserve the relative minima and maxima.③Adjust the distance between the Partial Reflectors toobtain a maximum meter reading. Record, d1, thedistance between the reflectors.d1 = _________________________.④While watching the meter, slowly move one Reflector away from the other. Move the Reflectoruntil the meter reading has passed through at least 10 minima and returned to a maximum.Record the number of minima that were traversed. Also record d2, the new distance between theReflectors.Minima traversed = _________________________.d2 = _________________________.⑤Use your data to calculate λλλλλ, the wavelength of the microwave radiation.λ = _________________________.⑥Repeat your measurements, beginning with a different distance between the Partial Reflectors.d1 = _________________________. Minima traversed = _________________________.d2 = _________________________. λ = _________________________.Figure 8.1 Fabry-Perot InterferometerPartial Reflectors
26012-04630GMicrowave OpticsQuestions①What spacing between the two Partial Reflectors should cause a minimum signal to be deliveredto the Receiver?②In an optical Fabry-Perot interferometer the interference pattern usually appears as a seriesof concentric rings. Do you expect such a pattern to occur here? Why? Check to see ifthere is one.
27012-04630G Microwave OpticsExperiment 9: Michelson InterferometerEQUIPMENT NEEDED:- Transmitter, - Receiver- Goniometer, - Fixed Arm Assembly- Component Holders (2) - Rotating Table, Reflectors (2)- Partial Reflector (1)IntroductionLike the Fabry-Perot interferometer, the Michelsoninterferometer splits a single wave, then brings theconstituent waves back together so that they superpose,forming an interference pattern. Figure 9.1 shows thesetup for the Michelson interferometer. A and B areReflectors and C is a Partial Reflector. Microwavestravel from the Transmitter to the Receiver over twodifferent paths. In one path, the wave passes directlythrough C, reflects back to C from A, and then is re-flected from C into the Receiver. In the other path, thewave reflects from C into B, and then back through Cinto the Receiver.If the two waves are in phase when they reach theReceiver, a maximum signal is detected. By movingone of the Reflectors, the path length of one wavechanges, thereby changing its phase at the Receiver soa maxium is no longer detected. Since each wavepasses twice between a Reflector and the Partial Re-flector, moving a Reflector a distance λλλλλ/2 will cause acomplete 360-degree change in the phase of one wave at the Receiver. This causes the meterreading to pass through a minimum and return to a maximum.Procedure①Arrange the equipment as shown in Figure 9.1. Plug in the Transmitter and adjust the Receiverfor an easily readable signal.②Slide Reflector A along the Goniometer arm and observe the relative maxima and minima of themeter deflections.③Set Reflector A to a position which produces a maximum meter reading. Record, x1, the posi-tion of the Reflector on the Goniometer arm.x1 = _________________________.④While watching the meter, slowly move Reflector A away from the Partial Reflector. Move theReflector until the meter reading has passed through at least 10 minima and returned to a maxi-mum. Record the number of minima that were traversed. Also record x2, the new position ofReflector A on the Goniometer arm.Minima traversed = _________________________.x2 = _________________________.ABCFigure 9.1 Michelson Interferometer
28012-04630GMicrowave Optics⑤Use your data to calculate λλλλλ, the wavelength of the microwave radiation.λ = _________________________.⑥Repeat your measurements, beginning with a different position for Reflector A.x1 = _________________________.Minima traversed = _________________________.x2 = _________________________.λ = _________________________.Questions①You have used the interferometer to measure the wavelength of the microwave radiation. If youalready knew the wavelength, you could use the interferometer to measure the distance over whichthe Reflector moved. Why would an optical interferometer (an interferometer using visible lightrather than microwaves) provide better resolution when measuring distance than a microwave inter-ferometer?An Idea for Further InvestigationPlace a cardboard box between the Partial Reflector and Reflector A. Move one of the reflectorsuntil the meter deflection is a maximum. Slowly fill the box with styrene pellets while observing themeter deflections. On the basis of these observations, adjust the position of Reflector A to restore theoriginal maximum. Measure the distance over which you adjusted the reflector. Also measure thedistance traversed by the beam through the pellets. From this data, can you determine the styrenepellets’ index of refraction at microwave frequencies? (The wavelength of electromagnetic radiationin a material is given by the relationship λλλλλ = λλλλλ0/n; where λλλλλ is the wavelength, λλλλλ0 is the wavelengthin a vacuum, and n is the index of refraction of the material.) Try boxes of various widths. Youmight also try filling them with a different material.
29012-04630G Microwave OpticsExperiment 10: Fiber OpticsEQUIPMENT NEEDED:- Transmitter - Receiver- Goniometer - Tubular Plastic Bags- Styrene PelletsIntroductionLight can propagate through empty space, but it can also propagate well through certain materi-als, such as glass. In fiber optics, a thin, flexible glass tube functions as a transmission line forlight from a laser, much as a copper wire can function as a transmission line for electrical im-pulses. In the same way that variation of the electrical impulses can carry information throughthe copper wire (for example as a phone message), variation in the intensity of the laser light cancarry information through the glass tube.Procedure①Align the Transmitter and Receiver directly across from each other on the Goniometer, and adjustthe Receiver controls for a readable signal.②Fill a tubular plastic bag with styrene pellets (tie the end or use a rubber band). Place one end ofthe bag in the Transmitter horn. What happens to the meter reading? Now place the other end inthe Receiver horn. How does the intensity of the detected signal compare to the intensity whenthe bag is not used?③Remove the plastic bag and turn the Rotatable Goniometer arm until no meter deflection appears.Place one end of the bag in the Transmitter horn, the other in the Receiver horn. Note the meterreading.④Vary the radius of curvature of the plastic bag. How does this effect the signal strength? Doesthe signal vary gradually or suddenly as the radial curvature of the plastic bag changes? Find theradius of curvature at which the signal begins to drop significantly.Questions①Check your textbook for information on Total Internal Reflection. Based on the radial curvaturewhen the signal begins to show attenuation as it passes through the plastic bag, determine theangle of total internal reflection for the styrene pellets. Can you use this value to determine theindex of refraction of the styrene pellets?②Would you expect the plastic bag filled with styrene pellets to work the same with radiation atoptical frequencies? Why?
30012-04630GMicrowave OpticsNotes
31012-04630G Microwave OpticsExperiment 11: Brewster's AngleEQUIPMENT NEEDED:- Transmitter - Receiver- Goniometer - Rotating Table- Polyethylene PanelIntroductionWhen electromagnetic radiation passes from one media into another, some of the radia-tion usually reflects from the surface of the new medium. In this experiment, you willfind that the magnitude of the reflected signal depends on the polarization of the radiation.In fact, at a certain angle of incidence—known as Brewster’s Angle—there is an angle ofpolarization for which no radiation will be reflected. (Check your textbook for more infor-mation on Brewster’s Angle.)Procedure①Arrange the equipment as shown in Figure 11.1, settingboth the Transmitter and the Receiver for horizontalpolarization (90°).②Adjust the Panel so the angle of incidence of the micro-wave from the Transmitter is 20°. Rotate the Goniom-eter arm until the Receiver is positioned where it candetect the maximum signal reflected from the Panel.Adjust the Receiver controls for a mid-scale reading,and record the meter reading in Table 11.1.Angle Meter Reading(Horizontal Polarization)Meter Reading(Vertical Polarization)20°25°30°35°40°45°50°55°60°65°70°75°Table 11.1Figure 11.1 Equipment SetupPolyethylenePanelRotatingTableAngle ofIncidence
32012-04630GMicrowave Optics③Without changing the angles between the transmitted beam, the Polyethylene Panel, and the Re-ceiver, rotate both the Transmitter and the Receiver horns so they align for vertical polarization (0°).Record the new meter reading in the table.④Repeat steps 2 and 3, setting the angle of incidence to each of the values shown in the table below.At each point set the Transmitter and Receiver for horizontal polarization and record the meter read-ing; then set them for vertical polarization and record that reading as well.⑤Plot a graph of “Meter Reading” versus “Angle of Incidence”. Plot both the vertical and horizontalpolarizations on the same graph. Label Brewster’s Angle—the angle at which the horizontally polar-ized wave does not reflect.Questions①Explain how Polaroid sun-glasses can be used to reduce the glare caused by the sun setting over alake or the ocean. Should the glasses be designed to block vertically or horizontally polarized light?②Could you use the microwave apparatus to locate Brewster’s Angle by examining the transmittedwave rather than the reflected wave? How?
33012-04630G Microwave OpticsExperiment 12: Bragg DiffractionEQUIPMENT NEEDED:- Transmitter - Receiver- Goniometer - Rotating Table- Cubic LatticeIntroductionBragg’s Law provides a powerful tool for investigating crystal structure by relating theinterplanar spacings in the crystal to the scattering angles of incident x-rays. In this experiment,Bragg’s Law is demonstrated on a macroscopic scale using a cubic “crystal” consisting of 10-mmmetal spheres embedded in an ethafoam cube.Before performing this experiment, you should understand the theory behind Bragg Diffraction.In particular, you should understand the two criteria that must be met for a wave to be diffractedfrom a crystal into a particular angle. Namely, there is a plane of atoms in the crystal orientedwith respect to the incident wave, such that:①The angle of incidence equals the angle of reflection, and②Bragg's equation, 2dsinθ = nλλλλλ, is satisified; where d is the spacing between the diffractingplanes, θ is the grazing angle of the incident wave, n is an integer, and λλλλλ is the wavelength of theradiation.Procedure①Arrange the equipment as shown in Figure 12.1.②Notice the three families of planes indicated in Figure12.2. (The designations (100), (110), and (210) arethe Miller indices for these sets of planes.) Adjust theTransmitter and Receiver so that they directly faceeach other. Align the crystal so that the (100) planesare parallel to the incident microwave beam. Adjustthe Receiver controls to provide a readable signal.Record the meter reading.Figure 12.1 Equipment SetupRotating TableCubic Lattice (210) (110)(100)Figure 12.2 "Atomic" Planes of theBragg CrystalFigure 12.3 Grazing AngleGrazing Angle
34012-04630GMicrowave Optics③Rotate the crystal (with the rotating table) one degree clockwise and the Rotatable Goniometer armtwo degrees clockwise. Record the grazing angle of the incident beam and the meter reading. (Thegrazing angle is the complement of the angle of incidence. It is measured with respect to the planeunder investigation, NOT the face of the cube; see Figure 12.3.)④Continue in this manner, rotating the Goniometer arm two degrees for every one degree rotation ofthe crystal. Record the angle and meter reading at each position. (If you need to adjust theINTENSITY setting on the Receiver, be sure to indicate that in your data.)⑤Graph the relative intensity of the diffracted signal as a function of the grazing angle of the incidentbeam. At what angles do definite peaks for the diffracted intensity occur?Use your data, the known wavelength of the microwave radiation (2.85 cm), and Bragg’s Law todetermine the spacing between the (100) planes of the Bragg Crystal. Measure the spacing betweenthe planes directly, and compare with your experimental determination.⑥If you have time, repeat the experiment for the (110) and (210) families of planes.Questions①What other families of planes might you expect to show diffraction in a cubic crystal? Would youexpect the diffraction to be observable with this apparatus? Why?②Suppose you did not know beforehand the orientation of the “inter-atomic planes” in the crystal.How would this affect the complexity of the experiment? How would you go about locating theplanes?The Bragg Diffraction Experiment was developed by Dr. Harry Meiners of Rensselaer Poly-technic Institute.
35012-04630G Microwave OpticsTeacher's GuideExp 1 – Introduction to the SystemNotes – on Procedure④ The meter reading does not vary with distance in anentirely predictable way, since the microwaves formstanding waves between the transmitter and receiver atcertain distances. In addition, the meter is not directlyrelated to either the electric field or the intensity of theincident beam. The meter is useful for measuring rela-tive intensity at a constant distance, polarization, andso on.⑤The meter reading oscillates as the distance is de-creased. (See experiment 3, method B)⑥The presence of a reflector increases the meter reading.⑦The receiver detects no signal when the transmitterand receiver are at 90° to each other.⑧The transmitter has a roughly gaussian output distribu-tion, with the 1/e points at about ±20°.There is no significant difference between the outputdistributions in the horizontal and vertical orientationsAnswers – to Questions①/② The meter reading is not proportional to either theelectric field or the intensity.③ The transmitter output is more plane wave thanspherical wave, but it has characteristics of both.
36012-04630GMicrowave OpticsNotes – on Procedure⑤Angle of Incidence Angle of Reflection20° 23°30° 31°40° 41°50° 54°60° 63°70° 85°*80° 78°*90° 70°*The last three points are suspect, due to the spread in theoutput pattern of the transmitter. See experiment 1, part 8.Answers – to Questions①The angle of incidence equals the angle of reflection.This does hold for all angles, although it is not clear inthis experiment due to the spread in the output pattern.②Some of the wave appeared to reflect into differentangles; particularly when the angle of incidence was70° or 90°. This is actually a diffraction effect, not re-flection.③The transmitter does not produce a perfect plane wave,and this does affect the results.Answers – to Questions for AdditionalExperimentation①Intensity of the reflection does vary with the angle ofincidence; from this we can deduce that the reflector isnot 100% efficient.②In general, conductors will reflect the microwavesmuch better than non-conductors.Exp 3– Standing Waves - Measuring WavelengthsNotes – on Procedure➤ NOTE: There are two different methodsdescribed in this lab. The first method, using theMicrowave Detector Probe, is the easier of thetwo; but either will work.Method A# of antinode Distance Wavelength5 7.1 2.8410 14.1 2.8215 20.0 2.6719 27.5 2.89Average: 2.81Frequency: 1.07E+10Method B# of antinode Distance Wavelength 10 13.3 2.6615 20.5 2.73Average: 2.70Frequency: 1.11E+10 (Fewer points were taken due to the limited resolutionof this method.)Answers – to QuestionsThe value obtained by the first method was 1.5% off,and the second was 5.6% off. If it is possible to takemore data points on the second method, you may getbetter results.Exp 2 – Reflection
37012-04630G Microwave OpticsExp 4– Refraction Through a PrismNotes – on Procedure①The empty foam prism absorbs the radiation by a veryslight amount.③θ = 7° (± 1°)④θ1 = 22°θ2 = 29°⑤/⑥ Our experimental value was: n1 = 1.3 ± 0.05Answers – to Questions①This assumption is valid. According to Snell’s law, ifthe angle of incidence is zero, the angle of refraction iszero also.③The index for a solid styrene prism would be higher,due to the greater “optical” density of the solid mate-rial.General Notes①The prism mold may be filled with other materials aswell. We used water for one such test. The water ab-sorbs most of the microwave energy (this is how a mi-crowave oven works) but enough gets through that itmay be measured on the most sensitive scale of thereceiver. We found that n = 1.4 ± 0.05.②The jar that the styrene pellets are shipped in has beenused as a cylindrical lens, with limited success.
38012-04630GMicrowave OpticsExp 5– PolarizationNotes – on Procedure②➤➤➤➤➤NOTE: There is a consistent “glitch” in thedata at a polarization angle of about 40 and 140degrees which is not entirely explained by thenon-linearity of the receiver. (This glitch is alsopresent when the polarizer slits are used in part 5of this lab.) If you have an explanation of whythis occurs, please let us know.③Continued rotation of the receiver results in duplica-tion of the pattern above.⑤⑥The meter reading is zero when the polarizer slits areoriented vertically or horizontally. When the slits areat 45°, the meter reads about 30% of its maximumvalue for that distance.Answers – to Questions①/ ② The meter reading more closely matches the intensity than it does the electric field.③The polarizer transmits only the component of thewave parallel to the polarizer.④When the transmitter and polarizer are at 90°, thewave is completely blocked. Placing a polarizer at 45°,however, introduces a component of the wave parallelto the receiver so that some of the wave is then pickedup.
39012-04630G Microwave OpticsExp 6– Double-Slit InterferenceAnswers – to Questions①/② For the 7.6 cm spacing, the maxima should occur at22° and 48°.For the 10.6 cm spacing, the maxima should be at 15°,33°, and 54°.These theoretical values are closely matched by theexperimental data. The theory assumes that the dis-tance between slit plates and receiver are large com-pared to the slit spacing and wavelength. This require-ment is barely met in the experimental setup used, andcould cause trouble in some situations.③The single-slit pattern (see experiment 7) acts as anupper limit to the multiple-slit pattern from this experi-ment.General Notes①The position of the experimenter has a definite effecton the measurements in this experiment. Experimentto find just how much effect there is with your particu-lar setup, and then take your data accordingly.②Single-slit diffraction may also be attempted on thisapparatus, though we don’t recommend it. The dis-tances are too short, relative to the wavelength; so theanalysis requires the Fresnel/Kirchoff approach insteadof the Fraunhoffer approximation. Even with theFresnel approach, the “fringes” are too small to beseen adequately.Basically, it doesn’t work well at all.
40012-04630GMicrowave OpticsNotes – on Procedure ③-⑧Fringe# h (mm) path length (mm) lambda1 85 7202 138 752 32.103 171 779 26.634 200 806 27.155 227 834 28.116 251 861 27.067 275 890 28.838 298 919 29.139 317 944 25.0810 338 973 28.69average: 27.59stdev: 1.37An alternate method is to graph path length versus fringenumber and take the slope of the graph. This slope will bethe wavelength.From this, λ = 2.79 cm.Answers – to Questions①It simplifies the calculations.Exp 7– Lloyd’s Mirror
41012-04630G Microwave OpticsExp 8– Fabry-Perot InterferometerNotes – on Procedure①-④ For best results, do not move the reflector closestto the transmitter. There are actually two standingwave patterns that may form: one between the trans-mitter and first reflector, and one between the two re-flectors. (There may also be others, such as betweenthe second reflector and the receiver or the second re-flector and the transmitter; but these will be negli-gible.) Moving the first reflector will change the am-plitude of the wave coming into the region betweenthe reflectors, and thus give erroneous results.⑤/⑥ = 2.85 cm‰ NOTE: An alternate method of analysis is tomake a graph of distance versus fringe number andtake the slope of the line to find the wavelength.λ = 2.84 cmAnswers – to QuestionsFirst Plate: 75.2nsecond plate distance Ð1 54.9 20.32 53.6 21.6 1.33 52.2 23.0 1.44 50.9 24.3 1.35 49.4 25.8 1.56 47.9 27.3 1.57 46.5 28.7 1.48 45.0 30.2 1.59 43.6 31.6 1.410 42.1 33.1 1.511 40.8 34.4 1.312 39.4 35.8 1.413 38.0 37.2 1.414 36.6 38.6 1.415 35.1 40.1 1.516 33.8 41.4 1.317 32.3 42.9 1.518 30.9 44.3 1.419 29.4 45.8 1.520 27.9 47.3 1.521 26.5 48.7 1.422 25.0 50.2 1.5 average: 1.42①Minima will occur when the spacing is nλ/4, where nis an odd integer.② We would normally expect just such a pattern; in thiscase, however, the reflectors are too small in relationto the wavelength used; so the next “ring” is locatedbeyond the edge of the reflectors and may not be seen.
42012-04630GMicrowave OpticsExp 9– Michelson InterferometerNotes – on Procedure①-④ Best results are obtained when the mirrors are botha significant distance from the central beamsplitter. Ifeither mirror is too close to the center, the maximasplits into two peaks due to secondary interference ef-fects.nRefl. Pos. _1 75.02 76.4 1.43 77.9 1.54 79.4 1.55 80.8 1.46 82.2 1.47 83.7 1.58 85.1 1.49 86.6 1.510 88.0 1.411 89.4 1.412 90.9 1.513 92.3 1.414 93.8 1.515 95.2 1.416 96.6 1.417 98.1 1.518 99.5 1.419 101.0 1.520 102.4 1.421 104.0 1.6average: 1.45From this we can calculate the wavelength as being2.90 cm.➤➤➤➤➤ NOTE: An alternate method of analysis is toplot the reflector position versus fringe number.The slope of this line will be half the wavelength.By this method, we calculate the wavelength as2.89 cm.Answers – to Questions①The limit of resolution for distance measurements witha Michelson interferometer is roughly 1/4 the wave-length of the light used. Thus with these microwaves,we can measure distance changes of about 7 mm.With a visible-light interferometer and a wavelength of633 nm (HeNe laser light) we can measure distancechanges of only 158 nm.
43012-04630G Microwave OpticsExp 10 – Fiber OpticsExp 11– Brewster's AngleNotes – on ProcedureAnswers – to Questions①Glare off water from a low source is primarily hori-zontal in polarization, so sunglasses should be de-signed to block horizontally polarized light.Notes – on Procedure②The meter reading with the “optical fiber” bag in placecan more than double the unobstructed meter reading.This is because the bag prevents the normal spreadingof the beam, and directs all the microwave radiationinto the receiver horn.③The bag can direct the beam through a full 90° turnwithout measurable attenuation, if the curvature isgradual.④The signal begins to be attenuated with a radius of cur-vature of about 5 cm, and drops off rather suddenly fromthere. It is difficult to get consistent results, though.Answers – to Questions①Theoretically one can use the radius at which the mi-crowaves begin to “leak” to determine the index ofrefraction of the material. In reality, this is quite diffi-cult. Our values for n using this method range from1.1 to 1.4.②The styrene pellets are very small, compared to themicrowave wavelength. Compared to visiblewavelengths, the pellets are enormous. Because ofthis size difference, optical radiation is scattered bythe pellets and microwave radiation is transmitted.Additional IdeaThis apparatus may also be used as a demonstra-tion of how the plane of polarization can be ro-tated by multiple reflections. Rotate the transmitteror receiver 90° to each other, so that no signal getsthrough. Now put the bag of pellets between thetwo. If the bag is held straight, there will be a zerometer reading; but if the bag is curved into a spiral,there will be a non-zero reading.②Theoretically, one could do this by finding thepoint at which there was no transmission of verti-cally polarized light. We have not been able to getgood results in this experiment, however.General Notes①The index of refraction of the polyethylene is 1.5.(Calculated from the dielectric constant at 10 GHz)②One must be careful on this experiment to note thatthere are actually two effects which are being mea-sured. In addition to the Brewster’s angle reflection,there is a certain amount of interference between thefront- and rear-surface reflections from the polyethyl-ene. This interference causes extra peaks at 13.8° and67.2°, and a local minimum at 43.6°. The interferenceis notable enough that you may want to demonstratethat, instead of the Brewster’s angle.①-⑤
44012-04630GMicrowave OpticsExp 12– Bragg DiffractionNotes – on Procedure①The polarization angle of the transmitter and receiver(horizontal or vertical) does not matter.⑤Peaks occur at 18°, 24°, and 45°. These correspond toplane spacings of 4.6cm, 3.4cm, and 4.0 cm (n = 2 forthe 45° peak) The actual spacing is 3.8 cm The firstpeak is apparently a reflection off a different planethan the one we’re measuring.⑥110 Plane:The peak at 29° gives a plane spacing of 2.9 cm; theactual spacing is 2.7 cmAnswers – to Questions①Other families of planes would be the 111 plane, the101 plane, and so on. These would be difficult to ob-serve with this apparatus due to the small size of our“crystal”.②Not knowing the orientation of the interatomic planesof the crystal would increase the complexity of theanalysis. We could orient the crystal so that there wasmaximum transmission; this would indicate to us a100 plane. From there, we could try different anglesuntil we had enough data to assemble a likely pictureof the atomic spacing in the crystal.➤ ➤ ➤ ➤ ➤ NOTE: 10-15% error is reasonable for thisexperiment.
45012-04630G Microwave OpticsAppendixReplacing the Receiver BatteryThe Receiver is powered by two 9-volt alkaline batteries.To replace them, simply remove the back panel of the Re-ceiver (the panel with the rotational scale) by removingthe four screws. Install the new batteries, place them intothe holder as shown below, and replace the panel.➤➤➤➤➤ NOTE: We highly recommend that you use onlyalkaline batteries.Adjusting the Receiver①Meter mechanical zero adjustment:a. Turn the INTENSITY control to OFF.b. The mechanical zero adjustment is located on themeter, centered just below the meter face. With themeter level and in the horizontal position, use asmall (1/8”) flat-blade screwdriver to adjust themeter needle to read as close to 0 as possible.②Electronic offset null adjustment:a. Make sure the Transmitter is OFF by unpluggingit.b. Turn the INTENSITY control to the 1X position.c. Turn the VARIABLE SENSITIVITY control allthe way clockwise to its maximum setting.d. The offset null adjustment is located through asmall hole just above the receiver antenna. Use asmall (1/8”) flat-blade screwdriver to adjust themeter reading as close as possible to 0.Replacing the Receiver Battery➤➤➤➤➤CAUTION: The electronics of the Transmitterand Receiver assemblies contain diodes that are noteasily repairable. An attempt to repair diode assem-blies may void your warranty.➤➤➤➤➤NOTE: Abnormal behavior (weak or erraticmeter readings, etc.) may be caused by weak batter-ies. Please make sure your batteries are good beforegiving us a call.
46012-04630GMicrowave OpticsSchematic Diagram, Microwave TransmitterSchematic Diagram, Microwave ReceiverSchematic Diagrams
47012-04630G Microwave OpticsReplacement Parts ListPasco Part No. Description Oty.Transmitter003-04319 Transmitter Assembly 1113-132 Resistor, 1.3K, 1/4W, 5% 1113-221 Resistor, 220 OHM, 1/4W 5% 1113-471 Resistor, 470 OHM, 1/4W, 5% 1430-085 IC-LM317T Positive V Reg. 1445-005 Module, Microwave Transmitter 1956-04311 Schematic, Microwave Transmitter 0Receiver003-04313 Receiver Assembly 1004-04312 Receiver P.C.B. Assembly 1113-153 Resistor, 15K, 1/4W, 5% 1113-184 Resistor, 180K, 1/4W, 5% 1113-621 Resistor,620 OHM 1/4W 5% 1123-013 Resistor, 562K 1/4w 1% MF 1123-016 Resistor, 51.1K 1/4w 1% MF 1142-028 Trimpot, 50K 1T .5W CERM SA 1216-026 Capacitor, 1000pF 5% 25V 1412-012 Zener Diode, 1N751A 5.1V 5% .4W 2430-086 IC-LF356N FET OP-AMP DIP 1510-019 Switch, Rotary, 2POLE 6POS 1527-001 L.E.D, Red 1555-02811 Printed Circuit Board 1113-152 Resistor, 1.5K, 1/4W, 5% 1113-300 Resistor, 30 OHM, 1/4W, 5% 1123-2001 Resistor, 2K 1/4W 1% MF 1140-01716 Modified Pot - 5K 1140-040 Pot, 5K 1445-006 Module, Microwave Receiver 1525-008 Meter 1710-04313 Wire List, Microwave Receiver 0956-04312 Schematic, Microwave Receiver 0Components003-01748 Assembly, Partial Reflector 2003-02090 Assembly, Receiver/Transmitter Stand 2003-02091 Assembly, Component Holder 2003-02092 Assembly, Rotating Component Holder 1003-02093 Assembly, Fixed Arm 1003-02094 Assembly, Goniometer 1003-02100 Assembly, Rotating Table 1003-02116 Assembly, Styrene Pellets 1003-02817 Assembly, Slit Extender Arm 1540-002 Battery, 9 Volt, Alkaline 2540-007 AC Adapter, 120VAC, 9VDC 1 or 540-013 AC Adapter, 220/240VAC, 9VDC 1648-01749 Metal Reflector 2648-02042 Slit Spacer, Narrow 1648-02043 Slit Spacer, Wide 1648-02052 Polarizer Screen 2648-02082 Ethafoam Prism 1735-027 Plastic Bag, 2 1/2” X 24” 4➤ ➤ ➤ ➤ ➤ NOTE: Replacementparts can be purchasedfrom PASCO or at mostelectronic stores.
48012-04630GMicrowave OpticsNotes
49012-04630G Microwave OpticsTechnical SupportFeedbackIf you have any comments about the product ormanual, please let us know. If you have anysuggestions on alternate experiments or find aproblem in the manual, please tell us. PASCOappreciates any customer feedback. Your input helpsus evaluate and improve our product.To Reach PASCOFor technical support, call us at 1-800-772-8700(toll-free within the U.S.) or (916) 786-3800.fax: (916) 786-3292e-mail: techsupp@pasco.comweb: www.pasco.comContacting Technical SupportBefore you call the PASCO Technical Support staff, itwould be helpful to prepare the following information:➤If your problem is with the PASCO apparatus,note:-Title and model number (usually listed on thelabel);-Approximate age of apparatus;-A detailed description of the problem/sequence ofevents (in case you can’t call PASCO right away,you won’t lose valuable data);-If possible, have the apparatus within reach whencalling to facilitate description of individual parts.➤If your problem relates to the instruction manual,note:- Part number and revision (listed by month andyear on the front cover);- Have the manual at hand to discuss yourquestions.

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