Design of a Beam-forming System in the Vehicle Cabin Wen-Kung Tseng

Size: px
Start display at page:

Download "Design of a Beam-forming System in the Vehicle Cabin Wen-Kung Tseng"

Transcription

1 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 Design of Bem-forming System in the Vehicle Cin Wen-Kung Tseng Astrct This pper presents the design of em-forming system ( directionl udile sound system) in the vehicle cin, where pssengers t different positions in the vehicle cin cn listen to different music. A directionl udile sound cn e generted in vehicle cin y mplitude-modulting the ultrsound crrier with n udio signl, then trnsmitting it from n rry of ultrsonic trnsducers. A novel method hs een proposed in this pper to control the em width of the min loe nd the level of the side loe for the em pttern y using n optimiztion technique. The performnce of the udile sound em steering hs lso een investigted. Some preliminry experiment hs een crried out to vlidte the simultion results. The results show tht the optimiztion method proposed in the pper cn effectively control the em width of the min loe nd the level of the side loe for the udile sound in vehicle cin. The results lso show tht the em steering ngle of directionl udile sound cn e controlled y using the proposed method. Index Terms Directionl Audile Sound, Ultrsound Crrier, Ultrsonic Trnsducers, in Loe. I. INTRODUCTION Trditionl in-cr communiction systems, such s cell phones or rdios, generlly used trditionl loudspekers to rodcst. There re severl weknesses in such systems. For instnce, people in the cr cn ll her the sound. This mkes it impossile to mintin privcy. Besides, people feel othered nd thus the ride qulity would not e so plesnt. If crs re equipped with directionl udile sound systems, ech pssenger in the vehicle interior cn listen to the different music or informtion s shown in Fig.. Thus, people in the vehicle cin would not feel othered. An rry of ultrsonic trnsducers my e employed for generting the directionl udile sound through the self-demodultion of finite-mplitude sound ems []-[6]. The construction of producing directionl udile sound ems includes n ultrsonic trnsducer, driving mplifier for the rry, n A modultor, pure-tone oscilltor for the crrier frequency nd equlizer s shown in Fig.. An rry of ultrsonic trnsducers my e clled prmetric speker regrding the ppliction of the prmetric rry theory. The prmetric speker hs een used for decdes in underwter sonr pplictions for its highly directive response even t low frequencies [7]. The trnsducer rry in prmetric speker systems my comprise plurlity of piezoelectric trnsducers or polyvinylidene fluoride (PVDF) film trnsducers. For simplicity, we cn ssume tht the trnsducer is fed with two ultrsonic signls t closely frequencies f nd f s shown in Fig. 3. The resultnt coustic wves will e the wves with the frequencies of f, f, f ± f, nd higher order hrmonics, etc. Among these new components, the high-frequency terms f, f nd f f, etc. will e strongly ttenuted in ir nd decy rpidly with incresing rnge from the speker. The remining difference frequency f f is produced due to the reltively low sorption of this term in ir [6]. oreover, this low-frequency sound, the udile sound, inherits the sptil chrcteristics of the primry wves, nd its shrp directivity is the result of the coustic nonlinerity. The udile sound is the secondry wve generted from the primry wve y nonliner effect, which hs een reported for few decdes [7]. Since the first ttempt to estlish n udio spotlight system [8], the development of directionl prmetric speker hs ttrcted much ttention. ost of the works relted to directionl udile sound em focused on investigting the directivity of the sound em or the different trnsducer rrngement. There were only few works on the em width control in prmetric rry [6], [9]. Yng et l. proposed the weighted prmetric rry using Cheyshev window method for the trnsducer weightings to generte the directionl udile sound [6]. However in this pper n optimiztion method is used to clculte the optiml trnsducer weightings for controlling the em width of the min loe nd the level of the side loes for the directionl udile sound in vehicle. Also the em steering performnce hs een investigted in this work. Some preliminry experiment hs een crried out to vlidte the simultion results. The pper is orgnized s follows. First, the directivity of the udile sound em nd the formultion of the optimiztion method re derived. Second, simultion results of controlling the em width of the min loe nd the 7

2 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 level of side loes nd the em steering performnce re presented. Then, the preliminry experiment is performed. Finlly the conclusions re mde. Fig.. Directionl udile sound in the vehicle cin Source Signl Equlizer A odultor Power Amplifier Ultrsonic Trnsducer Crrier Signl Fig.. Construction of producing directionl udile sound ems 7

3 Ultrsonic Signls ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 Ultrsonic Trnsducer Resultnt coustic wves f f f Nonliner Interction in medium f f f f - f Higher order hrmonics Fig. 3. Nonliner interction process in ir II. FORULATION OF DESIGNING DIRECTIONAL AUDIBLE SOUND BEA In this section the formultion for designing directionl udile sound systems using n optimiztion technique is presented. The directionl udile sound cn e descried y the Khokhlov Zolotsky Kuznetsov (KZK) eqution which ccounts for the comined effects of nonlinerity, sorption due to viscosity nd het conduction, nd diffrction in finite-mplitude sound em s follows [6], []: p c z p 3 c 3 p 3 c 3 p () where p denotes the coustic pressure, z is the coordinte long the xis of the em propgtion direction, τ is the dely time, c is the speed of the smll signl sound, ρ is the mient density, δ is the sound diffusivity, β is the coefficient of nonlinerity, nd is the trnsverse Lplcin opertor. The solution to () cn e otined using the method of successive pproximtions. For simplicity the primry source with Cussin mplitude shding is ssumed. By using qusi-liner theory, the solution for the finite-mplitude sound em generted y the Gussin source cn e expressed s []: q z r/ pe r, z exp jz / z jz / z where p is the pek source pressure, is the sorption coefficient t primry frequency ω, z = /k is the Ryleigh distnce, nd is the effective source rdius. The directivity cn e esily otined s []: D ( k, xp[ ( k) tn ] (3) where k = ω/c is the wve numer nd θ is the ngle with respect to the xis of the em. Therefore, for i-frequency Gussin source, provided the sorption is neglected, the directivity of the difference frequency is given y the product of the directivity functions of the primry wves [], i.e.: D ( ) D ( )D ( ) () where D (θ) nd D (θ) re the directivity for frequency ω nd ω, respectively. Consider group of weighted primry sources, which re eqully spced with n interelement spcing of d s shown in Fig.. The directivity D (θ) of the weighted primry sources rry for frequency ω cn e written s: D ( ) D ( k, )H( k, ) (5) D ( k, is the perture directivity for frequency ω nd H( k, ) where ) e expressed s []: () is the rry response which cn 73

4 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 jn ( ) H( k, ) hne (6) n where h n is the nth trnsducer weighting, nd n =,,,..., -. d / csin is the time dely due to the rry geometry. d / csin is the time dely due to the em steering ngle. Weightings h h Ultrsonic trnsducers d h Fig.. Uniform liner rry In our study the trnsducer weightings re vried with frequency. Therefore the rry response for frequency ω cn e expressed s: jn ( ) H( k, ) hn( (7) n Similrly, the directivity for primry frequency ω, D (θ), cn e written s: D ( ) D ( k, )H( k, ) (8) D ( k, is the perture directivity for frequency ω nd H( k, ) where ) e expressed s: H( k is the rry response which cn jn ( ), ) hne (9) n where h n is the nth trnsducer weighting, nd n =,,,..., -. If the weightings re vried with frequency, the fr-field rry response cn e expressed s: H( k jn ( ), ) hn( ) e () n Sustitution of (5) nd (8) into () yields D ( ) D ( k, )H( k, )D ( k, )H( k, ) D ( () where ) is em pttern for udile frequency, i.e. the difference frequency directivity. The em pttern for udile frequency cn lso e written y sustituting (3), (7) nd () into () s: 7

5 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 ( xp[ ( ) jn ( ) D k tn ] h ( exp[ ( k ) tn ] n n jn ( ) hn( n Sustituting k / c, f, d sin / c D ( ) exp[ (f, nd d / csin tn ] hn n ( f into eqution () yields jnf (sin sin ) d / c () exp[ ( jnf (sin sin ) d / c f tn ] hn( f (3) n Eqution (3) cn e used to determine the directivity of udile sound em. The min ojective of the optimiztion method proposed in the study is to control the em width of the min loe nd the side loes level of the difference frequency directivity in (3). The oservtion points re set from - to in the study. The formultion of the optimiztion pproch proposed in the work for designing directionl udile sound systems cn e expressed s: inimize D ( ) D ( ) Suject to D ( 3 ) D ( ) D ( 3 ) D ( ), is the ngle of the side loe, i.e. /, is the ngle of the side loe, i.e. /, 3 is the ngle of the min loe, i.e. / 3 /, is the desired em width, nd where () is the mplitude difference etween the min loe nd side loe. Sustitution of (3) into () yields inimize n exp[ (f h n ( f tn ] hn n ( f jnf (sin sin ) d / c exp[ (f tn ] sin ) d / c exp[ (f / ) tn ] ( ) c hn f e n jnf (sin jnf (sin sin ) d / c exp[ ( f Suject to exp[ (f n h n ( f (sin sin ) / tn jn f d c hn( f n tn 3] hn n ( f jnf (sin 3 sin ) d / c exp[ (f tn 3] 3 sin ) d / c exp[ (f / ) tn ] ( ) c hn f e n jnf (sin jnf (sin sin ) d / c 75

6 exp[ n ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 jn f (sin sin ) d / c ( f tn ] hn( f n exp[ (f h n ( f tn 3] hn n ( f jnf (sin 3 sin ) d / c exp[ (f tn 3] 3 sin ) d / c exp[ (f / ) tn ] ( ) c hn f e n jnf (sin jnf (sin sin ) d / c jn f (sin sin ) d / c exp[ ( f tn ] hn( f, (5) n The optiml vlues of h n (f ) nd h n (f ) cn e clculted using the function fmincon( ) in ATLAB. By sustituting the optiml vlues of h n (f ) nd h n (f ) into (3) the directivity of udile sound em, D ( ), cn e otined. III. SIULATION RESULTS In this section the simulted directivity of the udile sound em creted y using the optimiztion method s shown in (5) is presented, nd then compred to those otined y using Cheyshev weighting method [6]. In this study, the numer of weighting functions in the directionl udile sound system is 8 for frequencies f nd f s shown in Fig. 5. Therefore there re 6 weighting functions, i.e.. The crrier frequency of the ultrsonic h ( f ),h ( f ),...,h ( f ) h ( f ),h ( f ),...,h ( f ) 7 trnsducer rry is set s khz, i.e. f = khz. The demodulted signl is t the frequency from.5 khz to 6 khz with 5 Hz intervl. A totl of = 8 ultrsonic trnsducer rry is used with inter-element spcing d = 9.7 mm. The effective source rdius is set t = 3.85 mm nd the speed of sound c is 3 ms -. The weighting functions, h n (f ) nd h n (f ), re clculted for difference frequency s em width for, nd 6 using the proposed method. Figs. 6, 7 nd 8 show the difference frequency s directivity with, nd 7, i.e. without em steering, for 6 respectively. Figs. 6(), 7() nd 8() re the difference frequency s directivity using Cheyshev weighting method [6], nd Figs. 6(), 7() nd 8() re the difference frequency s directivity using the optimiztion method proposed in the pper. From the figures it cn e seen tht the mplitude in the side loe using the proposed method is lower thn tht using the Cheyshev weighting method. This is ecuse the optimiztion method tried to find the optiml weighting functions which minimize the sum of the squred mplitude of the side loe nd suject to the mplitude difference etween the min loe nd the side loe. Therefore the optimiztion method proposed in this pper performs etter thn the Cheyshev weighting method. As cn e seen from the figures the em width cn lso e controlled using the optimiztion method. This is ecuse the difference frequency s directivity is the product of two primry frequency s directivities, nd its em width lwys tkes on the nrrowest em width of the two primry wves. It cn oviously e seen tht constnt em width is chieved for ll frequencies using the proposed method. The highest side loe mplitude of difference frequency sound y using the optimiztion method nd Cheyshev weighting method is summrized in Tle. The highest side loe mplitude with the proposed method gets ttenuted more compred to the method with Cheyshev weighting. This is since the sum of the squred mplitude of the side loe region is minimized through ll the frequencies. Therefore the lower side loe mplitude is otined using the propose method. From the Figs. 6, 7, 8 nd Tle we cn oserve tht etter directivity of the udile sound em is creted using the optimiztion method proposed in the pper thn tht using the Cheyshev weighting method. In this study the performnce of the difference frequency s directivity for with nd em steering hs lso een investigted. Figs. 9 nd show the difference 76

7 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 frequency s directivity for with nd em steering respectively. As cn e seen from the figures the difference frequency cn e steered ccurtely nd the em width is lmost constnt through ll frequencies. Also the mplitude difference etween the min loe nd side loe is out 8dB. Therefore the difference frequency s steering ngle cn e controlled y using the proposed method. In the next section some preliminry experiments will e crried out to vlidte the simultion results. f f Weightings h (f ) h (f ) h (f ) h (f ) h (f ) h (f ) h 3 (f ) h 3 (f ) h (f ) h (f ) h 5 (f ) h 5 (f ) h 6 (f ) h 6 (f ) h 7 (f ) h 7 (f ) Trnsducers Fig. 5. The directionl udile sound system with 8 weighting functions for frequencies f nd f. () 77

8 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 Fig. 6. Difference frequency s directivity for (). () Cheyshev weighting method. () Optimiztion method. () 78

9 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 Fig. 7. Difference frequency s directivity for (). () Cheyshev weighting method. () Optimiztion method. () 79

10 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 () Fig. 8. Difference frequency s directivity for 6. () Cheyshev weighting method. () Optimiztion method. Tle The highest side loe level Cheyshev method Optimiztion method Bem width = -5 db - db Bem width = -5 db - db Bem width = 6-75 db - db 8

11 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 Fig. 9. Difference frequency s directivity for with em steering. Fig.. Difference frequency s directivity for with em steering 8

12 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 IV. PRELIINARY EXPERIENTS In this experiment we investigte the performnce of the directionl udile sound systems in the vehicle cin with weighted trnsducer rry using n optimiztion method. The configurtion of the directionl udile sound experimentl system is plced in front of the right front set in the vehicle cin s shown in Fig.. The experimentl setup of the directionl udile sound system s shown in Fig. includes n ultrsonic trnsducer rry comprising eight trnsducers s shown in Fig. 3, high-frequency microphone (type PCB 377C), mplifiers, filters, function genertor, nd n FFT nlyzer for signl cquisition. The high-frequency microphone ws set-up to rotte t rdius of cm from the center of the trnsducer rry on turntle. The rotting microphone ws swept round n rc from - to reltive to the trnsducer rry s shown in Fig.. It should e noted tht stndrd udio microphones re not suitle for these mesurements, s their own nonlinerities cn crete demodultion t the microphone element itself, cusing incorrect mesurements. One nd-pss filter ws connected etween the function genertor nd the 8 independent mplifiers. The other nd-pss filter ws connected etween the FFT nlyzer nd the mplifier. The signl mesured y the microphone, which ws pssed through nd-pss filter nd then smpled t frequency of 6 khz, ws recorded t increments. The smpled signls were cquired into n FFT nlyzer. A function genertor ws used to generte the signls from to 6 khz in 5 Hz intervls. The directivity of khz for ech trnsducer ws mesured first nd then the directivities of.5 khz 6 khz for ech trnsducer were mesured. The directivity dt mesured ove were tken to clculte the optiml weighting functions, h n (f ) nd h n (f ), for difference frequency s em width,, using the proposed method s shown in (5). The optiml weighting functions clculted were implemented in digitl signl processor (DSP) ord s shown in Fig.. Within the DSP, the udio signl ws converted into digitl signl y n nlogue-to-digitl converter (ADC), modulted y crrier frequency, weighted y weighting functions, nd converted ck to nlogue y the digitl-to-nlogue converter (DAC). The signls were finlly sent to the driver circuit, which provides high current to drive the high cpcitive ultrsonic trnsducers. Fig. 5 shows the difference frequency s directivity normlized to the mximum level for through the experiment. It cn e seen tht constnt em width is chieved for ll frequencies nd the mplitude difference etween the min loe nd side loe is out 7dB. From Fig. 5 we cn oserve tht the result in the experiment is similr to tht in the simultion s shown in Fig. 6(). Therefore the optimiztion method proposed in the pper cn etter control the em width. Also good directivity cn e chieved using the proposed method. - The directionl udile sound experimentl system icrophone Fig.. Configurtion of the directionl udile sound system in vehicle cin 8

13 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 icrophone - Amplifier Ultrsonic trnsducer rry Bnd-pss filter 8 independent mplifiers Power supply Bnd-pss filter FFT nlyzer Function Genertor Fig.. The directionl udile sound experimentl setup with the microphone t different positions reltive to the ultrsonic trnsducer rry, i.e., - to degrees. Fig. 3. An ultrsonic trnsducer rry comprising eight trnsducers 83

14 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 DAC Driver Ultrsonic trnsducers - Audio signl ADC odultion, weighting nd filtering DAC Driver DAC 7 Driver Amplifier DSP ord FFT nlyzer Bnd pss filter Fig.. Hrdwre configurtion of the directionl udile sound system Fig. 5. Difference frequency s directivity normlized to the mximum level for through the experiment. 8

15 ISSN: ISO 9:8 Certified Interntionl Journl of Engineering Science nd Innovtive Technology (IJESIT) Volume, Issue 6, Novemer 3 V. CONCLUSION In this pper n optimiztion method hs een proposed for designing directionl udile sound system in the vehicle cin. A uniform liner rry composed of eight ultrsonic trnsducers with different weighting functions ws used for generting the udile sound em. The optiml weighting functions were clculted using the optimiztion method. The theoreticl derivtion of the proposed method hs een descried nd some simultion results hve lso een presented in the pper. A preliminry experiment hs een crried out to vlidte the simultion results. The performnce of the em width control using the proposed method hs een evluted. It cn e seen tht the proposed method could effectively control the em width of the min loe nd the level of the side loes for the udile sound em. The directionl udile sound em could lso e steered using the proposed method. It is verified y the simultion nd experiment results tht the lower side loes level could e otined y using the proposed method. Therefore the proposed method could etter control the em width nd good directivity could lso e chieved. ACKNOWLEDGEENT The study ws supported y the Ntionl Science Council of Tiwn, the Repulic of Chin, under project numer NSC---E-8-. REFERENCES [] H.O. Berkty, Possile exploittion of nonliner coustics in underwter trnsmitting pplictions, Journl of Sound nd Virtion, vol. (), pp. 35-6, 965. [] in Chen, Limei Xu, Dgui Hung, Ying Wng nd Xuesheng Li, Experimentl verifiction of squre rooting lgorithm for prmetric loudspeker with PVDF film trnsducer, Interntionl Journl of Innovtive Computing, Informtion nd Control, vol., Numer 8, pp , August 8. [3] F.J. Pompei, The use of irorne ultrsonic for generting udile sound ems, Journl of Audio Engineering Society, vol. 7(9), pp , 999. [] P.F. Joseph, The use of irorne ultrsonic for generting udile sound ems, Journl of Audio Engineering Society, vol. 7(9), pp , 999. [5] D.I. Hvelock nd A.J. Brmmer, Directionl loudspekers using sound ems, Journl of Audio Engineering Society, vol. 8(), pp ,. [6] J. Yng, K.S. Tn, W.S. Gn, nd J. Tin, odeling of finite-mplitude sound ems: second order fields generted y prmetric loudspeker, IEEE Trnsctions on ultrsonics, ferroelectrics, nd frequency control, vol. 5(), pp. 6-68, 5. [7] P.J. Westervelt, Prmetric coustic rry, Journl of Acousticl Society of Americ, vol. 35(), pp , 963. [8]. Yoneym nd J. Fujimoto, The udio spotlight: An ppliction of nonliner interction of sound wves to new type of loudspeker design, Journl of Acousticl Society of Americ, vol. 73(5), pp , 993. [9] W.S. Gn, J. Yng, K.S. Tn, nd.h. Er, A digitl emsteerer for difference frequency in prmetric rry, IEEE trnsctions on udio, speech, nd lnguge processing, vol. (3), pp. 8-5, 6. [].F. Hmilton nd D.T. Blckstock, Nonliner Acoustics, Acdemic press, Sn Diego, 998. [] D.H. Johnson nd D.E. Dudgeon, Arry signl processing, Prentice-Hll, NJ, 993. AUTHOR BIOGRAPHY Wen-Kung Tseng received the B.Eng. in mechnicl engineering from the Ntionl Tipei University of Technology, Tipei, Tiwn, nd.sc. nd Ph.D. degrees in coustics from the University of Southmpton, U.K., in 998 nd, respectively. He joined the Nnki University of Technology, Tiwn, in y s n Assistnt Professor. He ws promoted to n Associte Professor in 7. He joined the Ntionl Chnghu University of Eduction, Tiwn, in August 7 s n Associte Professor. He ws promoted to Professor in 3. His reserch interests include ctive noise control, nonliner coustics, signl processing, optimiztion techniques, nd DSP pplictions. 85

OVER-DETERMINATION IN ACOUSTIC TWO-PORT DATA MEASUREMENT

OVER-DETERMINATION IN ACOUSTIC TWO-PORT DATA MEASUREMENT OVER-DEERMINAION IN ACOUSIC WO-POR DAA MEASUREMEN Sry Allm, Hns Bodén nd Mts Åom he Mrcus Wllenerg Lortory for Sound nd Virtion Reserch Dept. of Aeronuticl nd Vehicle Engineering, KH, SE-0044 Stockholm,

More information

15. Quantisation Noise and Nonuniform Quantisation

15. Quantisation Noise and Nonuniform Quantisation 5. Quntistion Noise nd Nonuniform Quntistion In PCM, n nlogue signl is smpled, quntised, nd coded into sequence of digits. Once we hve quntised the smpled signls, the exct vlues of the smpled signls cn

More information

a * a (2,1) 1,1 0,1 1,1 2,1 hkl 1,0 1,0 2,0 O 2,1 0,1 1,1 0,2 1,2 2,2

a * a (2,1) 1,1 0,1 1,1 2,1 hkl 1,0 1,0 2,0 O 2,1 0,1 1,1 0,2 1,2 2,2 18 34.3 The Reciprocl Lttice The inverse of the intersections of plne with the unit cell xes is used to find the Miller indices of the plne. The inverse of the d-spcing etween plnes ppers in expressions

More information

Partial Derivatives. Limits. For a single variable function f (x), the limit lim

Partial Derivatives. Limits. For a single variable function f (x), the limit lim Limits Prtil Derivtives For single vrible function f (x), the limit lim x f (x) exists only if the right-hnd side limit equls to the left-hnd side limit, i.e., lim f (x) = lim f (x). x x + For two vribles

More information

LINEAR ALGEBRA APPLIED

LINEAR ALGEBRA APPLIED 5.5 Applictions of Inner Product Spces 5.5 Applictions of Inner Product Spces 7 Find the cross product of two vectors in R. Find the liner or qudrtic lest squres pproimtion of function. Find the nth-order

More information

KINEMATICS OF RIGID BODIES

KINEMATICS OF RIGID BODIES KINEMTICS OF RIGID ODIES Introduction In rigid body kinemtics, e use the reltionships governing the displcement, velocity nd ccelertion, but must lso ccount for the rottionl motion of the body. Description

More information

CONIC SECTIONS. Chapter 11

CONIC SECTIONS. Chapter 11 CONIC SECTIONS Chpter. Overview.. Sections of cone Let l e fied verticl line nd m e nother line intersecting it t fied point V nd inclined to it t n ngle α (Fig..). Fig.. Suppose we rotte the line m round

More information

10 D. Chakraborty, D. Guha / IJIM Vol. 2, No. 1 (2010) 9-20

10 D. Chakraborty, D. Guha / IJIM Vol. 2, No. 1 (2010) 9-20 Aville online t http://ijim.sriu.c.ir Int. J. Industril Mthemtics Vol., No. (00) 9-0 Addition of Two Generlized Fuzzy Numers D. Chkrorty, D. Guh Deprtment of Mthemtics, IIT-Khrgpur Khrgpur-730, Indi Received

More information

Fully Kinetic Simulations of Ion Beam Neutralization

Fully Kinetic Simulations of Ion Beam Neutralization Fully Kinetic Simultions of Ion Bem Neutrliztion Joseph Wng University of Southern Cliforni Hideyuki Usui Kyoto University E-mil: josephjw@usc.edu; usui@rish.kyoto-u.c.jp 1. Introduction Ion em emission/neutrliztion

More information

Section 6: Area, Volume, and Average Value

Section 6: Area, Volume, and Average Value Chpter The Integrl Applied Clculus Section 6: Are, Volume, nd Averge Vlue Are We hve lredy used integrls to find the re etween the grph of function nd the horizontl xis. Integrls cn lso e used to find

More information

Industrial Electrical Engineering and Automation

Industrial Electrical Engineering and Automation CODEN:LUTEDX/(TEIE-719)/1-7/(7) Industril Electricl Engineering nd Automtion Estimtion of the Zero Sequence oltge on the D- side of Dy Trnsformer y Using One oltge Trnsformer on the D-side Frncesco Sull

More information

10 Vector Integral Calculus

10 Vector Integral Calculus Vector Integrl lculus Vector integrl clculus extends integrls s known from clculus to integrls over curves ("line integrls"), surfces ("surfce integrls") nd solids ("volume integrls"). These integrls hve

More information

Supplementary Information for Directional Reflective Surface Formed via Gradient- Impeding Acoustic Meta-surfaces

Supplementary Information for Directional Reflective Surface Formed via Gradient- Impeding Acoustic Meta-surfaces Supplementry Informtion for Directionl Reflective Surfce Formed vi Grdient- Impeding Acoustic Met-surfces Kyungjun Song 1*, Jedo Kim 2, Hur Shin 1, Jun-Hyuk Kwk 1, Seong-Hyun Lee 3,Tesung Kim 4 1 Deprtment

More information

Characterization of Impact Test Response of PCCP with System Identification Approaches

Characterization of Impact Test Response of PCCP with System Identification Approaches 7th World Conference on Nondestructive Testing, 25-28 Oct 2008, Shnghi, Chin Chrcteriztion of Impct Test Response of PCCP with System Identifiction Approches Astrct Zheng LIU, Alex WANG, nd Dennis KRYS

More information

Lesson 8. Thermomechanical Measurements for Energy Systems (MENR) Measurements for Mechanical Systems and Production (MMER)

Lesson 8. Thermomechanical Measurements for Energy Systems (MENR) Measurements for Mechanical Systems and Production (MMER) Lesson 8 Thermomechnicl Mesurements for Energy Systems (MEN) Mesurements for Mechnicl Systems nd Production (MME) A.Y. 205-6 Zccri (ino ) Del Prete Mesurement of Mechnicl STAIN Strin mesurements re perhps

More information

QUADRATURE is an old-fashioned word that refers to

QUADRATURE is an old-fashioned word that refers to World Acdemy of Science Engineering nd Technology Interntionl Journl of Mthemticl nd Computtionl Sciences Vol:5 No:7 011 A New Qudrture Rule Derived from Spline Interpoltion with Error Anlysis Hdi Tghvfrd

More information

This chapter will show you. What you should already know. 1 Write down the value of each of the following. a 5 2

This chapter will show you. What you should already know. 1 Write down the value of each of the following. a 5 2 1 Direct vrition 2 Inverse vrition This chpter will show you how to solve prolems where two vriles re connected y reltionship tht vries in direct or inverse proportion Direct proportion Inverse proportion

More information

u( t) + K 2 ( ) = 1 t > 0 Analyzing Damped Oscillations Problem (Meador, example 2-18, pp 44-48): Determine the equation of the following graph.

u( t) + K 2 ( ) = 1 t > 0 Analyzing Damped Oscillations Problem (Meador, example 2-18, pp 44-48): Determine the equation of the following graph. nlyzing Dmped Oscilltions Prolem (Medor, exmple 2-18, pp 44-48): Determine the eqution of the following grph. The eqution is ssumed to e of the following form f ( t) = K 1 u( t) + K 2 e!"t sin (#t + $

More information

FEM ANALYSIS OF ROGOWSKI COILS COUPLED WITH BAR CONDUCTORS

FEM ANALYSIS OF ROGOWSKI COILS COUPLED WITH BAR CONDUCTORS XIX IMEKO orld Congress Fundmentl nd Applied Metrology September 6 11, 2009, Lisbon, Portugl FEM ANALYSIS OF ROGOSKI COILS COUPLED ITH BAR CONDUCTORS Mirko Mrrcci, Bernrdo Tellini, Crmine Zppcost University

More information

1B40 Practical Skills

1B40 Practical Skills B40 Prcticl Skills Comining uncertinties from severl quntities error propgtion We usully encounter situtions where the result of n experiment is given in terms of two (or more) quntities. We then need

More information

Design and Analysis of Array Weighted Wideband Antenna using FRFT

Design and Analysis of Array Weighted Wideband Antenna using FRFT The Interntionl Arb Journl of Informtion Technology, Vol., o. 4, July 3 373 Design nd Anlysis of Arry Weighted Widebnd Antenn using FRFT Adri Sty Srinivs Ro nd Prudhivi Mllirjun Ro Deprtment of ECE, Adity

More information

Section 4: Integration ECO4112F 2011

Section 4: Integration ECO4112F 2011 Reding: Ching Chpter Section : Integrtion ECOF Note: These notes do not fully cover the mteril in Ching, ut re ment to supplement your reding in Ching. Thus fr the optimistion you hve covered hs een sttic

More information

The Trapezoidal Rule

The Trapezoidal Rule _.qd // : PM Pge 9 SECTION. Numericl Integrtion 9 f Section. The re of the region cn e pproimted using four trpezoids. Figure. = f( ) f( ) n The re of the first trpezoid is f f n. Figure. = Numericl Integrtion

More information

Designing Information Devices and Systems I Spring 2018 Homework 8

Designing Information Devices and Systems I Spring 2018 Homework 8 EECS 16A Designing Informtion Devices nd Systems I Spring 2018 Homework 8 This homework is due Mrch 19, 2018, t 23:59. Self-grdes re due Mrch 22, 2018, t 23:59. Sumission Formt Your homework sumission

More information

Linear Inequalities: Each of the following carries five marks each: 1. Solve the system of equations graphically.

Linear Inequalities: Each of the following carries five marks each: 1. Solve the system of equations graphically. Liner Inequlities: Ech of the following crries five mrks ech:. Solve the system of equtions grphiclly. x + 2y 8, 2x + y 8, x 0, y 0 Solution: Considerx + 2y 8.. () Drw the grph for x + 2y = 8 by line.it

More information

New Expansion and Infinite Series

New Expansion and Infinite Series Interntionl Mthemticl Forum, Vol. 9, 204, no. 22, 06-073 HIKARI Ltd, www.m-hikri.com http://dx.doi.org/0.2988/imf.204.4502 New Expnsion nd Infinite Series Diyun Zhng College of Computer Nnjing University

More information

Bend Forms of Circular Saws and Evaluation of their Mechanical Properties

Bend Forms of Circular Saws and Evaluation of their Mechanical Properties ISSN 139 13 MATERIALS SCIENCE (MEDŽIAGOTYRA). Vol. 11, No. 1. 5 Bend Forms of Circulr s nd Evlution of their Mechnicl Properties Kristin UKVALBERGIENĖ, Jons VOBOLIS Deprtment of Mechnicl Wood Technology,

More information

Quantum Nonlocality Pt. 2: No-Signaling and Local Hidden Variables May 1, / 16

Quantum Nonlocality Pt. 2: No-Signaling and Local Hidden Variables May 1, / 16 Quntum Nonloclity Pt. 2: No-Signling nd Locl Hidden Vriles My 1, 2018 Quntum Nonloclity Pt. 2: No-Signling nd Locl Hidden Vriles My 1, 2018 1 / 16 Non-Signling Boxes The primry lesson from lst lecture

More information

Trigonometric Functions

Trigonometric Functions Exercise. Degrees nd Rdins Chpter Trigonometric Functions EXERCISE. Degrees nd Rdins 4. Since 45 corresponds to rdin mesure of π/4 rd, we hve: 90 = 45 corresponds to π/4 or π/ rd. 5 = 7 45 corresponds

More information

SOME INTEGRAL INEQUALITIES OF GRÜSS TYPE

SOME INTEGRAL INEQUALITIES OF GRÜSS TYPE RGMIA Reserch Report Collection, Vol., No., 998 http://sci.vut.edu.u/ rgmi SOME INTEGRAL INEQUALITIES OF GRÜSS TYPE S.S. DRAGOMIR Astrct. Some clssicl nd new integrl inequlities of Grüss type re presented.

More information

Chapter 9 Definite Integrals

Chapter 9 Definite Integrals Chpter 9 Definite Integrls In the previous chpter we found how to tke n ntiderivtive nd investigted the indefinite integrl. In this chpter the connection etween ntiderivtives nd definite integrls is estlished

More information

2. VECTORS AND MATRICES IN 3 DIMENSIONS

2. VECTORS AND MATRICES IN 3 DIMENSIONS 2 VECTORS AND MATRICES IN 3 DIMENSIONS 21 Extending the Theory of 2-dimensionl Vectors x A point in 3-dimensionl spce cn e represented y column vector of the form y z z-xis y-xis z x y x-xis Most of the

More information

Flexible Beam. Objectives

Flexible Beam. Objectives Flexile Bem Ojectives The ojective of this l is to lern out the chllenges posed y resonnces in feedck systems. An intuitive understnding will e gined through the mnul control of flexile em resemling lrge

More information

Chapter 1. Chapter 1 1

Chapter 1. Chapter 1 1 Chpter Chpter : Signls nd Systems... 2. Introduction... 2.2 Signls... 3.2. Smpling... 4.2.2 Periodic Signls... 0.2.3 Discrete-Time Sinusoidl Signls... 2.2.4 Rel Exponentil Signls... 5.2.5 Complex Exponentil

More information

Simple Harmonic Motion I Sem

Simple Harmonic Motion I Sem Simple Hrmonic Motion I Sem Sllus: Differentil eqution of liner SHM. Energ of prticle, potentil energ nd kinetic energ (derivtion), Composition of two rectngulr SHM s hving sme periods, Lissjous figures.

More information

Polynomials and Division Theory

Polynomials and Division Theory Higher Checklist (Unit ) Higher Checklist (Unit ) Polynomils nd Division Theory Skill Achieved? Know tht polynomil (expression) is of the form: n x + n x n + n x n + + n x + x + 0 where the i R re the

More information

P 1 (x 1, y 1 ) is given by,.

P 1 (x 1, y 1 ) is given by,. MA00 Clculus nd Bsic Liner Alger I Chpter Coordinte Geometr nd Conic Sections Review In the rectngulr/crtesin coordintes sstem, we descrie the loction of points using coordintes. P (, ) P(, ) O The distnce

More information

Designing Information Devices and Systems I Spring 2018 Homework 7

Designing Information Devices and Systems I Spring 2018 Homework 7 EECS 16A Designing Informtion Devices nd Systems I Spring 2018 omework 7 This homework is due Mrch 12, 2018, t 23:59. Self-grdes re due Mrch 15, 2018, t 23:59. Sumission Formt Your homework sumission should

More information

Mathematics. Area under Curve.

Mathematics. Area under Curve. Mthemtics Are under Curve www.testprepkrt.com Tle of Content 1. Introduction.. Procedure of Curve Sketching. 3. Sketching of Some common Curves. 4. Are of Bounded Regions. 5. Sign convention for finding

More information

Chapter 6 Techniques of Integration

Chapter 6 Techniques of Integration MA Techniques of Integrtion Asst.Prof.Dr.Suprnee Liswdi Chpter 6 Techniques of Integrtion Recll: Some importnt integrls tht we hve lernt so fr. Tle of Integrls n+ n d = + C n + e d = e + C ( n ) d = ln

More information

EMF Notes 9; Electromagnetic Induction ELECTROMAGNETIC INDUCTION

EMF Notes 9; Electromagnetic Induction ELECTROMAGNETIC INDUCTION EMF Notes 9; Electromgnetic nduction EECTOMAGNETC NDUCTON (Y&F Chpters 3, 3; Ohnin Chpter 3) These notes cover: Motionl emf nd the electric genertor Electromgnetic nduction nd Frdy s w enz s w nduced electric

More information

OPEN NEWTON - COTES QUADRATURE WITH MIDPOINT DERIVATIVE FOR INTEGRATION OF ALGEBRAIC FUNCTIONS

OPEN NEWTON - COTES QUADRATURE WITH MIDPOINT DERIVATIVE FOR INTEGRATION OF ALGEBRAIC FUNCTIONS IJRET: Interntionl Journl of Reserch in Engineering nd Technology eissn: 9-6 pissn: -78 OPEN NEWTON - COTES QUADRATURE WITH MIDPOINT DERIVATIVE FOR INTEGRATION OF ALGEBRAIC FUNCTIONS T. Rmchndrn R.Priml

More information

CS12N: The Coming Revolution in Computer Architecture Laboratory 2 Preparation

CS12N: The Coming Revolution in Computer Architecture Laboratory 2 Preparation CS2N: The Coming Revolution in Computer Architecture Lortory 2 Preprtion Ojectives:. Understnd the principle of sttic CMOS gte circuits 2. Build simple logic gtes from MOS trnsistors 3. Evlute these gtes

More information

A027 Uncertainties in Local Anisotropy Estimation from Multi-offset VSP Data

A027 Uncertainties in Local Anisotropy Estimation from Multi-offset VSP Data A07 Uncertinties in Locl Anisotropy Estimtion from Multi-offset VSP Dt M. Asghrzdeh* (Curtin University), A. Bon (Curtin University), R. Pevzner (Curtin University), M. Urosevic (Curtin University) & B.

More information

Creating A New Planck s Formula of Spectral Density of Black-body Radiation by Means of AF(A) Diagram

Creating A New Planck s Formula of Spectral Density of Black-body Radiation by Means of AF(A) Diagram nd Jogj Interntionl Physics Conference Enhncing Network nd Collortion Developing Reserch nd Eduction in Physics nd Nucler Energy Septemer 6-9, 007, Yogykrt-Indonesi Creting A New Plnck s Formul of Spectrl

More information

Edexcel GCE Core Mathematics (C2) Required Knowledge Information Sheet. Daniel Hammocks

Edexcel GCE Core Mathematics (C2) Required Knowledge Information Sheet. Daniel Hammocks Edexcel GCE Core Mthemtics (C) Required Knowledge Informtion Sheet C Formule Given in Mthemticl Formule nd Sttisticl Tles Booklet Cosine Rule o = + c c cosine (A) Binomil Series o ( + ) n = n + n 1 n 1

More information

PHYS Summer Professor Caillault Homework Solutions. Chapter 2

PHYS Summer Professor Caillault Homework Solutions. Chapter 2 PHYS 1111 - Summer 2007 - Professor Cillult Homework Solutions Chpter 2 5. Picture the Problem: The runner moves long the ovl trck. Strtegy: The distnce is the totl length of trvel, nd the displcement

More information

Lesson 8.1 Graphing Parametric Equations

Lesson 8.1 Graphing Parametric Equations Lesson 8.1 Grphing Prmetric Equtions 1. rete tle for ech pir of prmetric equtions with the given vlues of t.. x t 5. x t 3 c. x t 1 y t 1 y t 3 y t t t {, 1, 0, 1, } t {4,, 0,, 4} t {4, 0,, 4, 8}. Find

More information

ELE B7 Power Systems Engineering. Power System Components Modeling

ELE B7 Power Systems Engineering. Power System Components Modeling Power Systems Engineering Power System Components Modeling Section III : Trnsformer Model Power Trnsformers- CONSTRUCTION Primry windings, connected to the lternting voltge source; Secondry windings, connected

More information

Continuous Random Variables Class 5, Jeremy Orloff and Jonathan Bloom

Continuous Random Variables Class 5, Jeremy Orloff and Jonathan Bloom Lerning Gols Continuous Rndom Vriles Clss 5, 8.05 Jeremy Orloff nd Jonthn Bloom. Know the definition of continuous rndom vrile. 2. Know the definition of the proility density function (pdf) nd cumultive

More information

5: The Definite Integral

5: The Definite Integral 5: The Definite Integrl 5.: Estimting with Finite Sums Consider moving oject its velocity (meters per second) t ny time (seconds) is given y v t = t+. Cn we use this informtion to determine the distnce

More information

Patch Antennas. Chapter Resonant Cavity Analysis

Patch Antennas. Chapter Resonant Cavity Analysis Chpter 4 Ptch Antenns A ptch ntenn is low-profile ntenn consisting of metl lyer over dielectric sustrte nd ground plne. Typiclly, ptch ntenn is fed y microstrip trnsmission line, ut other feed lines such

More information

AMPERE CONGRESS AMPERE on Magnetic Resonance and Related Phenomena. Under the auspices of The GROUPEMENT AMPERE

AMPERE CONGRESS AMPERE on Magnetic Resonance and Related Phenomena. Under the auspices of The GROUPEMENT AMPERE AMPERE 2000 th 30 CONGRESS AMPERE on Mgnetic Resonnce nd Relted Phenomen Lison, Portugl, 23-2 July 2000 Under the uspices of The GROUPEMENT AMPERE Edited y: A.F. MARTINS, A.G. FEIO nd J.G. MOURA Sponsoring

More information

Exercise 5.5: Large-scale log-normal fading

Exercise 5.5: Large-scale log-normal fading Exercise 5.5: Lrge-scle log-norml fding Since the system is designed to hndle propgtion loss of 135 db, outge will hppen when the propgtion loss is 8 db higher thn the deterministic loss of 17 db 135 17

More information

CALCULATED POWDER X-RAY DIFFRACTION LINE PROFILES VIA ABSORPTION

CALCULATED POWDER X-RAY DIFFRACTION LINE PROFILES VIA ABSORPTION 16 17 CALCULATED POWDER X-RAY DFFRACTON LNE PROFLES VA ABSORPTON Keji Liu nd Heifen Chen School of Mteril Science nd Engineering, Shnghi nstitute of Technology, Shnghi, Chin 2233 ABSTRACT We hve clculted

More information

Kinematic Waves. These are waves which result from the conservation equation. t + I = 0. (2)

Kinematic Waves. These are waves which result from the conservation equation. t + I = 0. (2) Introduction Kinemtic Wves These re wves which result from the conservtion eqution E t + I = 0 (1) where E represents sclr density field nd I, its outer flux. The one-dimensionl form of (1) is E t + I

More information

Introduction to Hybrid Beamforming Techniques

Introduction to Hybrid Beamforming Techniques Introduction to ybrid Bemforming Techniques Jmes Chen Advisor : Andy Wu Grdute Institute of Electronics Engineering Ntionl Tiwn University Tipei, Tiwn Mr 3, 205 2 Outline Introduction of Precoding Why

More information

Vibrational Relaxation of HF (v=3) + CO

Vibrational Relaxation of HF (v=3) + CO Journl of the Koren Chemicl Society 26, Vol. 6, No. 6 Printed in the Republic of Kore http://dx.doi.org/.52/jkcs.26.6.6.462 Notes Vibrtionl Relxtion of HF (v3) + CO Chng Soon Lee Deprtment of Chemistry,

More information

Thomas Whitham Sixth Form

Thomas Whitham Sixth Form Thoms Whithm Sith Form Pure Mthemtics Unit C Alger Trigonometry Geometry Clculus Vectors Trigonometry Compound ngle formule sin sin cos cos Pge A B sin Acos B cos Asin B A B sin Acos B cos Asin B A B cos

More information

Transmitter-receiver-transmitter configurations of ground-penetrating radar

Transmitter-receiver-transmitter configurations of ground-penetrating radar RADIO SCIENCE, VOL. 37, NO. 3, 1033, 10.1029/2001RS002500, 2002 Trnsmitter-receiver-trnsmitter configurtions of ground-penetrting rdr Levent Gürel nd Uğur Oğuz Deprtment of Electricl nd Electronics Engineering,

More information

FORM FIVE ADDITIONAL MATHEMATIC NOTE. ar 3 = (1) ar 5 = = (2) (2) (1) a = T 8 = 81

FORM FIVE ADDITIONAL MATHEMATIC NOTE. ar 3 = (1) ar 5 = = (2) (2) (1) a = T 8 = 81 FORM FIVE ADDITIONAL MATHEMATIC NOTE CHAPTER : PROGRESSION Arithmetic Progression T n = + (n ) d S n = n [ + (n )d] = n [ + Tn ] S = T = T = S S Emple : The th term of n A.P. is 86 nd the sum of the first

More information

Homework Assignment 6 Solution Set

Homework Assignment 6 Solution Set Homework Assignment 6 Solution Set PHYCS 440 Mrch, 004 Prolem (Griffiths 4.6 One wy to find the energy is to find the E nd D fields everywhere nd then integrte the energy density for those fields. We know

More information

Things to Memorize: A Partial List. January 27, 2017

Things to Memorize: A Partial List. January 27, 2017 Things to Memorize: A Prtil List Jnury 27, 2017 Chpter 2 Vectors - Bsic Fcts A vector hs mgnitude (lso clled size/length/norm) nd direction. It does not hve fixed position, so the sme vector cn e moved

More information

Harmonic Mean Derivative - Based Closed Newton Cotes Quadrature

Harmonic Mean Derivative - Based Closed Newton Cotes Quadrature IOSR Journl of Mthemtics (IOSR-JM) e-issn: - p-issn: 9-X. Volume Issue Ver. IV (My. - Jun. 0) PP - www.iosrjournls.org Hrmonic Men Derivtive - Bsed Closed Newton Cotes Qudrture T. Rmchndrn D.Udykumr nd

More information

Date Lesson Text TOPIC Homework. Solving for Obtuse Angles QUIZ ( ) More Trig Word Problems QUIZ ( )

Date Lesson Text TOPIC Homework. Solving for Obtuse Angles QUIZ ( ) More Trig Word Problems QUIZ ( ) UNIT 5 TRIGONOMETRI RTIOS Dte Lesson Text TOPI Homework pr. 4 5.1 (48) Trigonometry Review WS 5.1 # 3 5, 9 11, (1, 13)doso pr. 6 5. (49) Relted ngles omplete lesson shell & WS 5. pr. 30 5.3 (50) 5.3 5.4

More information

(See Notes on Spontaneous Emission)

(See Notes on Spontaneous Emission) ECE 240 for Cvity from ECE 240 (See Notes on ) Quntum Rdition in ECE 240 Lsers - Fll 2017 Lecture 11 1 Free Spce ECE 240 for Cvity from Quntum Rdition in The electromgnetic mode density in free spce is

More information

Name Solutions to Test 3 November 8, 2017

Name Solutions to Test 3 November 8, 2017 Nme Solutions to Test 3 November 8, 07 This test consists of three prts. Plese note tht in prts II nd III, you cn skip one question of those offered. Some possibly useful formuls cn be found below. Brrier

More information

8.6 The Hyperbola. and F 2. is a constant. P F 2. P =k The two fixed points, F 1. , are called the foci of the hyperbola. The line segments F 1

8.6 The Hyperbola. and F 2. is a constant. P F 2. P =k The two fixed points, F 1. , are called the foci of the hyperbola. The line segments F 1 8. The Hperol Some ships nvigte using rdio nvigtion sstem clled LORAN, which is n cronm for LOng RAnge Nvigtion. A ship receives rdio signls from pirs of trnsmitting sttions tht send signls t the sme time.

More information

Physics 201 Lab 3: Measurement of Earth s local gravitational field I Data Acquisition and Preliminary Analysis Dr. Timothy C. Black Summer I, 2018

Physics 201 Lab 3: Measurement of Earth s local gravitational field I Data Acquisition and Preliminary Analysis Dr. Timothy C. Black Summer I, 2018 Physics 201 Lb 3: Mesurement of Erth s locl grvittionl field I Dt Acquisition nd Preliminry Anlysis Dr. Timothy C. Blck Summer I, 2018 Theoreticl Discussion Grvity is one of the four known fundmentl forces.

More information

Numerical Analysis: Trapezoidal and Simpson s Rule

Numerical Analysis: Trapezoidal and Simpson s Rule nd Simpson s Mthemticl question we re interested in numericlly nswering How to we evlute I = f (x) dx? Clculus tells us tht if F(x) is the ntiderivtive of function f (x) on the intervl [, b], then I =

More information

Chapter E - Problems

Chapter E - Problems Chpter E - Prolems Blinn College - Physics 2426 - Terry Honn Prolem E.1 A wire with dimeter d feeds current to cpcitor. The chrge on the cpcitor vries with time s QHtL = Q 0 sin w t. Wht re the current

More information

Fully Complex Optical Modulation with an Analogue Ferroelectric Liquid Crystal Spatial Light Modulator

Fully Complex Optical Modulation with an Analogue Ferroelectric Liquid Crystal Spatial Light Modulator Full Comple Opticl Modultion with n Anlogue Ferroelectric Liquid Crstl Sptil Light Modultor Philip Birch Rupert Young Chris Chtwin Mri Frsri Dvid Budgett John Richrdson. School of Engineering Universit

More information

Discrete Mathematics and Probability Theory Summer 2014 James Cook Note 17

Discrete Mathematics and Probability Theory Summer 2014 James Cook Note 17 CS 70 Discrete Mthemtics nd Proility Theory Summer 2014 Jmes Cook Note 17 I.I.D. Rndom Vriles Estimting the is of coin Question: We wnt to estimte the proportion p of Democrts in the US popultion, y tking

More information

Review of Gaussian Quadrature method

Review of Gaussian Quadrature method Review of Gussin Qudrture method Nsser M. Asi Spring 006 compiled on Sundy Decemer 1, 017 t 09:1 PM 1 The prolem To find numericl vlue for the integrl of rel vlued function of rel vrile over specific rnge

More information

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 A NON-CONTACT SYSTEM FOR TRANSPORTING OBJECTS USING ULTRASONIC LEVITATION

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 A NON-CONTACT SYSTEM FOR TRANSPORTING OBJECTS USING ULTRASONIC LEVITATION 19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, -7 SEPTEMBER 007 A NON-CONTACT SYSTEM FOR TRANSPORTING OBJECTS USING ULTRASONIC LEVITATION PACS: 3.5.Uv Gudr, Tdeusz 1 ; Perkowski, Dniel ; Opielinski,

More information

Using air lines as references for VNA phase measurements

Using air lines as references for VNA phase measurements Using ir lines s references for VNA phse mesurements Stephen Protheroe nd Nick Ridler Electromgnetics Tem, Ntionl Physicl Lbortory, UK Emil: Stephen.protheroe@npl.co.uk Abstrct Air lines re often used

More information

Jackson 2.26 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Jackson 2.26 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell Jckson 2.26 Homework Problem Solution Dr. Christopher S. Bird University of Msschusetts Lowell PROBLEM: The two-dimensionl region, ρ, φ β, is bounded by conducting surfces t φ =, ρ =, nd φ = β held t zero

More information

Designing Information Devices and Systems I Discussion 8B

Designing Information Devices and Systems I Discussion 8B Lst Updted: 2018-10-17 19:40 1 EECS 16A Fll 2018 Designing Informtion Devices nd Systems I Discussion 8B 1. Why Bother With Thévenin Anywy? () Find Thévenin eqiuvlent for the circuit shown elow. 2kΩ 5V

More information

Definition of Continuity: The function f(x) is continuous at x = a if f(a) exists and lim

Definition of Continuity: The function f(x) is continuous at x = a if f(a) exists and lim Mth 9 Course Summry/Study Guide Fll, 2005 [1] Limits Definition of Limit: We sy tht L is the limit of f(x) s x pproches if f(x) gets closer nd closer to L s x gets closer nd closer to. We write lim f(x)

More information

The area under the graph of f and above the x-axis between a and b is denoted by. f(x) dx. π O

The area under the graph of f and above the x-axis between a and b is denoted by. f(x) dx. π O 1 Section 5. The Definite Integrl Suppose tht function f is continuous nd positive over n intervl [, ]. y = f(x) x The re under the grph of f nd ove the x-xis etween nd is denoted y f(x) dx nd clled the

More information

MASKING OF FERROMAGNETIC ELLIPTICAL SHELL IN TRANSVERSE MAGNETIC FIELD

MASKING OF FERROMAGNETIC ELLIPTICAL SHELL IN TRANSVERSE MAGNETIC FIELD POZNAN UNVE RSTY OF TE HNOLOGY AADE M JOURNALS No 7 Electricl Engineering Kzimierz JAKUUK* Mirosł WOŁOSZYN* Peł ZMNY* MASKNG OF FERROMAGNET ELLPTAL SHELL N TRANSVERSE MAGNET FELD A ferromgnetic oject,

More information

Satellite Retrieval Data Assimilation

Satellite Retrieval Data Assimilation tellite etrievl Dt Assimiltion odgers C. D. Inverse Methods for Atmospheric ounding: Theor nd Prctice World cientific Pu. Co. Hckensck N.J. 2000 Chpter 3 nd Chpter 8 Dve uhl Artist depiction of NAA terr

More information

Alg. Sheet (1) Department : Math Form : 3 rd prep. Sheet

Alg. Sheet (1) Department : Math Form : 3 rd prep. Sheet Ciro Governorte Nozh Directorte of Eduction Nozh Lnguge Schools Ismili Rod Deprtment : Mth Form : rd prep. Sheet Alg. Sheet () [] Find the vlues of nd in ech of the following if : ) (, ) ( -5, 9 ) ) (,

More information

Probabilistic Investigation of Sensitivities of Advanced Test- Analysis Model Correlation Methods

Probabilistic Investigation of Sensitivities of Advanced Test- Analysis Model Correlation Methods Probbilistic Investigtion of Sensitivities of Advnced Test- Anlysis Model Correltion Methods Liz Bergmn, Mtthew S. Allen, nd Dniel C. Kmmer Dept. of Engineering Physics University of Wisconsin-Mdison Rndll

More information

6. Photoionization of acridine through singlet and triplet channels

6. Photoionization of acridine through singlet and triplet channels Chpter 6: Photoioniztion of cridine through singlet nd triplet chnnels 59 6. Photoioniztion of cridine through singlet nd triplet chnnels Photoioinztion of cridine (Ac) in queous micelles hs not yet een

More information

Space Curves. Recall the parametric equations of a curve in xy-plane and compare them with parametric equations of a curve in space.

Space Curves. Recall the parametric equations of a curve in xy-plane and compare them with parametric equations of a curve in space. Clculus 3 Li Vs Spce Curves Recll the prmetric equtions of curve in xy-plne nd compre them with prmetric equtions of curve in spce. Prmetric curve in plne x = x(t) y = y(t) Prmetric curve in spce x = x(t)

More information

MA123, Chapter 10: Formulas for integrals: integrals, antiderivatives, and the Fundamental Theorem of Calculus (pp.

MA123, Chapter 10: Formulas for integrals: integrals, antiderivatives, and the Fundamental Theorem of Calculus (pp. MA123, Chpter 1: Formuls for integrls: integrls, ntiderivtives, nd the Fundmentl Theorem of Clculus (pp. 27-233, Gootmn) Chpter Gols: Assignments: Understnd the sttement of the Fundmentl Theorem of Clculus.

More information

10.2 The Ellipse and the Hyperbola

10.2 The Ellipse and the Hyperbola CHAPTER 0 Conic Sections Solve. 97. Two surveors need to find the distnce cross lke. The plce reference pole t point A in the digrm. Point B is meters est nd meter north of the reference point A. Point

More information

LECTURE 14. Dr. Teresa D. Golden University of North Texas Department of Chemistry

LECTURE 14. Dr. Teresa D. Golden University of North Texas Department of Chemistry LECTURE 14 Dr. Teres D. Golden University of North Texs Deprtment of Chemistry Quntittive Methods A. Quntittive Phse Anlysis Qulittive D phses by comprison with stndrd ptterns. Estimte of proportions of

More information

Lab 11 Approximate Integration

Lab 11 Approximate Integration Nme Student ID # Instructor L Period Dte Due L 11 Approximte Integrtion Ojectives 1. To ecome fmilir with the right endpoint rule, the trpezoidl rule, nd Simpson's rule. 2. To compre nd contrst the properties

More information

Torsion in Groups of Integral Triangles

Torsion in Groups of Integral Triangles Advnces in Pure Mthemtics, 01,, 116-10 http://dxdoiorg/1046/pm011015 Pulished Online Jnury 01 (http://wwwscirporg/journl/pm) Torsion in Groups of Integrl Tringles Will Murry Deprtment of Mthemtics nd Sttistics,

More information

Multi-objective optimization of dielectric layer photonic crystal filter

Multi-objective optimization of dielectric layer photonic crystal filter Optic Applict, Vol. XLVII, No. 1, 017 DOI: 10.577/o170103 Multi-objective optimiztion of dielectric lyer photonic crystl filter HONGWEI YANG *, CUIYING HUANG, SHANSHAN MENG College of Applied Sciences,

More information

k ) and directrix x = h p is A focal chord is a line segment which passes through the focus of a parabola and has endpoints on the parabola.

k ) and directrix x = h p is A focal chord is a line segment which passes through the focus of a parabola and has endpoints on the parabola. Stndrd Eqution of Prol with vertex ( h, k ) nd directrix y = k p is ( x h) p ( y k ) = 4. Verticl xis of symmetry Stndrd Eqution of Prol with vertex ( h, k ) nd directrix x = h p is ( y k ) p( x h) = 4.

More information

Math 124A October 04, 2011

Math 124A October 04, 2011 Mth 4A October 04, 0 Viktor Grigoryn 4 Vibrtions nd het flow In this lecture we will derive the wve nd het equtions from physicl principles. These re second order constnt coefficient liner PEs, which model

More information

Matching patterns of line segments by eigenvector decomposition

Matching patterns of line segments by eigenvector decomposition Title Mtching ptterns of line segments y eigenvector decomposition Author(s) Chn, BHB; Hung, YS Cittion The 5th IEEE Southwest Symposium on Imge Anlysis nd Interprettion Proceedings, Snte Fe, NM., 7-9

More information

Temperature influence compensation in microbolometer detector for image quality enhancement

Temperature influence compensation in microbolometer detector for image quality enhancement .26/qirt.26.68 Temperture influence compenstion in microolometer detector for imge qulity enhncement More info out this rticle: http://www.ndt.net/?id=2647 Astrct y M. Krupiński*, T. Sosnowski*, H. Mdur*

More information

4.1. Probability Density Functions

4.1. Probability Density Functions STT 1 4.1-4. 4.1. Proility Density Functions Ojectives. Continuous rndom vrile - vers - discrete rndom vrile. Proility density function. Uniform distriution nd its properties. Expected vlue nd vrince of

More information

Jack Simons, Henry Eyring Scientist and Professor Chemistry Department University of Utah

Jack Simons, Henry Eyring Scientist and Professor Chemistry Department University of Utah 1. Born-Oppenheimer pprox.- energy surfces 2. Men-field (Hrtree-Fock) theory- orbitls 3. Pros nd cons of HF- RHF, UHF 4. Beyond HF- why? 5. First, one usully does HF-how? 6. Bsis sets nd nottions 7. MPn,

More information

β 1 = 2 π and the path length difference is δ 1 = λ. The small angle approximation gives us y 1 L = tanθ 1 θ 1 sin θ 1 = δ 1 y 1

β 1 = 2 π and the path length difference is δ 1 = λ. The small angle approximation gives us y 1 L = tanθ 1 θ 1 sin θ 1 = δ 1 y 1 rgsdle (zdr8) HW13 ditmire (58335) 1 This print-out should hve 1 questions. Multiple-choice questions my continue on the next column or pge find ll choices before nswering. 001 (prt 1 of ) 10.0 points

More information

AN INEQUALITY OF OSTROWSKI TYPE AND ITS APPLICATIONS FOR SIMPSON S RULE AND SPECIAL MEANS. I. Fedotov and S. S. Dragomir

AN INEQUALITY OF OSTROWSKI TYPE AND ITS APPLICATIONS FOR SIMPSON S RULE AND SPECIAL MEANS. I. Fedotov and S. S. Dragomir RGMIA Reserch Report Collection, Vol., No., 999 http://sci.vu.edu.u/ rgmi AN INEQUALITY OF OSTROWSKI TYPE AND ITS APPLICATIONS FOR SIMPSON S RULE AND SPECIAL MEANS I. Fedotov nd S. S. Drgomir Astrct. An

More information