5th International Conference on Measurement, Instrumentation and Automation (ICMIA 2016) Star image identification uninfluenced by rotation

Size: px
Start display at page:

Download "5th International Conference on Measurement, Instrumentation and Automation (ICMIA 2016) Star image identification uninfluenced by rotation"

Transcription

1 5th Internatonal Conference on Measurement, Instrumentaton and Automaton (ICMIA 2016) Star mage dentfcaton unnfluenced by rotaton Jang D1,a, Zhang Ke1, Lv Mebo1 1 Nortwestern Polytechncal Unversty, X an, Chna a cndyjangd@sna.com Key words: mage dentfcaton; rotaton; star sensor; gude catalog Abstract: All-sky autonomous star map dentfcaton has come up wth hgher requrement on calculatng speed and storage space. Error caused by rotaton and locaton nose nfluences the performance of star mage dentfcaton algorthms. So varous algorthms nclude procedure of rotatng star mage to the poston where the algorthm plans. That wll have a negatve effect on enhancng the performance of dentfcaton. Ths paper presented a recognton method unnfluenced by rotaton. The rotaton error s elmnated automatcally n recognton course. Both poston and magntude nformaton are consdered n t. The smulaton result ndcates that t cost less storage space and the accuracy was ncreased. Introducton It often occurs that gude stars are rotated off ther actual postons when star mages are photographed n CCD cameras[1]. Thus, most star dentfcaton methods come up wth procedures ncludng rotatng the stars to postons they plan. For eample, the grd algorthm. However, the speed of dentfcaton wll be reduced f we conduct rotaton procedures. On the other hand, stars magntude s often gnored n the match between mages acqured and those n gude star database[2][3]. Ths artcle presents an algorthm elmnatng the rotaton n star mages observed. It also takes star magntude nto consderaton to dentfy stars n mages. Method descrptons The algorthm chooses stars n Hpparcos catalog wth magntude lower than 7 to buld a gude catalog for gudance stars. The catalog contans 7548 stars. In the meantme, we assume that the star sensor s feld of vew s 12 by 12, and the sze of mage plane s 512 by 512 pels. Method to generate star mages for match N cos δ sn(α α ) = 2 tan(fov / 2) (sn δ sn δ + cos δ cos δ cos(α α )) N y (sn δ cos δ cos δ sn δ cos(α α )) y = 2 tan(fovy / 2) (sn δ sn δ + cos δ cos δ cos(α α )) (1) Equaton (1) s used to calculate the coordnate (,y) of each star captured by CCD camera. In Equaton (1), δ rght ascenson of each star n the star table chosen, α declnaton of each star n the star table chosen, δ rght ascenson of the star whch s ponted to by as of vew, α declnaton of the star whch s ponted to by as of vew The authors - Publshed by Atlants Press 673

2 The sze of mage plane s N N y, whch s pels here, The star sensor s feld of vew s FOV FOV y, whch s here. The stars magntude M s converted to grayscale G accordng to Equaton (2). 255 G= 2.51 M 1 (2) Fgure 1 llustrates an eample of star mage n gude star database. It s generated va smulaton accordng to Equaton (1) and (2) wthout rotaton. In Fgure 1, camera s as of vew ponts to the star of rght ascenson 41h and declnaton 1h 2 54 wth magntudes shown as gray scale of star spots.it s smplfed so as to be observed more clearly. Gude templates In ths artcle we regard rght ascenson and declnaton of each star n Hpparcos catalog n celestal coordnate system as the drecton of vsual as and smulate ts correspondng star mage, then we acqure 7548 star mages. They are regarded as gude templates. In fact, the algorthm doesn t smulate mages, but only calculate out 7548 matres of gray scales correspondng to these star mages. So the calculaton speed can be enhanced. Then we calculate the features of these templates. We defne the feature as below. m k P = G () ( ) + ( y y ) (3) 2 2 k = 1 In Equaton (3), P k refers to the k th feature and the sequence numbers of the features are the same wth the stars sequence numbers n gude star catalog; s the sequence number of the stars captured n the k th star mage, and the sequence number s made from left to rght and from top to bottom n the mage; G () s the grayscale of the th star n the mage; and y are star spot s coordnate values n mage space coordnate system ; and y refer to the of the mage and they are all 256 here. That s to say, there are 7548 features as the bass for pattern match afterwards. Moreover, we store the grayscale of central pel of the mages whch are taken as gude templates [4]. And we gve these grayscales the same sequence numbers wth the features [5]. We defne the star whch satsfes the condtons below as the man star n the star mage observed. The condtons are: t has the magntude lower than the other stars wthn a range. The range s that the angular separaton between the man star and the others s less than p FOV. In ths artcle, we set p = 0.3. It s possble that an observed mage wll contan several man stars. The algorthm chooses the man star whch s nearest to the center of the mage as the only man star. Then we translate ths star to the center. And wth ths procedure, the whole mage s translated. In order to elmnate the nfluence of translaton to the greatest etent, we epand the mage to the sze of 1.5N. Thus a new mage on the bass of the former one s generated. After ths step, we calculate the feature P of the new mage accordng to Equaton (4). m 2 2 ( ) ( j ) ( j ) (4) j= 1 P= G j + y y j s the sequence number of the spot whch satsfes Equaton (5) and has a brghtness larger than 0 n the observed star mage and the sequence number s made from left to rght and from top to bottom n the mage; 674

3 2 2 2 ( j ) ( yj y) R R=512 +, (5) G( j ) s the grayscale of the jth star n the mage; and y are star spot s coordnate values n mage space coordnate system ; j j and y refer to the of the mage and they are all 384 here. observaton templates The algorthm presented n ths paper constructed an observaton template as s llustrated. When calculatng the feature of the observaton template, the star spot out of the range of Equaton (5) won t be ncluded because we ntend to fnd the stars whch can match those n one gude template around the only man star. The purpose of epandng the feld of vew when constructng observaton template s to avod loss n the course of translaton. P s compared wth P ( = 1,2, L, k) one by one. The gude templates whch the algorthm s searchng for has feature that s at the same order of magntude wth P. We need to set a threshold value for match course. If the dfference between P and P s less than the threshold value, then the gude template correspondng to P s possble to be the match concluson. Ths s the ntal fltrate course. If a gude template has a feature satsfyng the threshold value, we compare the grayscale value of the central pel n ts grayscale matr wth the grayscale value of the central pel n observed star mage. The former grayscale value s stored n advance. Theoretcally, f the two grayscale values are equal to each other, the algorthm wll certfy the star correspondng to gude template s the man star n observed star mage. Smulaton eamples In order to verfy the algorthm n ths artcle, we generated a star mage as s shown n Fgure2 wth a random drecton of vsual as and assume that t s the mage observed through star sensor n operaton. Fgure 2 contans more than 10 man stars. The algorthm certfed that the only man star s the pel spot of the coordnate (226,213) n the mage. Its grayscale s Then the mage was translated so that the man star could be at the center of the new mage generated by translaton, as s shown n Fgure 3. It corresponds to a grayscale matr J. Accordng to Equaton (4), the feature 4 of J s P= Fgure 1 Images n database of gudng stars Fgure 2 Star mage observed by star sensor In ths eample, we set 150 as the threshold value. The result of match s the gude template 4 No.1648 wth P = and the grayscale value of the central pel n the 1648th gude

4 template s equal to We smulated the star mage of No.1648 as s shown n Fgure 4 to prove the result s accurate. Fgure 3 Star mage observed after translaton Fgure 4 the gude template No.1648 The spot of coordnate (226,213) n Fgure 2 s eactly the central star n Fgure 4. It means that the star whch s represented by the spot of coordnate (226,213) n Fgure 2 s the 1648th star n gude catalog. The star has rght ascenson 11h and declnaton -10h It can be seen that even f rotaton error s added to the mage observed, ts feature won t change. That s decded by the defnton of the feature. So n the course of star mage dentfcaton, the rotaton off orgnal star postons can be totally elmnated. The part above presented the effectveness of the algorthm n dealzed condton. It can be nferred that f Equaton (4) s used to calculate the feature of mages wth nose, the spots wth grayscale more than 0 wll ncrease a lot. And ths won t accord wth the real stuaton. To solve the problem, the algorthm adopted a lmtng prncple that only f the pel has the grayscale value more than that of Grade 7 star, ts grayscale wll be ncluded to calculate the feature of star mage. 71 That means addng a constrant condtong( j) 255/2.51 = to Equaton (4). In observed star mages wth nose, the result of pattern dentfcaton may be that several gude templates all satsfy the constrant condton set by the algorthm. At that tme, the algorthm wll choose the gude template whch has the least dfference n feature and central pel s magntude wth observaton template. Epermental results We generated 1000 drectons of vsual as randomly to test the success rate of man star dentfcaton. In the condton where grayscale value nose of 0.1 unts standard devaton and locaton nose of 0.5 pels standard devaton (nose referred to n ths paper are all Gaussan nose) were added to observed star mages, the rate that the only man star of each observed star mage was recognzed successfully s 95.7%. Performance on elmnatng error Seen from the smulaton result, the algorthm s performance to elmnate error caused by rotaton n captured star mage s obvous. For eample, Fgure 5 s an mage smulated as observed star mage contanng grayscale value nose of 0.1 unts standard devaton and locaton nose of 0.5 pels standard devaton. By the algorthm n ths paper, we got the result of star mage dentfcaton, whch was that the only man star n Fgure 5 s the 1800th star n gude star catalog. When we set the drecton of vsual as as the drecton of that star [6], we got the gude template correspondng to the observed mage, as s llustrated n Fgure

5 Fgure 5 observed mage Fgure 6 result of dentfcaton We can see that the two mages are almost opposte to each other, however, the result of match s accurate. Actually there was no procedure of rotaton n the course of star pattern recognton, but the result showed that the algorthm could dentfy the man star correctly even there was a large etent of rotaton between the observed mage and gude template. performance comparson The performances of trangle algorthm, match group algorthm, grd algorthm and the algorthm n ths artcle are shown n Table 1 [7][8]. The operaton condton of the three algorthms s the same wth that of the algorthm presented n ths paper. Table 1 Performance comparson of varous dentfcaton algorthms Algorthm Run tme(s) Memory requrement(mb) Trangle Match group Grd Method of ths artcle We can see that the memory cost of ths algorthm s a lot less compared wth the other three algorthms n Table 1. That s because t only needs space to store the features of dfferent gude templates and magntudes of gude stars. In Fgure 7, four curves represent the percentage of star felds dentfed over 500 random orentatons of the sensor. The locaton error was held constant wth a standard devaton of 0.5 pels. The standard devaton for the brghtness error s shown along the horzontal as n unts stellar magntude. In Fgure 8, four curves represent the percentage of star felds dentfed over 500 random orentatons of the sensor. The brghtness error was held constant wth a standard devaton of 0.3 unts stellar magntude. The standard devaton for the locaton error s shown along the horzontal as n pels. Conclusons Ths artcle presented algorthm for star mage dentfcaton unnfluenced by rotaton. The feature defned n the algorthm elmnates the nfluence from rotaton error. Thus the procedure for mage processng before pattern recognton can be elmnated. That s an advantage compared wth tradtonal algorthms of star mage dentfcaton. The result of smulaton ndcated the 677

6 performance of ths algorthm aganst locaton error and magntude error s ecellent and the tme and storage cost for dentfcaton s optmzed. 100 Fgure 7 Rate of dentfcaton wth several methods wth magntude error changng rate of dentfcaton(%) grd trangle match group method n artcle locaton error n p els Fgure 8 Rate of dentfcaton wth several methods wth locaton error changng References [1] Zhang Le, He Xn, We Zhonghu, Lu Yanjun, and Guo Jngmng. Modfcaton of trangle dentfcaton algorthm [J]. Optcs and precson engneerng. 2010, (2): [2] Ln Tao, Zhou Janl, Zhang Junpng, Ja Xaoguang, and Qan Guohu. All-sky automated quaternary star pattern recognton [J]. Journal of astronautcs. 2000, 21(2) : [3] Zhang Shaod, Wang Yanje, and Sun Hongha. Applcaton of trangulaton and RBF neural network to star pattern recognton[j]. Optcs and precson engneerng. 2012, (2): [4] LI L-hong, XU Hong-ze, ZHANG Fu-en. A knd of mproved grd algorthm for all-sky autonomous star feld dentfcaton [J], Optcal Technque, 2000, 26(3): [5] We Xn-guo, Zhang Guang-jun, Jang Je. A star map dentfcaton algorthm usng radal and cyclc features [J], Opto-Electronc Engneerng, 2004, 31(8): 4-7. [6] Padgett C, Kreutz-Delgado K, Udomkesmalee S. Evaluaton of star dentfcaton technques[j], Journal of Gudance, Control and Dynamcs, 1997, 20(2): [7] M. S. Scholl. Star-Feld Identfcaton for Autonomous Atttude Determnaton [J]. Journal of Gudance, control and dynamcs, 1995,18(1): [8] K.Ho. A survey of algorthms for star dentfcaton wth low-cost star trackers [J]. Acta astronautca. 2012, (73):

Laboratory Test System Design for Star Sensor Performance Evaluation

Laboratory Test System Design for Star Sensor Performance Evaluation 1056 JOURNAL OF COMPUTERS, VOL. 7, NO. 4, APRIL 2012 Laboratory Test System Desgn for Star Sensor Performance Evaluaton Jun Yang, Bn Lang, Tao Zhang, Jngyan Song and Langlang Song Department of Automaton,

More information

An Improved multiple fractal algorithm

An Improved multiple fractal algorithm Advanced Scence and Technology Letters Vol.31 (MulGraB 213), pp.184-188 http://dx.do.org/1.1427/astl.213.31.41 An Improved multple fractal algorthm Yun Ln, Xaochu Xu, Jnfeng Pang College of Informaton

More information

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH Turbulence classfcaton of load data by the frequency and severty of wnd gusts Introducton Oscar Moñux, DEWI GmbH Kevn Blebler, DEWI GmbH Durng the wnd turbne developng process, one of the most mportant

More information

The Study of Teaching-learning-based Optimization Algorithm

The Study of Teaching-learning-based Optimization Algorithm Advanced Scence and Technology Letters Vol. (AST 06), pp.05- http://dx.do.org/0.57/astl.06. The Study of Teachng-learnng-based Optmzaton Algorthm u Sun, Yan fu, Lele Kong, Haolang Q,, Helongang Insttute

More information

829. An adaptive method for inertia force identification in cantilever under moving mass

829. An adaptive method for inertia force identification in cantilever under moving mass 89. An adaptve method for nerta force dentfcaton n cantlever under movng mass Qang Chen 1, Mnzhuo Wang, Hao Yan 3, Haonan Ye 4, Guola Yang 5 1,, 3, 4 Department of Control and System Engneerng, Nanng Unversty,

More information

Operating conditions of a mine fan under conditions of variable resistance

Operating conditions of a mine fan under conditions of variable resistance Paper No. 11 ISMS 216 Operatng condtons of a mne fan under condtons of varable resstance Zhang Ynghua a, Chen L a, b, Huang Zhan a, *, Gao Yukun a a State Key Laboratory of Hgh-Effcent Mnng and Safety

More information

REAL-TIME DETERMINATION OF INDOOR CONTAMINANT SOURCE LOCATION AND STRENGTH, PART II: WITH TWO SENSORS. Beijing , China,

REAL-TIME DETERMINATION OF INDOOR CONTAMINANT SOURCE LOCATION AND STRENGTH, PART II: WITH TWO SENSORS. Beijing , China, REAL-TIME DETERMIATIO OF IDOOR COTAMIAT SOURCE LOCATIO AD STREGTH, PART II: WITH TWO SESORS Hao Ca,, Xantng L, Wedng Long 3 Department of Buldng Scence, School of Archtecture, Tsnghua Unversty Bejng 84,

More information

Improvement of Histogram Equalization for Minimum Mean Brightness Error

Improvement of Histogram Equalization for Minimum Mean Brightness Error Proceedngs of the 7 WSEAS Int. Conference on Crcuts, Systems, Sgnal and elecommuncatons, Gold Coast, Australa, January 7-9, 7 3 Improvement of Hstogram Equalzaton for Mnmum Mean Brghtness Error AAPOG PHAHUA*,

More information

Report on Image warping

Report on Image warping Report on Image warpng Xuan Ne, Dec. 20, 2004 Ths document summarzed the algorthms of our mage warpng soluton for further study, and there s a detaled descrpton about the mplementaton of these algorthms.

More information

SCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors.

SCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors. SCALARS AND ECTORS All phscal uanttes n engneerng mechancs are measured usng ether scalars or vectors. Scalar. A scalar s an postve or negatve phscal uantt that can be completel specfed b ts magntude.

More information

CONTRAST ENHANCEMENT FOR MIMIMUM MEAN BRIGHTNESS ERROR FROM HISTOGRAM PARTITIONING INTRODUCTION

CONTRAST ENHANCEMENT FOR MIMIMUM MEAN BRIGHTNESS ERROR FROM HISTOGRAM PARTITIONING INTRODUCTION CONTRAST ENHANCEMENT FOR MIMIMUM MEAN BRIGHTNESS ERROR FROM HISTOGRAM PARTITIONING N. Phanthuna 1,2, F. Cheevasuvt 2 and S. Chtwong 2 1 Department of Electrcal Engneerng, Faculty of Engneerng Rajamangala

More information

Image Processing for Bubble Detection in Microfluidics

Image Processing for Bubble Detection in Microfluidics Image Processng for Bubble Detecton n Mcrofludcs Introducton Chen Fang Mechancal Engneerng Department Stanford Unverst Startng from recentl ears, mcrofludcs devces have been wdel used to buld the bomedcal

More information

International Power, Electronics and Materials Engineering Conference (IPEMEC 2015)

International Power, Electronics and Materials Engineering Conference (IPEMEC 2015) Internatonal Power, Electroncs and Materals Engneerng Conference (IPEMEC 2015) Dynamc Model of Wnd Speed Dstrbuton n Wnd Farm Consderng the Impact of Wnd Drecton and Interference Effects Zhe Dong 1, a,

More information

Kernel Methods and SVMs Extension

Kernel Methods and SVMs Extension Kernel Methods and SVMs Extenson The purpose of ths document s to revew materal covered n Machne Learnng 1 Supervsed Learnng regardng support vector machnes (SVMs). Ths document also provdes a general

More information

Army Ants Tunneling for Classical Simulations

Army Ants Tunneling for Classical Simulations Electronc Supplementary Materal (ESI) for Chemcal Scence. Ths journal s The Royal Socety of Chemstry 2014 electronc supplementary nformaton (ESI) for Chemcal Scence Army Ants Tunnelng for Classcal Smulatons

More information

Tutorial 2. COMP4134 Biometrics Authentication. February 9, Jun Xu, Teaching Asistant

Tutorial 2. COMP4134 Biometrics Authentication. February 9, Jun Xu, Teaching Asistant Tutoral 2 COMP434 ometrcs uthentcaton Jun Xu, Teachng sstant csjunxu@comp.polyu.edu.hk February 9, 207 Table of Contents Problems Problem : nswer the questons Problem 2: Power law functon Problem 3: Convoluton

More information

The Order Relation and Trace Inequalities for. Hermitian Operators

The Order Relation and Trace Inequalities for. Hermitian Operators Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence

More information

Using Immune Genetic Algorithm to Optimize BP Neural Network and Its Application Peng-fei LIU1,Qun-tai SHEN1 and Jun ZHI2,*

Using Immune Genetic Algorithm to Optimize BP Neural Network and Its Application Peng-fei LIU1,Qun-tai SHEN1 and Jun ZHI2,* Advances n Computer Scence Research (ACRS), volume 54 Internatonal Conference on Computer Networks and Communcaton Technology (CNCT206) Usng Immune Genetc Algorthm to Optmze BP Neural Network and Its Applcaton

More information

VQ widely used in coding speech, image, and video

VQ widely used in coding speech, image, and video at Scalar quantzers are specal cases of vector quantzers (VQ): they are constraned to look at one sample at a tme (memoryless) VQ does not have such constrant better RD perfomance expected Source codng

More information

CS 468 Lecture 16: Isometry Invariance and Spectral Techniques

CS 468 Lecture 16: Isometry Invariance and Spectral Techniques CS 468 Lecture 16: Isometry Invarance and Spectral Technques Justn Solomon Scrbe: Evan Gawlk Introducton. In geometry processng, t s often desrable to characterze the shape of an object n a manner that

More information

Comparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy

Comparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy Comparatve Studes of Law of Conservaton of Energy and Law Clusters of Conservaton of Generalzed Energy No.3 of Comparatve Physcs Seres Papers Fu Yuhua (CNOOC Research Insttute, E-mal:fuyh1945@sna.com)

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle

More information

on the improved Partial Least Squares regression

on the improved Partial Least Squares regression Internatonal Conference on Manufacturng Scence and Engneerng (ICMSE 05) Identfcaton of the multvarable outlers usng T eclpse chart based on the mproved Partal Least Squares regresson Lu Yunlan,a X Yanhu,b

More information

Spatial Statistics and Analysis Methods (for GEOG 104 class).

Spatial Statistics and Analysis Methods (for GEOG 104 class). Spatal Statstcs and Analyss Methods (for GEOG 104 class). Provded by Dr. An L, San Dego State Unversty. 1 Ponts Types of spatal data Pont pattern analyss (PPA; such as nearest neghbor dstance, quadrat

More information

Experience with Automatic Generation Control (AGC) Dynamic Simulation in PSS E

Experience with Automatic Generation Control (AGC) Dynamic Simulation in PSS E Semens Industry, Inc. Power Technology Issue 113 Experence wth Automatc Generaton Control (AGC) Dynamc Smulaton n PSS E Lu Wang, Ph.D. Staff Software Engneer lu_wang@semens.com Dngguo Chen, Ph.D. Staff

More information

Physics 111: Mechanics Lecture 11

Physics 111: Mechanics Lecture 11 Physcs 111: Mechancs Lecture 11 Bn Chen NJIT Physcs Department Textbook Chapter 10: Dynamcs of Rotatonal Moton q 10.1 Torque q 10. Torque and Angular Acceleraton for a Rgd Body q 10.3 Rgd-Body Rotaton

More information

A Robust Method for Calculating the Correlation Coefficient

A Robust Method for Calculating the Correlation Coefficient A Robust Method for Calculatng the Correlaton Coeffcent E.B. Nven and C. V. Deutsch Relatonshps between prmary and secondary data are frequently quantfed usng the correlaton coeffcent; however, the tradtonal

More information

find (x): given element x, return the canonical element of the set containing x;

find (x): given element x, return the canonical element of the set containing x; COS 43 Sprng, 009 Dsjont Set Unon Problem: Mantan a collecton of dsjont sets. Two operatons: fnd the set contanng a gven element; unte two sets nto one (destructvely). Approach: Canoncal element method:

More information

arxiv:cs.cv/ Jun 2000

arxiv:cs.cv/ Jun 2000 Correlaton over Decomposed Sgnals: A Non-Lnear Approach to Fast and Effectve Sequences Comparson Lucano da Fontoura Costa arxv:cs.cv/0006040 28 Jun 2000 Cybernetc Vson Research Group IFSC Unversty of São

More information

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI 2017 2nd Internatonal Conference on Electrcal and Electroncs: echnques and Applcatons (EEA 2017) ISBN: 978-1-60595-416-5 Study on Actve Mcro-vbraton Isolaton System wth Lnear Motor Actuator Gong-yu PAN,

More information

Fiber Optic Gyroscope Dynamic North-Finder Algorithm Modeling and Analysis Based on Simulink

Fiber Optic Gyroscope Dynamic North-Finder Algorithm Modeling and Analysis Based on Simulink PHOTONIC SENSORS / Vol. 7, No. 3, 17: 83 88 Fber Optc Gyroscope Dynamc North-Fnder Algorthm Modelng and Analyss Based on Smulnk Zhengy ZHANG * and Chuntong LIU Department Two, Rocket Force Unversty of

More information

Conservation of Angular Momentum = "Spin"

Conservation of Angular Momentum = Spin Page 1 of 6 Conservaton of Angular Momentum = "Spn" We can assgn a drecton to the angular velocty: drecton of = drecton of axs + rght hand rule (wth rght hand, curl fngers n drecton of rotaton, thumb ponts

More information

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification Desgn Project Specfcaton Medan Flter Department of Electrcal & Electronc Engneeng Imperal College London E4.20 Dgtal IC Desgn Medan Flter Project Specfcaton A medan flter s used to remove nose from a sampled

More information

An Algorithm to Solve the Inverse Kinematics Problem of a Robotic Manipulator Based on Rotation Vectors

An Algorithm to Solve the Inverse Kinematics Problem of a Robotic Manipulator Based on Rotation Vectors An Algorthm to Solve the Inverse Knematcs Problem of a Robotc Manpulator Based on Rotaton Vectors Mohamad Z. Al-az*, Mazn Z. Othman**, and Baker B. Al-Bahr* *AL-Nahran Unversty, Computer Eng. Dep., Baghdad,

More information

Chapter 13: Multiple Regression

Chapter 13: Multiple Regression Chapter 13: Multple Regresson 13.1 Developng the multple-regresson Model The general model can be descrbed as: It smplfes for two ndependent varables: The sample ft parameter b 0, b 1, and b are used to

More information

Power law and dimension of the maximum value for belief distribution with the max Deng entropy

Power law and dimension of the maximum value for belief distribution with the max Deng entropy Power law and dmenson of the maxmum value for belef dstrbuton wth the max Deng entropy Bngy Kang a, a College of Informaton Engneerng, Northwest A&F Unversty, Yanglng, Shaanx, 712100, Chna. Abstract Deng

More information

Second Order Analysis

Second Order Analysis Second Order Analyss In the prevous classes we looked at a method that determnes the load correspondng to a state of bfurcaton equlbrum of a perfect frame by egenvalye analyss The system was assumed to

More information

11. Dynamics in Rotating Frames of Reference

11. Dynamics in Rotating Frames of Reference Unversty of Rhode Island DgtalCommons@URI Classcal Dynamcs Physcs Course Materals 2015 11. Dynamcs n Rotatng Frames of Reference Gerhard Müller Unversty of Rhode Island, gmuller@ur.edu Creatve Commons

More information

One-sided finite-difference approximations suitable for use with Richardson extrapolation

One-sided finite-difference approximations suitable for use with Richardson extrapolation Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,

More information

Week 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product

Week 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product The Vector Product Week 11: Chapter 11 Angular Momentum There are nstances where the product of two vectors s another vector Earler we saw where the product of two vectors was a scalar Ths was called the

More information

RBF Neural Network Model Training by Unscented Kalman Filter and Its Application in Mechanical Fault Diagnosis

RBF Neural Network Model Training by Unscented Kalman Filter and Its Application in Mechanical Fault Diagnosis Appled Mechancs and Materals Submtted: 24-6-2 ISSN: 662-7482, Vols. 62-65, pp 2383-2386 Accepted: 24-6- do:.428/www.scentfc.net/amm.62-65.2383 Onlne: 24-8- 24 rans ech Publcatons, Swtzerland RBF Neural

More information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information Thrd Chnese-German Jont Symposum on Coastal and Ocean Engneerng Natonal Cheng Kung Unversty, Tanan November 8-16, 2006 Modal Stran Energy Decomposton Method for Damage Detecton of an Offshore Structure

More information

Tracking with Kalman Filter

Tracking with Kalman Filter Trackng wth Kalman Flter Scott T. Acton Vrgna Image and Vdeo Analyss (VIVA), Charles L. Brown Department of Electrcal and Computer Engneerng Department of Bomedcal Engneerng Unversty of Vrgna, Charlottesvlle,

More information

Multi-Robot Formation Control Based on Leader-Follower Optimized by the IGA

Multi-Robot Formation Control Based on Leader-Follower Optimized by the IGA IOSR Journal of Computer Engneerng (IOSR-JCE e-issn: 2278-0661,p-ISSN: 2278-8727, Volume 19, Issue 1, Ver. III (Jan.-Feb. 2017, PP 08-13 www.osrjournals.org Mult-Robot Formaton Control Based on Leader-Follower

More information

Indeterminate pin-jointed frames (trusses)

Indeterminate pin-jointed frames (trusses) Indetermnate pn-jonted frames (trusses) Calculaton of member forces usng force method I. Statcal determnacy. The degree of freedom of any truss can be derved as: w= k d a =, where k s the number of all

More information

A Novel Feistel Cipher Involving a Bunch of Keys supplemented with Modular Arithmetic Addition

A Novel Feistel Cipher Involving a Bunch of Keys supplemented with Modular Arithmetic Addition (IJACSA) Internatonal Journal of Advanced Computer Scence Applcatons, A Novel Festel Cpher Involvng a Bunch of Keys supplemented wth Modular Arthmetc Addton Dr. V.U.K Sastry Dean R&D, Department of Computer

More information

Modeling of Dynamic Systems

Modeling of Dynamic Systems Modelng of Dynamc Systems Ref: Control System Engneerng Norman Nse : Chapters & 3 Chapter objectves : Revew the Laplace transform Learn how to fnd a mathematcal model, called a transfer functon Learn how

More information

Lecture 14: Forces and Stresses

Lecture 14: Forces and Stresses The Nuts and Bolts of Frst-Prncples Smulaton Lecture 14: Forces and Stresses Durham, 6th-13th December 2001 CASTEP Developers Group wth support from the ESF ψ k Network Overvew of Lecture Why bother? Theoretcal

More information

OPTIMISATION. Introduction Single Variable Unconstrained Optimisation Multivariable Unconstrained Optimisation Linear Programming

OPTIMISATION. Introduction Single Variable Unconstrained Optimisation Multivariable Unconstrained Optimisation Linear Programming OPTIMIATION Introducton ngle Varable Unconstraned Optmsaton Multvarable Unconstraned Optmsaton Lnear Programmng Chapter Optmsaton /. Introducton In an engneerng analss, sometmes etremtes, ether mnmum or

More information

Spin-rotation coupling of the angularly accelerated rigid body

Spin-rotation coupling of the angularly accelerated rigid body Spn-rotaton couplng of the angularly accelerated rgd body Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 E-mal: louaelzen@gmal.com November 1, 2017 All Rghts Reserved. Abstract Ths paper s

More information

Uncertainty in measurements of power and energy on power networks

Uncertainty in measurements of power and energy on power networks Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:

More information

Rigid body simulation

Rigid body simulation Rgd bod smulaton Rgd bod smulaton Once we consder an object wth spacal etent, partcle sstem smulaton s no longer suffcent Problems Problems Unconstraned sstem rotatonal moton torques and angular momentum

More information

Chapter - 2. Distribution System Power Flow Analysis

Chapter - 2. Distribution System Power Flow Analysis Chapter - 2 Dstrbuton System Power Flow Analyss CHAPTER - 2 Radal Dstrbuton System Load Flow 2.1 Introducton Load flow s an mportant tool [66] for analyzng electrcal power system network performance. Load

More information

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Physics 5153 Classical Mechanics. Principle of Virtual Work-1 P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal

More information

Design and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm

Design and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm Desgn and Optmzaton of Fuzzy Controller for Inverse Pendulum System Usng Genetc Algorthm H. Mehraban A. Ashoor Unversty of Tehran Unversty of Tehran h.mehraban@ece.ut.ac.r a.ashoor@ece.ut.ac.r Abstract:

More information

Star Tracker Attitude Estimation for an Indoor Ground- Based Spacecraft Simulator

Star Tracker Attitude Estimation for an Indoor Ground- Based Spacecraft Simulator AIAA Modelng and Smulaton echnologes Conference 08 - August 0, Portland, Oregon AIAA 0-670 Star racker Atttude Estmaton for an Indoor Ground- Based Spacecraft Smulator Jack appe, Jae Jun Km, Albert Jordan,

More information

Beyond Zudilin s Conjectured q-analog of Schmidt s problem

Beyond Zudilin s Conjectured q-analog of Schmidt s problem Beyond Zudln s Conectured q-analog of Schmdt s problem Thotsaporn Ae Thanatpanonda thotsaporn@gmalcom Mathematcs Subect Classfcaton: 11B65 33B99 Abstract Usng the methodology of (rgorous expermental mathematcs

More information

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity LINEAR REGRESSION ANALYSIS MODULE IX Lecture - 30 Multcollnearty Dr. Shalabh Department of Mathematcs and Statstcs Indan Insttute of Technology Kanpur 2 Remedes for multcollnearty Varous technques have

More information

Similar Constructing Method for Solving the Boundary Value Problem of the Compound Kummer Equation

Similar Constructing Method for Solving the Boundary Value Problem of the Compound Kummer Equation Amercan Journal of Mathematcal Analyss, 05, Vol. 3, No., 39-43 Avalable onlne at http://pubs.scepub.com/ajma/3//3 Scence and Educaton Publshng DOI:0.69/ajma-3--3 Smlar Constructng Method for Solvng the

More information

A New Scrambling Evaluation Scheme based on Spatial Distribution Entropy and Centroid Difference of Bit-plane

A New Scrambling Evaluation Scheme based on Spatial Distribution Entropy and Centroid Difference of Bit-plane A New Scramblng Evaluaton Scheme based on Spatal Dstrbuton Entropy and Centrod Dfference of Bt-plane Lang Zhao *, Avshek Adhkar Kouch Sakura * * Graduate School of Informaton Scence and Electrcal Engneerng,

More information

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient 58:080 Expermental Engneerng 1 OBJECTIVE Lab 2e Thermal System Response and Effectve Heat Transfer Coeffcent Warnng: though the experment has educatonal objectves (to learn about bolng heat transfer, etc.),

More information

A NEW DEVICE FOR PREDICTING LANDSLIDES

A NEW DEVICE FOR PREDICTING LANDSLIDES Internatonal Journal of Latest Research n Scence and Technology Volume 3, Issue : Page No45-49,March-Aprl, 14 http://wwwmnkjournalscom/jlrsthtm ISSN (Onlne):7-599 A NEW DEVICE FOR PREDICTING LANDSLIDES

More information

So far: simple (planar) geometries

So far: simple (planar) geometries Physcs 06 ecture 5 Torque and Angular Momentum as Vectors SJ 7thEd.: Chap. to 3 Rotatonal quanttes as vectors Cross product Torque epressed as a vector Angular momentum defned Angular momentum as a vector

More information

Performance of Different Algorithms on Clustering Molecular Dynamics Trajectories

Performance of Different Algorithms on Clustering Molecular Dynamics Trajectories Performance of Dfferent Algorthms on Clusterng Molecular Dynamcs Trajectores Chenchen Song Abstract Dfferent types of clusterng algorthms are appled to clusterng molecular dynamcs trajectores to get nsght

More information

Parameter Estimation for Dynamic System using Unscented Kalman filter

Parameter Estimation for Dynamic System using Unscented Kalman filter Parameter Estmaton for Dynamc System usng Unscented Kalman flter Jhoon Seung 1,a, Amr Atya F. 2,b, Alexander G.Parlos 3,c, and Klto Chong 1,4,d* 1 Dvson of Electroncs Engneerng, Chonbuk Natonal Unversty,

More information

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00 ONE IMENSIONAL TRIANGULAR FIN EXPERIMENT Techncal Advsor: r..c. Look, Jr. Verson: /3/ 7. GENERAL OJECTIVES a) To understand a one-dmensonal epermental appromaton. b) To understand the art of epermental

More information

ERROR RESEARCH ON A HEPA FILTER MEDIA TESTING SYSTEM OF MPPS(MOST PENETRATION PARTICLE SIZE) EFFICIENCY

ERROR RESEARCH ON A HEPA FILTER MEDIA TESTING SYSTEM OF MPPS(MOST PENETRATION PARTICLE SIZE) EFFICIENCY Proceedngs: Indoor Ar 2005 ERROR RESEARCH ON A HEPA FILTER MEDIA TESTING SYSTEM OF MPPS(MOST PENETRATION PARTICLE SIZE) EFFICIENCY S Lu, J Lu *, N Zhu School of Envronmental Scence and Technology, Tanjn

More information

CHAPTER 6. LAGRANGE S EQUATIONS (Analytical Mechanics)

CHAPTER 6. LAGRANGE S EQUATIONS (Analytical Mechanics) CHAPTER 6 LAGRANGE S EQUATIONS (Analytcal Mechancs) 1 Ex. 1: Consder a partcle movng on a fxed horzontal surface. r P Let, be the poston and F be the total force on the partcle. The FBD s: -mgk F 1 x O

More information

Grid Generation around a Cylinder by Complex Potential Functions

Grid Generation around a Cylinder by Complex Potential Functions Research Journal of Appled Scences, Engneerng and Technolog 4(): 53-535, 0 ISSN: 040-7467 Mawell Scentfc Organzaton, 0 Submtted: December 0, 0 Accepted: Januar, 0 Publshed: June 0, 0 Grd Generaton around

More information

Errors for Linear Systems

Errors for Linear Systems Errors for Lnear Systems When we solve a lnear system Ax b we often do not know A and b exactly, but have only approxmatons  and ˆb avalable. Then the best thng we can do s to solve ˆx ˆb exactly whch

More information

CSci 6974 and ECSE 6966 Math. Tech. for Vision, Graphics and Robotics Lecture 21, April 17, 2006 Estimating A Plane Homography

CSci 6974 and ECSE 6966 Math. Tech. for Vision, Graphics and Robotics Lecture 21, April 17, 2006 Estimating A Plane Homography CSc 6974 and ECSE 6966 Math. Tech. for Vson, Graphcs and Robotcs Lecture 21, Aprl 17, 2006 Estmatng A Plane Homography Overvew We contnue wth a dscusson of the major ssues, usng estmaton of plane projectve

More information

ˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m)

ˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m) 7.. = = 3 = 4 = 5. The electrc feld s constant everywhere between the plates. Ths s ndcated by the electrc feld vectors, whch are all the same length and n the same drecton. 7.5. Model: The dstances to

More information

Nodal analysis of finite square resistive grids and the teaching effectiveness of students projects

Nodal analysis of finite square resistive grids and the teaching effectiveness of students projects 2 nd World Conference on Technology and Engneerng Educaton 2 WIETE Lublana Slovena 5-8 September 2 Nodal analyss of fnte square resstve grds and the teachng effectveness of students proects P. Zegarmstrz

More information

A Network Intrusion Detection Method Based on Improved K-means Algorithm

A Network Intrusion Detection Method Based on Improved K-means Algorithm Advanced Scence and Technology Letters, pp.429-433 http://dx.do.org/10.14257/astl.2014.53.89 A Network Intruson Detecton Method Based on Improved K-means Algorthm Meng Gao 1,1, Nhong Wang 1, 1 Informaton

More information

High Precision Edge Detection Algorithm for Mechanical Parts

High Precision Edge Detection Algorithm for Mechanical Parts MEASUREMENT SCIENCE REVIEW, 18, (018), No., 65-71 Journal homepage: http://www.degruyter.com/vew/j/msr Hgh Precson Edge Detecton Algorthm for Mechancal Parts Zhenyun Duan 1, Nng Wang 1, Jngshun Fu 1, Wenhu

More information

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

The equation of motion of a dynamical system is given by a set of differential equations. That is (1) Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence

More information

B and H sensors for 3-D magnetic property testing

B and H sensors for 3-D magnetic property testing B and H sensors for 3-D magnetc property testng Zh We Ln, Jan Guo Zhu, You Guang Guo, Jn Jang Zhong, and Ha We Lu Faculty of Engneerng, Unversty of Technology, Sydney, PO Bo 123, Broadway, SW 2007, Australa

More information

Study on Effect of Different Porosity on Thermally Driven Heat Transfer in a Centrifugal Force Field

Study on Effect of Different Porosity on Thermally Driven Heat Transfer in a Centrifugal Force Field 5th Internatonal Conference on Cvl Engneerng and Transportaton (ICCET 015) Study on Effect of Dfferent Porosty on Thermally Drven Heat Transfer n a Centrfugal Force Feld 1 Xa Je1,a*, Chang Ha-png,b, and

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

Formulas for the Determinant

Formulas for the Determinant page 224 224 CHAPTER 3 Determnants e t te t e 2t 38 A = e t 2te t e 2t e t te t 2e 2t 39 If 123 A = 345, 456 compute the matrx product A adj(a) What can you conclude about det(a)? For Problems 40 43, use

More information

Multiple Sound Source Location in 3D Space with a Synchronized Neural System

Multiple Sound Source Location in 3D Space with a Synchronized Neural System Multple Sound Source Locaton n D Space wth a Synchronzed Neural System Yum Takzawa and Atsush Fukasawa Insttute of Statstcal Mathematcs Research Organzaton of Informaton and Systems 0- Mdor-cho, Tachkawa,

More information

Temperature. Chapter Heat Engine

Temperature. Chapter Heat Engine Chapter 3 Temperature In prevous chapters of these notes we ntroduced the Prncple of Maxmum ntropy as a technque for estmatng probablty dstrbutons consstent wth constrants. In Chapter 9 we dscussed the

More information

Modeling of Risk Treatment Measurement Model under Four Clusters Standards (ISO 9001, 14001, 27001, OHSAS 18001)

Modeling of Risk Treatment Measurement Model under Four Clusters Standards (ISO 9001, 14001, 27001, OHSAS 18001) Avalable onlne at www.scencedrect.com Proceda Engneerng 37 (202 ) 354 358 The Second SREE Conference on Engneerng Modelng and Smulaton Modelng of Rsk Treatment Measurement Model under Four Clusters Standards

More information

Research Article Green s Theorem for Sign Data

Research Article Green s Theorem for Sign Data Internatonal Scholarly Research Network ISRN Appled Mathematcs Volume 2012, Artcle ID 539359, 10 pages do:10.5402/2012/539359 Research Artcle Green s Theorem for Sgn Data Lous M. Houston The Unversty of

More information

Mathematical Preparations

Mathematical Preparations 1 Introducton Mathematcal Preparatons The theory of relatvty was developed to explan experments whch studed the propagaton of electromagnetc radaton n movng coordnate systems. Wthn expermental error the

More information

NP-Completeness : Proofs

NP-Completeness : Proofs NP-Completeness : Proofs Proof Methods A method to show a decson problem Π NP-complete s as follows. (1) Show Π NP. (2) Choose an NP-complete problem Π. (3) Show Π Π. A method to show an optmzaton problem

More information

4 Analysis of Variance (ANOVA) 5 ANOVA. 5.1 Introduction. 5.2 Fixed Effects ANOVA

4 Analysis of Variance (ANOVA) 5 ANOVA. 5.1 Introduction. 5.2 Fixed Effects ANOVA 4 Analyss of Varance (ANOVA) 5 ANOVA 51 Introducton ANOVA ANOVA s a way to estmate and test the means of multple populatons We wll start wth one-way ANOVA If the populatons ncluded n the study are selected

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

The Synchronous 8th-Order Differential Attack on 12 Rounds of the Block Cipher HyRAL

The Synchronous 8th-Order Differential Attack on 12 Rounds of the Block Cipher HyRAL The Synchronous 8th-Order Dfferental Attack on 12 Rounds of the Block Cpher HyRAL Yasutaka Igarash, Sej Fukushma, and Tomohro Hachno Kagoshma Unversty, Kagoshma, Japan Emal: {garash, fukushma, hachno}@eee.kagoshma-u.ac.jp

More information

Grover s Algorithm + Quantum Zeno Effect + Vaidman

Grover s Algorithm + Quantum Zeno Effect + Vaidman Grover s Algorthm + Quantum Zeno Effect + Vadman CS 294-2 Bomb 10/12/04 Fall 2004 Lecture 11 Grover s algorthm Recall that Grover s algorthm for searchng over a space of sze wors as follows: consder the

More information

A New Grey Relational Fusion Algorithm Based on Approximate Antropy

A New Grey Relational Fusion Algorithm Based on Approximate Antropy Journal of Computatonal Informaton Systems 9: 20 (2013) 8045 8052 Avalable at http://www.jofcs.com A New Grey Relatonal Fuson Algorthm Based on Approxmate Antropy Yun LIN, Jnfeng PANG, Ybng LI College

More information

CHAPTER 4. Vector Spaces

CHAPTER 4. Vector Spaces man 2007/2/16 page 234 CHAPTER 4 Vector Spaces To crtcze mathematcs for ts abstracton s to mss the pont entrel. Abstracton s what makes mathematcs work. Ian Stewart The man am of ths tet s to stud lnear

More information

Electronic Quantum Monte Carlo Calculations of Energies and Atomic Forces for Diatomic and Polyatomic Molecules

Electronic Quantum Monte Carlo Calculations of Energies and Atomic Forces for Diatomic and Polyatomic Molecules RESERVE HIS SPACE Electronc Quantum Monte Carlo Calculatons of Energes and Atomc Forces for Datomc and Polyatomc Molecules Myung Won Lee 1, Massmo Mella 2, and Andrew M. Rappe 1,* 1 he Maknen heoretcal

More information

Linear Feature Engineering 11

Linear Feature Engineering 11 Lnear Feature Engneerng 11 2 Least-Squares 2.1 Smple least-squares Consder the followng dataset. We have a bunch of nputs x and correspondng outputs y. The partcular values n ths dataset are x y 0.23 0.19

More information

CHAPTER 17 Amortized Analysis

CHAPTER 17 Amortized Analysis CHAPTER 7 Amortzed Analyss In an amortzed analyss, the tme requred to perform a sequence of data structure operatons s averaged over all the operatons performed. It can be used to show that the average

More information

GEO-SLOPE International Ltd, Calgary, Alberta, Canada Vibrating Beam

GEO-SLOPE International Ltd, Calgary, Alberta, Canada   Vibrating Beam GEO-SLOPE Internatonal Ltd, Calgary, Alberta, Canada www.geo-slope.com Introducton Vbratng Beam Ths example looks at the dynamc response of a cantlever beam n response to a cyclc force at the free end.

More information

Physics 2A Chapter 3 HW Solutions

Physics 2A Chapter 3 HW Solutions Phscs A Chapter 3 HW Solutons Chapter 3 Conceptual Queston: 4, 6, 8, Problems: 5,, 8, 7, 3, 44, 46, 69, 70, 73 Q3.4. Reason: (a) C = A+ B onl A and B are n the same drecton. Sze does not matter. (b) C

More information

Fast Simulation of Pyroshock Responses of a Conical Structure Using Rotation-Superposition Method

Fast Simulation of Pyroshock Responses of a Conical Structure Using Rotation-Superposition Method Appled Mathematcs & Informaton Scences An Internatonal Journal 211 NSP 5 (2) (211), 187S-193S Fast Smulaton of Pyroshock Responses of a Concal Structure Usng Rotaton-Superposton Method Yongjan Mao 1, Yulong

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

Simulated Power of the Discrete Cramér-von Mises Goodness-of-Fit Tests

Simulated Power of the Discrete Cramér-von Mises Goodness-of-Fit Tests Smulated of the Cramér-von Mses Goodness-of-Ft Tests Steele, M., Chaselng, J. and 3 Hurst, C. School of Mathematcal and Physcal Scences, James Cook Unversty, Australan School of Envronmental Studes, Grffth

More information