Buckling Analysis of Polar Orthotropic Circular and Annular Plates of Uniform and Linearly Varying Thickness with Different Edge Conditions

Size: px
Start display at page:

Download "Buckling Analysis of Polar Orthotropic Circular and Annular Plates of Uniform and Linearly Varying Thickness with Different Edge Conditions"

Transcription

1 Joural of Sold Mechacs Vol., No. (00 pp Bucklg Aalyss of Polar Orthotropc Crcular ad Aular Plates of Uform ad Learly Varyg Thckess wth Dfferet Edge Codtos F. Farhata,*, A. Golshah Mechacal Egeerg Faculty, Islamc Azad Uversty - Brach of Khomeshahr, Boulvard Mazare, Khomeshahr, Isfaha, Ira Ira Arcraft Maufacturg (HESA, Moallem Hghway, Isfaha, Ira Receved 8 May 00; accepted 0 July 00 ABSTRACT Ths paper vestgates symmetrcal bucklg of orthotropc crcular ad aular plates of cotuous varable thckess. Uform compresso loadg s appled at the plate outer boudary. Thckess vares learly alog radal drecto. Ier edge s free, whle outer edge has dfferet boudary codtos: clamped, smply ad elastcally restrat agast rotato. The optmzed Rtz method s appled for bucklg aalyss. I ths method, a polyomal fucto that s based o statc deformato of orthotropc crcular plates bedg s used. Also, by employg a expoetal parameter deformato fucto, egevalue s mmzed respect to ths parameter. The advatage of ths procedure s smplcty, comparso wth other methods, whle whole algorthm for soluto ca be coded for computer programmg. The effects of varato of radus, thckess, dfferet boudary codtos, rato of radal Youg modulus to crcumferetal oe, ad rato of outer radus to er oe aular plates o bucklg load factor are vestgated. The obtaed results show that plate wth detcal thckess, creasg of outer radus decreases the bucklg load factor. Moreover, crease of thckess of the plates results crease of bucklg load factor. 00 IAU, Arak Brach. All rghts reserved. Keywords: Bucklg; Orthotropc Plates; Crcular ad aular plates; Dfferet edge codtos INTRODUCTION O RTHOTROPIC crcular ad aular plates are always used by mechacal, cvl, aerospace ad structural egeers ad desgers. Some applcatos of these systems are pressure vessel valve, reforced crcular plates by radal ad crcumferece supporter, composte plates, cylder head cover, bulkhead plates submares, separated plates arcraft, optcal leses, ad acoustc trasducers rockets. Woosky [], for the frst tme, studed the problem of elastc stablty of orthotropc crcular plates. He troduced umerc results by usg Bessel fucto for bucklg of plates. Mek et al. [] studed o varato of thckess o bucklg of orthotropc rectagular plate. Laura et al. [3] foud crtcal load of bucklg for sotropc aular plate wth costat thckess by optmzed Raylegh-Rtz method. Imposed boudary codto of plate for ether er edge or outer edge was uder dfferet supports. Caco [4] studed o bucklg of crcular ad aular sotropc plate wth varable thckess that was used as a part of submare. Ths plate was cosdered wth free support o er edge ad clamped support ad resstat of rotato for outer edge. The thckess of plate s expoetal fucto of ts radus. He aalyzed the plate by optmzed Raylegh-Rtz method. Bremec et al. [5] also troduced oe optmzed rate of varato of thckess for bucklg of sotropc plates whch both er edge ad outer edge was uder costat * Correspodg author. E-mal address: farhata@aukhsh.ac.r (F. Farhata. 00 IAU, Arak Brach. All rghts reserved.

2 F. Farhata ad A. Golshah 57 The work doe by -plae radal force s gve as: radal loadd ad thckess was vared radal drecto. Bucklgg fucto was lear fasho ad solved by umerc method m uder smply ad clamped support. Guterrez et al. [6] cosdered bucklg ad vbrato of the sotropc plate p wth varable thckesss o elastc support usg Raylegh-Rtz method, ad obtaed acceptable results. Lag et al. [7] foud atural frequeces of oe orthotropc crcularr ad aular plate wth varable thckess usg u Raylegh-Rtz method that agreed wth the result of fte elemet method. I ths paper, bucklg of orthotropc crcular ad aular platess wth lear varato of thckess uder costat compressve radal loadg s studed. The boudary codto off aular plates are F-C plates (free er, ad clamped outer edge or clamped crcular sold oes, F-S plates (free er, smply outer edge or smply supported sold crcular oes, ad aular plates wth free er support ad resstat elastc agast rotato outer edge. Crcular plates cota plates wth clamped, smply ad elastc resstat agast rotato boudary codto. Solvg bucklg dfferetal d equato of orthotropc crcular or aular plate wth varable thckess s mpossble by aalytcal method m ad t should be solved usg umercal or eergy method. For ths reaso, optmzed Raylegh- of Rtz method s used. The results of ths method s more precsely tha Raylegh-Rtz method. For optmzato Raylegh-Rtz method, oe expoetal parameter approxmate fucto s cosdered. Egevalues (bucklg load factor that s obtaed, are mmzed accordg to ths expoetal parameter. Furthermore, the comparso betwee results of ths method ad the results of ANSYS commercal fte elemet package s doe. The effects of thckess varato, v boudary codtos, Youg module rato radus ad crcumferece axs, varato of rato of er radus to outer oe o bucklg load factor are cosdered. THEORY. Basc formulato f of the problem The formulato of the problem s derved uder the followg assumptos:. The plate s the state of plae stress.. The stress-stra relatoshp follows orthotropc materal. 3. The plate s th. Therefore, the Krchhoff assumptos are corporated. 4. The thckess s vared the drecto of radus of the plate. Cosder a crcular aular plate wth varable thckess h(r, a, b er ad outer radus, respectvely as show Fg.. For bucklg aalyss, the -plae dsplacemet u ad v may be eglected ad oly out-of-plae deformato w s cosdered. The goverg eergy fuctoal ca be gve by: J=U+VV ( where U ss the stored stra eergy per ut volume that the polar coordate system for plae stress s gve as follows [8]: U = òòò v ( r r + + r r r d r d dz ( V = òò A é æ wö N æ wö ù ê r ç + N çè r ç ø çè êë ø ú r d r d úû (3 Fg. Schematc vew of aular plate wth varable thckess (cetrally thcker crcular plate. 00 IAU, Arak Brach

3 58 Bucklg Aalyss of Polar Orthotropc Crcular ad Aular Plates I the preset study, the axal radal symmetry s assumed. Therefore, plate s depedet of azmuthal varable: a æ wö V Nr = ò ç r dr çè r (4 ø b For orthotropc aular plate, V s derved as follows [9] é ùæ ö ò (5 - ë û a + - N0 a - b w V = r - ú r dr + h b a a b ê ç r úçè r ø Also, usg the stress-stra relato for orthotropc materal, substtutg to Eq. (, oe may obta: é z æd wö æd wöædwö ædwö ù U = E r E d d d r ç E r r z òòò + ç + - ç v r dr ç dr çèdr ø çèrdr ê è ø è ø (6 ø ë ú û As show Fg the thckess of plate s cotuously varyg h(r, wth tegratg alog the thckess, the stored stra eergy ca be expressed by the followg equato: where b é ædwö ædwöædwö æ dwö ù U = Dr ( r ç r dr ò + + ç ç dr ç dr çèrdr ø çèrdr (7 è ø è ø ø a ê ë ú û 3 Eh r ( r E D( r Dr ( r =, = = ( - E D ( r r r r (8 I above equato, Dr ( r ad D ( r deote crcumferetal ad radal bedg stffess of the plate, respectvely. I ths study, aular ad sold crcular plates wth cotuously varyg thckess are cosdered. The varato of thckess alog the radus drecto ca be expressed as follows: æ r ö æ ö hr ( = h o + ç çèa ø çè ø (9 where h o ad a represet the thckess the cetre (er radus for aular plate ad the outer radus of plate, respectvely. I order to cosder the fluece of o uform thckess o bucklg load factor, two values are assged for the parameter, =0, for uform ad learly varyg thckess, respectvely. s o-dmesoal geometrc parameter that may be postve (cetrally ther crcular plate or egatve (cetrally thcker crcular plate ad s defed as follows: For crcular sold plates: ha = - (0 h o For crcular aular plates: hb- ho = ( h ( r o b 00 IAU, Arak Brach

4 F. Farhata ad A. Golshah 59 I above equato, r b s the rato of er radus to the outer oe (b/a. I the sake of coveece, the varables Eqs. (7 ad (5 are trasformed to dmesoless oe, so the total potetal eergy fuctoal s as follows: ì é ù a æd Wö æd Wöæ dw ö æ dw ö é r ùæ b dwö ü - JW ( = ïgr ( R RdR ï + D ò í ý ç 0 dr ç ç dr ç RdR çrdr r ê r b R úç dr ( ï êè ø è øè ø è ø ú - è ø ï b ïî ë û ë û ïþ that, Eh r gr = + R D = R= a 3 3 r o ( (, 0, ( - r (3 where λ s the bucklg load factor that s related to bucklg load as follows: N a 0 = (4 D 0. Optmzed Rtz method Cosderg the fact that Raylegh-Rtz method s a upper boud method, the determed egevalue s more tha real oe. Therefore, f oe ca optmze t somehow, the results wll be closer to real oe. I geeral, the fucto whch troduces the ukow quatty, s a lear combato of shape modes, as follows: N f ( x = å c ( x (5 = where c s the ukow costats. Accordg to the dea of optmzato, by performg the Optmzed Raylegh- Rtz method, t s qute coveet to approxmate f(x by meas of a summato: N f ( x = å c ( x, k (6 = Note that k above equato s the expoetal optmzato parameter. Regardg to the Eq. (6, out-plae dsplacemet W(R s gve as follows: N WR ( = å cw( Rk, (7 = By mmzg potetal eergy fuctoal Raylegh-Rtz method: J = 0, =,..., N c (8 Total umber of N lear homogeous algebrac equatos are geerated that the ukows are costats c. It forms the egevalue problem that the egevlaues are the values of bucklg load parameter. The o-trval codto leads to a trascedetal equato whose lowest root s the desred bucklg load factor [4]. Sce / k = 0, by requrg, oe s able to optmze the fudametal egevalue. 00 IAU, Arak Brach

5 60 Bucklg Aalyss of Polar Orthotropc Crcular ad Aular Plates.3 Bucklg of aular plate Regardg to the Eq. (7, w (R,k s defed as follows [9] w R a R br R k + - ( = ( + + (9 Ukow costats a ad b are determed by applyg boudary codtos..3. Clamped outer edge (F-C plate For a clamped outer edge, ra or R, the goverg boudary codtos are: ì w ( = 0 ï í dw ï ( = 0 ïî dr (0 By substtuto Eq. (9 to eq. (0, the a ad b values are determed as follows: -- k a =, b = + - k + -k (.3. Smply supported outer edge (S-F plate For a smply supported outer edge, the out-plae dsplacemet must satsfy the followg codtos: ì w ( = 0 ï í d w dw ï ( + ( 0 = ïî dr dr ( Cosderg the boudary codto outer edge, the a ad b values are determed: ( + ( a = ( k( k + + k( 3 k b = ( k( k + + (3.3.3 Elastcally restraed agast rotato For the case of elastcally restraed agast rotato: ì w ( = 0 ï í dw é d w dw ( gr ( ( ( dr dr ù =- + ê dr ú ïî ë û (4 where a ad b values are determed as follows: 00 IAU, Arak Brach

6 F. Farhata ad A. Golshah 6 Q -L S -Q a =-, b =- S -L S -L (5 I above equato, S, Q, ad L are defed as follows: [ ] [ ] [ ] S = ( k+ - + g( R (- + + k+ L = ( + + g( R ( Q = ( - + g( R (- + + (6 where = ak / D0 represets the dmesoless flexblty coeffcet. Usg the Eq. (8, total umber of N lear homogeous algebrac equatos s geerated. The o-trval codto leads to set zero the determat of coeffcets matrx, as follows: A- B = 0 (7 where A j ad B j are determed as follows: éæ d w öæd w ö d d d d j w w j dw w ù æ öæ ö æ öæ ö j ædw öæ w ö j Aj = g( R R dr r ò b dr dr dr R d R R d R R dr dr êçè ø èç ø çè øçè ø ç è øçè øú ç è øçè dr ë û ø (8 é d r ù æ b dw ö æ w ö - j Bj = R - R dr + -r ê rb b R ú ç dr ç è dr ø ë û (9 I the above equato, for the case of smply supported ad clamped outer edge, =0 ad =, respectvely..4 Bucklg of crcular sold plate Regardg to Eq. (7, for crcular sold plate w (R s defed as follows [9] w R a R br R k + ( - ( = ( + + (30 I order to obta a ad b as costats, the followg boudary codtos must be satsfed:.4. Clamped outer edge, (C-F plate k -- b =, a = + - k + -k (3.4. Smply supported outer edge, (S-F plate ( + ( a = ( k( k + + k( 5 4 k b = ( k( k + + (3 00 IAU, Arak Brach

7 6 Bucklg Aalyss of Polar Orthotropc Crcular ad Aular Plates.4.3 Elastcally restraed agast rotato Q -L S -Q a =-, b =- S -L S -L where S = ( k+ - é g( R K( 3 k ù êë úû L = (+ - é g( R K( ù êë úû Q = ( - é + g( R K( ù êë úû (33 (34 where A j ad B j are determed as follows: éæ d w öæd w ö d d d d ( j w w j dw w ù æ öæ ö æ öæ ö j æd w( öæ w ö j Aj = g( R R dr 0 ò dr dr dr RdR RdR RdR RdR êçè øè ç ø çè øçè ø ç è øçè øú ç è øçè RdR ë û ø (35 æ d dw ö æ w ö - j Bj = R ò R dr 0 ç èdr ç øè ç dr ø (36 I the above equato, lke before, for the case of smply supported 0 ad clamped outer edge. 3 NUMERICAL RESULTS Ths secto presets a umber of umercal examples that shows the good performace of the proposed method, whch was mplemeted Mathematca 5. computer program. The results of the developed optmzed Rtz method are compared wth some other results whch were obtaed from FE method that are developed ANSYS 0 commercal package. All calculato has bee performed for E r 0000 Mpa, υ ө 0.3, a= m, h o 0.08 m. It was revealed that coverget bucklg load factor s obtaed wth 4-term seres. Table ( shows ths covergece for cetrally thcker aular orthotropc plate. I presetg results, the dmesoless bucklg load factor s used. Value of ths factor s obtaed for plates of uform ad learly cotuously thckess. 3. Aular plate Table depcts the fluece of parameters,, r b o the bucklg load factor. It s observed that wth creasg the amout of β, bucklg load factor s creased too. Oe observes that orthotropc plate ( > has more stffess agast bucklg occaso comparso to sotropc oe. Furthermore, creasg parameter toward postve values makes the bucklg load factor to crease. Regardg to Table, some values of r b (r b > decreases the bucklg load factor λ, meawhle some other values makes t decrease. As t was expected, show Table 3, clamped boudary codto represets the hghest value of factor whle the smply supported oe shows the lowest. The fluece of parameters,, r b s the same as clamped case. Tables 4-6 depct the fluece of rotatoal costat o bucklg load factor for dfferet value of. It s revealed that whe 0, the boudary codto s closer to smply supported case ad the loadg factor shows lower tha whe the outer edge s clamped ad stff agast rotato. Table Covergece study for aular orthotropc plate r b m IAU, Arak Brach

8 F. Farhata ad A. Golshah 63 Table Bucklg load factor varato wth smply supported outer edge r b Table 3 Bucklg load factor varato wth clamped outer edge r b IAU, Arak Brach

9 64 Bucklg Aalyss of Polar Orthotropc Crcular ad Aular Plates Table 4 Bucklg load factor varato wth edge elastcally restraed (= r b Table 5 Load factor varato wth edge elastcally restraed ( = r b Crcular sold plate Fgs. ad 3 llustrate the varato of buckg load factor wth respect to boudary codto case, orthotropc ad geometry parameters ad. As show, plate wth <0 (cetrally thcker sold plate, h a /h o < has lower bucklg load factor tha plate wth >0 (cetrally ther crcular plate, h a /h o >. Bucklg factor patter for all boudary codtos are smlar. 00 IAU, Arak Brach

10 F. Farhata ad A. Golshah 65 Table 6 Load factor varato wth edge elastcally restraed ( = r b Fg. Varato of bucklg load factor wth respect to orthotropc parameter ad o-dmesoal geometrc parameter wth clamped outer edge. Fg. 3 Varato of bucklg load factor wth respect to orthotropc parameter ad o-dmesoal geometrc parameter wth smply supported outer edge. 00 IAU, Arak Brach

11 66 Bucklg Aalyss of Polar Orthotropc Crcular ad Aular Plates Fg. 4 Varato of bucklg load factor wth respect to orthotropcc parameter for dfferet boudary codtos.. Table 7 Comparso of results for bucklg load factor Optmzed Rtz method (I ad ANSYS (II I II I 9.87 II I.56 II Fg 4 llustrates the fluece of rotatoal costat o bucklg load factor for dfferet values of. For dfferet boudary codtos, the obtaed result s the same as the aular plate. I fact, for smply supported outer edge, the evaluated bucklg load factor s lower tha clamped ad elastcally restraed agast rotato outer edge. As show Table 7, the results obtaed from preset method compare very well wth obtaed from ANSYS commercal package. Ths cofrms the accuracy of Optmzed Rtz method bucklg aalyzg of crcular plates. 4 CONCLUSIONS The bucklg aalyss of orthotropc crcular aular ad sold plates uder uform radal compresso loadg wth uform ad learly varyg thckess was preseted. The er edge s free whle the outer edge s uder dfferet types of classcal boudary codtos ad also wth edges elastcally restraed agast rotato. Ths s mplemeted by optmzed Rtz method. I ths method, a optmzato expoetal parameter s utlzed that bucklg load factor was mmzed wth respect to t. Followg aree some of the cocludg remarks: I. Icreasg orthotropc parameter ad radus rato (er to outer radus,, creases the resstace of plate agast bucklg pheomea. II. Plate wth clamped boudary codto exhbts the hgher value of the bucklg parameter, whle the smply supported case shows lowest. Also, plate wth edges elastcallyy restraed agast rotato has value of betwee two boudary codto cases. III. Cetrally ther crcular plate has hgher bucklg parameter tha cetrally thcker oe. REFERENCES [] Woowsk-Kreg ger S., 958, Bucklg stablty of crcular plates wth crcular cyldrcal Aeolotropy, Igeeur- Archv 6: IAU, Arak Brach

12 F. Farhata ad A. Golshah 67 [] Mek T., Huybrechts S., Galey J., 999, The effect of varyg thckess o the bucklg of orthotropc plate, Joural of Composte Materals 33: [3] Laura P.A.A, Guterrez R.H., Saz H.C., Elvra G., 000, Bucklg of crcular, sold ad aular plates wth a termedate crcular support, Ocea Egeerg 7: [4] Caco P.M., Reyes J.A., 003, Bucklg of crcular aular plates of cotuously varable thckess used as teral bulkheads submersbles, Ocea egeerg 30: [5] Bremec B., Kosel F., 006, Thckess optmzato of crcular aular plates at bucklg, Th-Walled Structures 3: [6] Guterrez R.H., Romall E., Laura P.A.A., 996, Vbrato ad elastc stablty of th crcular plates wth varable profle, Joural of Soud ad Vbrato 95: [7] Lag B., Zhag Sh., Che D., 007, Natural frequeces of crcular aular plates wth varable thckess by a ew method, Joural of Pressure Vessels ad Ppg 84: [8] Tmosheko S.P., Gere J.M., 96, Theory of Elastc Stablty, Secod Edto, McGraw-Hll, New York. [9] Gupta U.S., Lal R., Verma C.P., 986, Bucklg ad vbratos of polar orthotropc aular plates of varable thckess, Joural of Soud ad Vbrato 04: IAU, Arak Brach

Chapter 2 - Free Vibration of Multi-Degree-of-Freedom Systems - II

Chapter 2 - Free Vibration of Multi-Degree-of-Freedom Systems - II CEE49b Chapter - Free Vbrato of Mult-Degree-of-Freedom Systems - II We ca obta a approxmate soluto to the fudametal atural frequecy through a approxmate formula developed usg eergy prcples by Lord Raylegh

More information

Functions of Random Variables

Functions of Random Variables Fuctos of Radom Varables Chapter Fve Fuctos of Radom Varables 5. Itroducto A geeral egeerg aalyss model s show Fg. 5.. The model output (respose) cotas the performaces of a system or product, such as weght,

More information

Dynamic Analysis of Axially Beam on Visco - Elastic Foundation with Elastic Supports under Moving Load

Dynamic Analysis of Axially Beam on Visco - Elastic Foundation with Elastic Supports under Moving Load Dyamc Aalyss of Axally Beam o Vsco - Elastc Foudato wth Elastc Supports uder Movg oad Saeed Mohammadzadeh, Seyed Al Mosayeb * Abstract: For dyamc aalyses of ralway track structures, the algorthm of soluto

More information

Lecture 07: Poles and Zeros

Lecture 07: Poles and Zeros Lecture 07: Poles ad Zeros Defto of poles ad zeros The trasfer fucto provdes a bass for determg mportat system respose characterstcs wthout solvg the complete dfferetal equato. As defed, the trasfer fucto

More information

Derivation of 3-Point Block Method Formula for Solving First Order Stiff Ordinary Differential Equations

Derivation of 3-Point Block Method Formula for Solving First Order Stiff Ordinary Differential Equations Dervato of -Pot Block Method Formula for Solvg Frst Order Stff Ordary Dfferetal Equatos Kharul Hamd Kharul Auar, Kharl Iskadar Othma, Zara Bb Ibrahm Abstract Dervato of pot block method formula wth costat

More information

Cubic Nonpolynomial Spline Approach to the Solution of a Second Order Two-Point Boundary Value Problem

Cubic Nonpolynomial Spline Approach to the Solution of a Second Order Two-Point Boundary Value Problem Joural of Amerca Scece ;6( Cubc Nopolyomal Sple Approach to the Soluto of a Secod Order Two-Pot Boudary Value Problem W.K. Zahra, F.A. Abd El-Salam, A.A. El-Sabbagh ad Z.A. ZAk * Departmet of Egeerg athematcs

More information

The solution of Euler-Bernoulli beams using variational derivative method

The solution of Euler-Bernoulli beams using variational derivative method Scetfc Research ad Essays Vol. 5(9), pp. 9-4, 4 May Avalable ole at http://www.academcjourals.org/sre ISSN 99-48 Academc Jourals Full egth Research Paper The soluto of Euler-Beroull beams usg varatoal

More information

C-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory

C-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory ROAD MAP... AE301 Aerodyamcs I UNIT C: 2-D Arfols C-1: Aerodyamcs of Arfols 1 C-2: Aerodyamcs of Arfols 2 C-3: Pael Methods C-4: Th Arfol Theory AE301 Aerodyamcs I Ut C-3: Lst of Subects Problem Solutos?

More information

ANALYTICAL SOLUTION FOR NONLINEAR BENDING OF FG PLATES BY A LAYERWISE THEORY

ANALYTICAL SOLUTION FOR NONLINEAR BENDING OF FG PLATES BY A LAYERWISE THEORY 6 TH ITERATIOAL COFERECE O COMPOSITE MATERIALS AALYTICAL SOLUTIO FOR OLIEAR BEDIG OF FG PLATES BY A LAYERWISE THEORY M. Taha*, S.M. Mrababaee** *Departmet of Mechacal Egeerg, Ferdows Uversty of Mashhad,

More information

Stress Wave propagation in Electro-Magneto-Elastic plate of arbitrary cross-sections

Stress Wave propagation in Electro-Magneto-Elastic plate of arbitrary cross-sections Iteratoal Joural of Scetfc & Egeerg Research Volume 3, Issue 8, August-1 1 ISSN 9-5518 Stress Wave propagato Electro-Mageto-Elastc plate of arbtrary cross-sectos P. Pousamy Departmet of Mathematcs Govermet

More information

Comparison of Analytical and Numerical Results in Modal Analysis of Multispan Continuous Beams with LS-DYNA

Comparison of Analytical and Numerical Results in Modal Analysis of Multispan Continuous Beams with LS-DYNA th Iteratoal S-N Users oferece Smulato Techology omparso of alytcal ad Numercal Results Modal alyss of Multspa otuous eams wth S-N bht Mahapatra ad vk hatteree etral Mechacal Egeerg Research Isttute, urgapur

More information

FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM

FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Joural of Appled Matematcs ad Computatoal Mecacs 04, 3(4), 7-34 FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Ata Cekot, Stasław Kukla Isttute of Matematcs, Czestocowa Uversty of Tecology Częstocowa,

More information

d dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin

d dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin Learzato of the Swg Equato We wll cover sectos.5.-.6 ad begg of Secto 3.3 these otes. 1. Sgle mache-fte bus case Cosder a sgle mache coected to a fte bus, as show Fg. 1 below. E y1 V=1./_ Fg. 1 The admttace

More information

A NEW FINITE ELEMENT CONSIDERING SHEAR LAG

A NEW FINITE ELEMENT CONSIDERING SHEAR LAG Bullet of the raslvaa Uversty of Braşov CIBv 204 Vol. 7 (56) Specal Issue No. - 204 A NEW FINIE EEMEN CONSIDERING SHEAR AG A. PROIC M. VOJNIC PURCAR D. UIC Abstract: A ew model of descrbg the shear lag

More information

MOLECULAR VIBRATIONS

MOLECULAR VIBRATIONS MOLECULAR VIBRATIONS Here we wsh to vestgate molecular vbratos ad draw a smlarty betwee the theory of molecular vbratos ad Hückel theory. 1. Smple Harmoc Oscllator Recall that the eergy of a oe-dmesoal

More information

Ahmed Elgamal. MDOF Systems & Modal Analysis

Ahmed Elgamal. MDOF Systems & Modal Analysis DOF Systems & odal Aalyss odal Aalyss (hese otes cover sectos from Ch. 0, Dyamcs of Structures, Al Chopra, Pretce Hall, 995). Refereces Dyamcs of Structures, Al K. Chopra, Pretce Hall, New Jersey, ISBN

More information

2C09 Design for seismic and climate changes

2C09 Design for seismic and climate changes 2C09 Desg for sesmc ad clmate chages Lecture 08: Sesmc aalyss of elastc MDOF systems Aurel Strata, Poltehca Uversty of Tmsoara 06/04/2017 Europea Erasmus Mudus Master Course Sustaable Costructos uder atural

More information

Chapter 9 Jordan Block Matrices

Chapter 9 Jordan Block Matrices Chapter 9 Jorda Block atrces I ths chapter we wll solve the followg problem. Gve a lear operator T fd a bass R of F such that the matrx R (T) s as smple as possble. f course smple s a matter of taste.

More information

Engineering Vibration 1. Introduction

Engineering Vibration 1. Introduction Egeerg Vbrato. Itroducto he study of the moto of physcal systems resultg from the appled forces s referred to as dyamcs. Oe type of dyamcs of physcal systems s vbrato, whch the system oscllates about certa

More information

BERNSTEIN COLLOCATION METHOD FOR SOLVING NONLINEAR DIFFERENTIAL EQUATIONS. Aysegul Akyuz Dascioglu and Nese Isler

BERNSTEIN COLLOCATION METHOD FOR SOLVING NONLINEAR DIFFERENTIAL EQUATIONS. Aysegul Akyuz Dascioglu and Nese Isler Mathematcal ad Computatoal Applcatos, Vol. 8, No. 3, pp. 293-300, 203 BERNSTEIN COLLOCATION METHOD FOR SOLVING NONLINEAR DIFFERENTIAL EQUATIONS Aysegul Ayuz Dascoglu ad Nese Isler Departmet of Mathematcs,

More information

Estimation of Stress- Strength Reliability model using finite mixture of exponential distributions

Estimation of Stress- Strength Reliability model using finite mixture of exponential distributions Iteratoal Joural of Computatoal Egeerg Research Vol, 0 Issue, Estmato of Stress- Stregth Relablty model usg fte mxture of expoetal dstrbutos K.Sadhya, T.S.Umamaheswar Departmet of Mathematcs, Lal Bhadur

More information

On the construction of symmetric nonnegative matrix with prescribed Ritz values

On the construction of symmetric nonnegative matrix with prescribed Ritz values Joural of Lear ad Topologcal Algebra Vol. 3, No., 14, 61-66 O the costructo of symmetrc oegatve matrx wth prescrbed Rtz values A. M. Nazar a, E. Afshar b a Departmet of Mathematcs, Arak Uversty, P.O. Box

More information

L5 Polynomial / Spline Curves

L5 Polynomial / Spline Curves L5 Polyomal / Sple Curves Cotets Coc sectos Polyomal Curves Hermte Curves Bezer Curves B-Sples No-Uform Ratoal B-Sples (NURBS) Mapulato ad Represetato of Curves Types of Curve Equatos Implct: Descrbe a

More information

ANALYSIS ON THE NATURE OF THE BASIC EQUATIONS IN SYNERGETIC INTER-REPRESENTATION NETWORK

ANALYSIS ON THE NATURE OF THE BASIC EQUATIONS IN SYNERGETIC INTER-REPRESENTATION NETWORK Far East Joural of Appled Mathematcs Volume, Number, 2008, Pages Ths paper s avalable ole at http://www.pphm.com 2008 Pushpa Publshg House ANALYSIS ON THE NATURE OF THE ASI EQUATIONS IN SYNERGETI INTER-REPRESENTATION

More information

Arithmetic Mean and Geometric Mean

Arithmetic Mean and Geometric Mean Acta Mathematca Ntresa Vol, No, p 43 48 ISSN 453-6083 Arthmetc Mea ad Geometrc Mea Mare Varga a * Peter Mchalča b a Departmet of Mathematcs, Faculty of Natural Sceces, Costate the Phlosopher Uversty Ntra,

More information

Analysis of von Kármán plates using a BEM formulation

Analysis of von Kármán plates using a BEM formulation Boudary Elemets ad Other Mesh Reducto Methods XXIX 213 Aalyss of vo Kármá plates usg a BEM formulato L. Wademam & W. S. Vetur São Carlos School of Egeerg, Uversty of São Paulo, Brazl Abstract Ths work

More information

Long blade vibration model for turbine-generator shafts torsional vibration analysis

Long blade vibration model for turbine-generator shafts torsional vibration analysis Avalable ole www.ocpr.co Joural of Checal ad Pharaceutcal Research, 05, 7(3):39-333 Research Artcle ISSN : 0975-7384 CODEN(USA) : JCPRC5 Log blade vbrato odel for turbe-geerator shafts torsoal vbrato aalyss

More information

Modeling and analysis of waves in a heat conducting thermo-elastic plate of elliptical shape

Modeling and analysis of waves in a heat conducting thermo-elastic plate of elliptical shape 589 Modelg ad aalyss of waves a heat coductg thermo-elastc plate of ellptcal shape Abstract Wave propagato heat coductg thermo elastc plate of ellptcal cross-secto s studed usg the Fourer expaso collocato

More information

A Remark on the Uniform Convergence of Some Sequences of Functions

A Remark on the Uniform Convergence of Some Sequences of Functions Advaces Pure Mathematcs 05 5 57-533 Publshed Ole July 05 ScRes. http://www.scrp.org/joural/apm http://dx.do.org/0.436/apm.05.59048 A Remark o the Uform Covergece of Some Sequeces of Fuctos Guy Degla Isttut

More information

Numerical Analysis Formulae Booklet

Numerical Analysis Formulae Booklet Numercal Aalyss Formulae Booklet. Iteratve Scemes for Systems of Lear Algebrac Equatos:.... Taylor Seres... 3. Fte Dfferece Approxmatos... 3 4. Egevalues ad Egevectors of Matrces.... 3 5. Vector ad Matrx

More information

Solution of General Dual Fuzzy Linear Systems. Using ABS Algorithm

Solution of General Dual Fuzzy Linear Systems. Using ABS Algorithm Appled Mathematcal Sceces, Vol 6, 0, o 4, 63-7 Soluto of Geeral Dual Fuzzy Lear Systems Usg ABS Algorthm M A Farborz Aragh * ad M M ossezadeh Departmet of Mathematcs, Islamc Azad Uversty Cetral ehra Brach,

More information

CH E 374 Computational Methods in Engineering Fall 2007

CH E 374 Computational Methods in Engineering Fall 2007 CH E 7 Computatoal Methods Egeerg Fall 007 Sample Soluto 5. The data o the varato of the rato of stagato pressure to statc pressure (r ) wth Mach umber ( M ) for the flow through a duct are as follows:

More information

Lecture 7. Confidence Intervals and Hypothesis Tests in the Simple CLR Model

Lecture 7. Confidence Intervals and Hypothesis Tests in the Simple CLR Model Lecture 7. Cofdece Itervals ad Hypothess Tests the Smple CLR Model I lecture 6 we troduced the Classcal Lear Regresso (CLR) model that s the radom expermet of whch the data Y,,, K, are the outcomes. The

More information

Beam Warming Second-Order Upwind Method

Beam Warming Second-Order Upwind Method Beam Warmg Secod-Order Upwd Method Petr Valeta Jauary 6, 015 Ths documet s a part of the assessmet work for the subject 1DRP Dfferetal Equatos o Computer lectured o FNSPE CTU Prague. Abstract Ths documet

More information

Analysis of Lagrange Interpolation Formula

Analysis of Lagrange Interpolation Formula P IJISET - Iteratoal Joural of Iovatve Scece, Egeerg & Techology, Vol. Issue, December 4. www.jset.com ISS 348 7968 Aalyss of Lagrage Iterpolato Formula Vjay Dahya PDepartmet of MathematcsMaharaja Surajmal

More information

1 Lyapunov Stability Theory

1 Lyapunov Stability Theory Lyapuov Stablty heory I ths secto we cosder proofs of stablty of equlbra of autoomous systems. hs s stadard theory for olear systems, ad oe of the most mportat tools the aalyss of olear systems. It may

More information

Solving Constrained Flow-Shop Scheduling. Problems with Three Machines

Solving Constrained Flow-Shop Scheduling. Problems with Three Machines It J Cotemp Math Sceces, Vol 5, 2010, o 19, 921-929 Solvg Costraed Flow-Shop Schedulg Problems wth Three Maches P Pada ad P Rajedra Departmet of Mathematcs, School of Advaced Sceces, VIT Uversty, Vellore-632

More information

ONE GENERALIZED INEQUALITY FOR CONVEX FUNCTIONS ON THE TRIANGLE

ONE GENERALIZED INEQUALITY FOR CONVEX FUNCTIONS ON THE TRIANGLE Joural of Pure ad Appled Mathematcs: Advaces ad Applcatos Volume 4 Number 205 Pages 77-87 Avalable at http://scetfcadvaces.co. DOI: http://.do.org/0.8642/jpamaa_7002534 ONE GENERALIZED INEQUALITY FOR CONVEX

More information

Lecture Note to Rice Chapter 8

Lecture Note to Rice Chapter 8 ECON 430 HG revsed Nov 06 Lecture Note to Rce Chapter 8 Radom matrces Let Y, =,,, m, =,,, be radom varables (r.v. s). The matrx Y Y Y Y Y Y Y Y Y Y = m m m s called a radom matrx ( wth a ot m-dmesoal dstrbuto,

More information

MATH 247/Winter Notes on the adjoint and on normal operators.

MATH 247/Winter Notes on the adjoint and on normal operators. MATH 47/Wter 00 Notes o the adjot ad o ormal operators I these otes, V s a fte dmesoal er product space over, wth gve er * product uv, T, S, T, are lear operators o V U, W are subspaces of V Whe we say

More information

Lecture 12 APPROXIMATION OF FIRST ORDER DERIVATIVES

Lecture 12 APPROXIMATION OF FIRST ORDER DERIVATIVES FDM: Appromato of Frst Order Dervatves Lecture APPROXIMATION OF FIRST ORDER DERIVATIVES. INTRODUCTION Covectve term coservato equatos volve frst order dervatves. The smplest possble approach for dscretzato

More information

EPM RT HYBRID FINITE ELEMENT METHOD APPLIED TO THE ANALYSIS OF FREE VIBRATION OF SPHERICAL SHELL

EPM RT HYBRID FINITE ELEMENT METHOD APPLIED TO THE ANALYSIS OF FREE VIBRATION OF SPHERICAL SHELL EPM T 03-0 HYBID FINITE ELEMENT METHOD APPLIED TO THE ANALYSIS OF FEE VIBATION OF SPHEICAL SHELL M. Meaa, A.A. Laks Départemet de Gée mécaque École Polytechque de Motréal Avrl 03 EPM-T-03-0 HYBID FINITE

More information

The Mathematical Appendix

The Mathematical Appendix The Mathematcal Appedx Defto A: If ( Λ, Ω, where ( λ λ λ whch the probablty dstrbutos,,..., Defto A. uppose that ( Λ,,..., s a expermet type, the σ-algebra o λ λ λ are defed s deoted by ( (,,...,, σ Ω.

More information

ON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS

ON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS ON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS Şl uv dr g Ja-Crsta GRIGORE, Uverstatea d Pteşt, strtîrgu dvale Nr Prof uv dr g Ncolae PANDREA, Uverstatea d Pteşt, strtîrgu dvale Nr Cof

More information

LINEAR REGRESSION ANALYSIS

LINEAR REGRESSION ANALYSIS LINEAR REGRESSION ANALYSIS MODULE V Lecture - Correctg Model Iadequaces Through Trasformato ad Weghtg Dr. Shalabh Departmet of Mathematcs ad Statstcs Ida Isttute of Techology Kapur Aalytcal methods for

More information

Ordinary Least Squares Regression. Simple Regression. Algebra and Assumptions.

Ordinary Least Squares Regression. Simple Regression. Algebra and Assumptions. Ordary Least Squares egresso. Smple egresso. Algebra ad Assumptos. I ths part of the course we are gog to study a techque for aalysg the lear relatoshp betwee two varables Y ad X. We have pars of observatos

More information

h-analogue of Fibonacci Numbers

h-analogue of Fibonacci Numbers h-aalogue of Fboacc Numbers arxv:090.0038v [math-ph 30 Sep 009 H.B. Beaoum Prce Mohammad Uversty, Al-Khobar 395, Saud Araba Abstract I ths paper, we troduce the h-aalogue of Fboacc umbers for o-commutatve

More information

The internal structure of natural numbers, one method for the definition of large prime numbers, and a factorization test

The internal structure of natural numbers, one method for the definition of large prime numbers, and a factorization test Fal verso The teral structure of atural umbers oe method for the defto of large prme umbers ad a factorzato test Emmaul Maousos APM Isttute for the Advacemet of Physcs ad Mathematcs 3 Poulou str. 53 Athes

More information

Mu Sequences/Series Solutions National Convention 2014

Mu Sequences/Series Solutions National Convention 2014 Mu Sequeces/Seres Solutos Natoal Coveto 04 C 6 E A 6C A 6 B B 7 A D 7 D C 7 A B 8 A B 8 A C 8 E 4 B 9 B 4 E 9 B 4 C 9 E C 0 A A 0 D B 0 C C Usg basc propertes of arthmetc sequeces, we fd a ad bm m We eed

More information

A Method for Damping Estimation Based On Least Square Fit

A Method for Damping Estimation Based On Least Square Fit Amerca Joural of Egeerg Research (AJER) 5 Amerca Joural of Egeerg Research (AJER) e-issn: 3-847 p-issn : 3-936 Volume-4, Issue-7, pp-5-9 www.ajer.org Research Paper Ope Access A Method for Dampg Estmato

More information

Introduction to local (nonparametric) density estimation. methods

Introduction to local (nonparametric) density estimation. methods Itroducto to local (oparametrc) desty estmato methods A slecture by Yu Lu for ECE 66 Sprg 014 1. Itroducto Ths slecture troduces two local desty estmato methods whch are Parze desty estmato ad k-earest

More information

u 1 Figure 1 3D Solid Finite Elements

u 1 Figure 1 3D Solid Finite Elements Sold Elemets he Fte Elemet Lbrary of the MIDAS Famly Programs cludes the follog Sold Elemets: - ode tetrahedro, -ode petahedro, ad -ode hexahedro sho Fg.. he fte elemet formulato of all elemet types s

More information

EVALUATION OF FUNCTIONAL INTEGRALS BY MEANS OF A SERIES AND THE METHOD OF BOREL TRANSFORM

EVALUATION OF FUNCTIONAL INTEGRALS BY MEANS OF A SERIES AND THE METHOD OF BOREL TRANSFORM EVALUATION OF FUNCTIONAL INTEGRALS BY MEANS OF A SERIES AND THE METHOD OF BOREL TRANSFORM Jose Javer Garca Moreta Ph. D research studet at the UPV/EHU (Uversty of Basque coutry) Departmet of Theoretcal

More information

Econometric Methods. Review of Estimation

Econometric Methods. Review of Estimation Ecoometrc Methods Revew of Estmato Estmatg the populato mea Radom samplg Pot ad terval estmators Lear estmators Ubased estmators Lear Ubased Estmators (LUEs) Effcecy (mmum varace) ad Best Lear Ubased Estmators

More information

Analysis of Variance with Weibull Data

Analysis of Variance with Weibull Data Aalyss of Varace wth Webull Data Lahaa Watthaacheewaul Abstract I statstcal data aalyss by aalyss of varace, the usual basc assumptos are that the model s addtve ad the errors are radomly, depedetly, ad

More information

best estimate (mean) for X uncertainty or error in the measurement (systematic, random or statistical) best

best estimate (mean) for X uncertainty or error in the measurement (systematic, random or statistical) best Error Aalyss Preamble Wheever a measuremet s made, the result followg from that measuremet s always subject to ucertaty The ucertaty ca be reduced by makg several measuremets of the same quatty or by mprovg

More information

Chapter 5 Properties of a Random Sample

Chapter 5 Properties of a Random Sample Lecture 6 o BST 63: Statstcal Theory I Ku Zhag, /0/008 Revew for the prevous lecture Cocepts: t-dstrbuto, F-dstrbuto Theorems: Dstrbutos of sample mea ad sample varace, relatoshp betwee sample mea ad sample

More information

UNIT 2 SOLUTION OF ALGEBRAIC AND TRANSCENDENTAL EQUATIONS

UNIT 2 SOLUTION OF ALGEBRAIC AND TRANSCENDENTAL EQUATIONS Numercal Computg -I UNIT SOLUTION OF ALGEBRAIC AND TRANSCENDENTAL EQUATIONS Structure Page Nos..0 Itroducto 6. Objectves 7. Ital Approxmato to a Root 7. Bsecto Method 8.. Error Aalyss 9.4 Regula Fals Method

More information

THE NEW OPTIMALITY CRITERIA FOR STRUCTURAL DESIGN WITH CONSTRAINING ELASTIC DISPLACEMENTS (NON-COMPOSITE FORWARD SWEPT WING WITHOUT DIVERGENCE)

THE NEW OPTIMALITY CRITERIA FOR STRUCTURAL DESIGN WITH CONSTRAINING ELASTIC DISPLACEMENTS (NON-COMPOSITE FORWARD SWEPT WING WITHOUT DIVERGENCE) 8 TH INTRNATIONAL CONGRSS OF TH ARONAUTICAL SCINCS TH NW OPTIMALITY CRITRIA FOR STRUCTURAL DSIGN WITH CONSTRAINING LASTIC DISPLACMNTS (NON-COMPOSIT FORWARD SWPT WING WITHOUT DIVRGNC) Alexader I Dal, Samara

More information

Fractional Order Finite Difference Scheme For Soil Moisture Diffusion Equation And Its Applications

Fractional Order Finite Difference Scheme For Soil Moisture Diffusion Equation And Its Applications IOS Joural of Mathematcs (IOS-JM e-iss: 78-578. Volume 5, Issue 4 (Ja. - Feb. 3, PP -8 www.osrourals.org Fractoal Order Fte Dfferece Scheme For Sol Mosture Dffuso quato Ad Its Applcatos S.M.Jogdad, K.C.Takale,

More information

A NEW NUMERICAL APPROACH FOR SOLVING HIGH-ORDER LINEAR AND NON-LINEAR DIFFERANTIAL EQUATIONS

A NEW NUMERICAL APPROACH FOR SOLVING HIGH-ORDER LINEAR AND NON-LINEAR DIFFERANTIAL EQUATIONS Secer, A., et al.: A New Numerıcal Approach for Solvıg Hıgh-Order Lıear ad No-Lıear... HERMAL SCIENCE: Year 8, Vol., Suppl., pp. S67-S77 S67 A NEW NUMERICAL APPROACH FOR SOLVING HIGH-ORDER LINEAR AND NON-LINEAR

More information

ESS Line Fitting

ESS Line Fitting ESS 5 014 17. Le Fttg A very commo problem data aalyss s lookg for relatoshpetwee dfferet parameters ad fttg les or surfaces to data. The smplest example s fttg a straght le ad we wll dscuss that here

More information

DATE: 21 September, 1999 TO: Jim Russell FROM: Peter Tkacik RE: Analysis of wide ply tube winding as compared to Konva Kore CC: Larry McMillan

DATE: 21 September, 1999 TO: Jim Russell FROM: Peter Tkacik RE: Analysis of wide ply tube winding as compared to Konva Kore CC: Larry McMillan M E M O R A N D U M DATE: 1 September, 1999 TO: Jm Russell FROM: Peter Tkack RE: Aalyss of wde ply tube wdg as compared to Kova Kore CC: Larry McMlla The goal of ths report s to aalyze the spral tube wdg

More information

x y exp λ'. x exp λ 2. x exp 1.

x y exp λ'. x exp λ 2. x exp 1. egecosmcd Egevalue-egevector of the secod dervatve operator d /d hs leads to Fourer seres (se, cose, Legedre, Bessel, Chebyshev, etc hs s a eample of a systematc way of geeratg a set of mutually orthogoal

More information

UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS

UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS Postpoed exam: ECON430 Statstcs Date of exam: Jauary 0, 0 Tme for exam: 09:00 a.m. :00 oo The problem set covers 5 pages Resources allowed: All wrtte ad prted

More information

7.0 Equality Contraints: Lagrange Multipliers

7.0 Equality Contraints: Lagrange Multipliers Systes Optzato 7.0 Equalty Cotrats: Lagrage Multplers Cosder the zato of a o-lear fucto subject to equalty costrats: g f() R ( ) 0 ( ) (7.) where the g ( ) are possbly also olear fuctos, ad < otherwse

More information

Lecture 3 Probability review (cont d)

Lecture 3 Probability review (cont d) STATS 00: Itroducto to Statstcal Iferece Autum 06 Lecture 3 Probablty revew (cot d) 3. Jot dstrbutos If radom varables X,..., X k are depedet, the ther dstrbuto may be specfed by specfyg the dvdual dstrbuto

More information

Assignment 5/MATH 247/Winter Due: Friday, February 19 in class (!) (answers will be posted right after class)

Assignment 5/MATH 247/Winter Due: Friday, February 19 in class (!) (answers will be posted right after class) Assgmet 5/MATH 7/Wter 00 Due: Frday, February 9 class (!) (aswers wll be posted rght after class) As usual, there are peces of text, before the questos [], [], themselves. Recall: For the quadratc form

More information

Research Article An Improved Fourier Series Method for the Free Vibration Analysis of the Three-Dimensional Coupled Beams

Research Article An Improved Fourier Series Method for the Free Vibration Analysis of the Three-Dimensional Coupled Beams Hdaw Publshg Corporato Shock ad Vbrato Volume 6, Artcle ID 97844, 8 pages http://dx.do.org/.55/6/97844 Research Artcle A Improved Fourer Seres Method for the Free Vbrato Aalyss of the Three-Dmesoal Coupled

More information

Numerical Solution of Linear Second Order Ordinary Differential Equations with Mixed Boundary Conditions by Galerkin Method

Numerical Solution of Linear Second Order Ordinary Differential Equations with Mixed Boundary Conditions by Galerkin Method Mathematcs ad Computer Scece 7; (5: 66-78 http://www.scecepublshggroup.com//mcs do:.648/.mcs.75. Numercal Soluto of Lear Secod Order Ordary Dfferetal Equatos wth Mxed Boudary Codtos by Galer Method Aalu

More information

{ }{ ( )} (, ) = ( ) ( ) ( ) Chapter 14 Exercises in Sampling Theory. Exercise 1 (Simple random sampling): Solution:

{ }{ ( )} (, ) = ( ) ( ) ( ) Chapter 14 Exercises in Sampling Theory. Exercise 1 (Simple random sampling): Solution: Chapter 4 Exercses Samplg Theory Exercse (Smple radom samplg: Let there be two correlated radom varables X ad A sample of sze s draw from a populato by smple radom samplg wthout replacemet The observed

More information

Fourth Order Four-Stage Diagonally Implicit Runge-Kutta Method for Linear Ordinary Differential Equations ABSTRACT INTRODUCTION

Fourth Order Four-Stage Diagonally Implicit Runge-Kutta Method for Linear Ordinary Differential Equations ABSTRACT INTRODUCTION Malasa Joural of Mathematcal Sceces (): 95-05 (00) Fourth Order Four-Stage Dagoall Implct Ruge-Kutta Method for Lear Ordar Dfferetal Equatos Nur Izzat Che Jawas, Fudzah Ismal, Mohamed Sulema, 3 Azm Jaafar

More information

Carbonyl Groups. University of Chemical Technology, Beijing , PR China;

Carbonyl Groups. University of Chemical Technology, Beijing , PR China; Electroc Supplemetary Materal (ESI) for Physcal Chemstry Chemcal Physcs Ths joural s The Ower Socetes 0 Supportg Iformato A Theoretcal Study of Structure-Solublty Correlatos of Carbo Doxde Polymers Cotag

More information

NP!= P. By Liu Ran. Table of Contents. The P versus NP problem is a major unsolved problem in computer

NP!= P. By Liu Ran. Table of Contents. The P versus NP problem is a major unsolved problem in computer NP!= P By Lu Ra Table of Cotets. Itroduce 2. Prelmary theorem 3. Proof 4. Expla 5. Cocluso. Itroduce The P versus NP problem s a major usolved problem computer scece. Iformally, t asks whether a computer

More information

DIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS

DIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS DIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS Course Project: Classcal Mechacs (PHY 40) Suja Dabholkar (Y430) Sul Yeshwath (Y444). Itroducto Hamltoa mechacs s geometry phase space. It deals

More information

A New Family of Transformations for Lifetime Data

A New Family of Transformations for Lifetime Data Proceedgs of the World Cogress o Egeerg 4 Vol I, WCE 4, July - 4, 4, Lodo, U.K. A New Famly of Trasformatos for Lfetme Data Lakhaa Watthaacheewakul Abstract A famly of trasformatos s the oe of several

More information

COMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL

COMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL Sebasta Starz COMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL Abstract The am of the work s to preset a method of rakg a fte set of dscrete radom varables. The proposed method s based o two approaches:

More information

ECE 595, Section 10 Numerical Simulations Lecture 19: FEM for Electronic Transport. Prof. Peter Bermel February 22, 2013

ECE 595, Section 10 Numerical Simulations Lecture 19: FEM for Electronic Transport. Prof. Peter Bermel February 22, 2013 ECE 595, Secto 0 Numercal Smulatos Lecture 9: FEM for Electroc Trasport Prof. Peter Bermel February, 03 Outle Recap from Wedesday Physcs-based devce modelg Electroc trasport theory FEM electroc trasport

More information

Research Article A New Derivation and Recursive Algorithm Based on Wronskian Matrix for Vandermonde Inverse Matrix

Research Article A New Derivation and Recursive Algorithm Based on Wronskian Matrix for Vandermonde Inverse Matrix Mathematcal Problems Egeerg Volume 05 Artcle ID 94757 7 pages http://ddoorg/055/05/94757 Research Artcle A New Dervato ad Recursve Algorthm Based o Wroska Matr for Vadermode Iverse Matr Qu Zhou Xja Zhag

More information

ENGI 4421 Joint Probability Distributions Page Joint Probability Distributions [Navidi sections 2.5 and 2.6; Devore sections

ENGI 4421 Joint Probability Distributions Page Joint Probability Distributions [Navidi sections 2.5 and 2.6; Devore sections ENGI 441 Jot Probablty Dstrbutos Page 7-01 Jot Probablty Dstrbutos [Navd sectos.5 ad.6; Devore sectos 5.1-5.] The jot probablty mass fucto of two dscrete radom quattes, s, P ad p x y x y The margal probablty

More information

5 Short Proofs of Simplified Stirling s Approximation

5 Short Proofs of Simplified Stirling s Approximation 5 Short Proofs of Smplfed Strlg s Approxmato Ofr Gorodetsky, drtymaths.wordpress.com Jue, 20 0 Itroducto Strlg s approxmato s the followg (somewhat surprsg) approxmato of the factoral,, usg elemetary fuctos:

More information

A Robust Total Least Mean Square Algorithm For Nonlinear Adaptive Filter

A Robust Total Least Mean Square Algorithm For Nonlinear Adaptive Filter A Robust otal east Mea Square Algorthm For Nolear Adaptve Flter Ruxua We School of Electroc ad Iformato Egeerg X'a Jaotog Uversty X'a 70049, P.R. Cha rxwe@chare.com Chogzhao Ha, azhe u School of Electroc

More information

Chapter 4 Multiple Random Variables

Chapter 4 Multiple Random Variables Revew for the prevous lecture: Theorems ad Examples: How to obta the pmf (pdf) of U = g (, Y) ad V = g (, Y) Chapter 4 Multple Radom Varables Chapter 44 Herarchcal Models ad Mxture Dstrbutos Examples:

More information

F. Inequalities. HKAL Pure Mathematics. 進佳數學團隊 Dr. Herbert Lam 林康榮博士. [Solution] Example Basic properties

F. Inequalities. HKAL Pure Mathematics. 進佳數學團隊 Dr. Herbert Lam 林康榮博士. [Solution] Example Basic properties 進佳數學團隊 Dr. Herbert Lam 林康榮博士 HKAL Pure Mathematcs F. Ieualtes. Basc propertes Theorem Let a, b, c be real umbers. () If a b ad b c, the a c. () If a b ad c 0, the ac bc, but f a b ad c 0, the ac bc. Theorem

More information

Chapter 8. Inferences about More Than Two Population Central Values

Chapter 8. Inferences about More Than Two Population Central Values Chapter 8. Ifereces about More Tha Two Populato Cetral Values Case tudy: Effect of Tmg of the Treatmet of Port-We tas wth Lasers ) To vestgate whether treatmet at a youg age would yeld better results tha

More information

Applying the condition for equilibrium to this equilibrium, we get (1) n i i =, r G and 5 i

Applying the condition for equilibrium to this equilibrium, we get (1) n i i =, r G and 5 i CHEMICAL EQUILIBRIA The Thermodyamc Equlbrum Costat Cosder a reversble reacto of the type 1 A 1 + 2 A 2 + W m A m + m+1 A m+1 + Assgg postve values to the stochometrc coeffcets o the rght had sde ad egatve

More information

A Conventional Approach for the Solution of the Fifth Order Boundary Value Problems Using Sixth Degree Spline Functions

A Conventional Approach for the Solution of the Fifth Order Boundary Value Problems Using Sixth Degree Spline Functions Appled Matheatcs, 1, 4, 8-88 http://d.do.org/1.4/a.1.448 Publshed Ole Aprl 1 (http://www.scrp.org/joural/a) A Covetoal Approach for the Soluto of the Ffth Order Boudary Value Probles Usg Sth Degree Sple

More information

Block-Based Compact Thermal Modeling of Semiconductor Integrated Circuits

Block-Based Compact Thermal Modeling of Semiconductor Integrated Circuits Block-Based Compact hermal Modelg of Semcoductor Itegrated Crcuts Master s hess Defese Caddate: Jg Ba Commttee Members: Dr. Mg-Cheg Cheg Dr. Daqg Hou Dr. Robert Schllg July 27, 2009 Outle Itroducto Backgroud

More information

PGE 310: Formulation and Solution in Geosystems Engineering. Dr. Balhoff. Interpolation

PGE 310: Formulation and Solution in Geosystems Engineering. Dr. Balhoff. Interpolation PGE 30: Formulato ad Soluto Geosystems Egeerg Dr. Balhoff Iterpolato Numercal Methods wth MATLAB, Recktewald, Chapter 0 ad Numercal Methods for Egeers, Chapra ad Caale, 5 th Ed., Part Fve, Chapter 8 ad

More information

NP!= P. By Liu Ran. Table of Contents. The P vs. NP problem is a major unsolved problem in computer

NP!= P. By Liu Ran. Table of Contents. The P vs. NP problem is a major unsolved problem in computer NP!= P By Lu Ra Table of Cotets. Itroduce 2. Strategy 3. Prelmary theorem 4. Proof 5. Expla 6. Cocluso. Itroduce The P vs. NP problem s a major usolved problem computer scece. Iformally, t asks whether

More information

8.1 Hashing Algorithms

8.1 Hashing Algorithms CS787: Advaced Algorthms Scrbe: Mayak Maheshwar, Chrs Hrchs Lecturer: Shuch Chawla Topc: Hashg ad NP-Completeess Date: September 21 2007 Prevously we looked at applcatos of radomzed algorthms, ad bega

More information

Non-degenerate Perturbation Theory

Non-degenerate Perturbation Theory No-degeerate Perturbato Theory Proble : H E ca't solve exactly. But wth H H H' H" L H E Uperturbed egevalue proble. Ca solve exactly. E Therefore, kow ad. H ' H" called perturbatos Copyrght Mchael D. Fayer,

More information

Reflection of Plane Waves from a Free Surface of an Initially Stressed Transversely Isotropic Dissipative Medium

Reflection of Plane Waves from a Free Surface of an Initially Stressed Transversely Isotropic Dissipative Medium ppled Mathematcs 0 9- do:0.6/am.0.956 Publshed Ole September 0 (http://www.scrp.org/joural/am) Reflecto of Plae Waves from a Free Surface of a Itally Stressed Trasversely Isotropc Dsspatve Medum bstract

More information

The conformations of linear polymers

The conformations of linear polymers The coformatos of lear polymers Marc R. Roussel Departmet of Chemstry ad Bochemstry Uversty of Lethbrdge February 19, 9 Polymer scece s a rch source of problems appled statstcs ad statstcal mechacs. I

More information

1 0, x? x x. 1 Root finding. 1.1 Introduction. Solve[x^2-1 0,x] {{x -1},{x 1}} Plot[x^2-1,{x,-2,2}] 3

1 0, x? x x. 1 Root finding. 1.1 Introduction. Solve[x^2-1 0,x] {{x -1},{x 1}} Plot[x^2-1,{x,-2,2}] 3 Adrew Powuk - http://www.powuk.com- Math 49 (Numercal Aalyss) Root fdg. Itroducto f ( ),?,? Solve[^-,] {{-},{}} Plot[^-,{,-,}] Cubc equato https://e.wkpeda.org/wk/cubc_fucto Quartc equato https://e.wkpeda.org/wk/quartc_fucto

More information

Periodic Table of Elements. EE105 - Spring 2007 Microelectronic Devices and Circuits. The Diamond Structure. Electronic Properties of Silicon

Periodic Table of Elements. EE105 - Spring 2007 Microelectronic Devices and Circuits. The Diamond Structure. Electronic Properties of Silicon EE105 - Srg 007 Mcroelectroc Devces ad Crcuts Perodc Table of Elemets Lecture Semcoductor Bascs Electroc Proertes of Slco Slco s Grou IV (atomc umber 14) Atom electroc structure: 1s s 6 3s 3 Crystal electroc

More information

X ε ) = 0, or equivalently, lim

X ε ) = 0, or equivalently, lim Revew for the prevous lecture Cocepts: order statstcs Theorems: Dstrbutos of order statstcs Examples: How to get the dstrbuto of order statstcs Chapter 5 Propertes of a Radom Sample Secto 55 Covergece

More information

( q Modal Analysis. Eigenvectors = Mode Shapes? Eigenproblem (cont) = x x 2 u 2. u 1. x 1 (4.55) vector and M and K are matrices.

( q Modal Analysis. Eigenvectors = Mode Shapes? Eigenproblem (cont) = x x 2 u 2. u 1. x 1 (4.55) vector and M and K are matrices. 4.3 - Modal Aalyss Physcal coordates are ot always the easest to work Egevectors provde a coveet trasformato to modal coordates Modal coordates are lear combato of physcal coordates Say we have physcal

More information

Q-analogue of a Linear Transformation Preserving Log-concavity

Q-analogue of a Linear Transformation Preserving Log-concavity Iteratoal Joural of Algebra, Vol. 1, 2007, o. 2, 87-94 Q-aalogue of a Lear Trasformato Preservg Log-cocavty Daozhog Luo Departmet of Mathematcs, Huaqao Uversty Quazhou, Fua 362021, P. R. Cha ldzblue@163.com

More information

Simulation Output Analysis

Simulation Output Analysis Smulato Output Aalyss Summary Examples Parameter Estmato Sample Mea ad Varace Pot ad Iterval Estmato ermatg ad o-ermatg Smulato Mea Square Errors Example: Sgle Server Queueg System x(t) S 4 S 4 S 3 S 5

More information