Analysis of Dynamics of Boundary Shape Perturbation of a Rotating Elastoplastic Radially Inhomogeneous Plane Circular Disk: Analytical Approach
|
|
- Coleen Johns
- 6 years ago
- Views:
Transcription
1 Alid Mtmtics tt://dxdoiorg/436/m3568 Pulisd Onlin My (tt://wwwscirporg/journl/m) Anlysis of Dynmics of Boundry S Prturtion of Rotting Elstolstic Rdilly Inomognous Pln Circulr Disk: Anlyticl Aroc Dmytro М Lil А А Mrtynyuk Crksy Ntionl Bodn Kmlnytsky Univrsity Crksy Ukrin Stility of Procsss Drtmnt S P Timosnko Institut of Mcnics Ntionl Acdmy of Scincs of Ukrin Kyiv Ukrin Emil: dim_l@ukrnt Rcivd Mrc 5 ; rvisd Mrc 6 ; cctd Aril 3 ABSTRACT For rotting inomognous circulr disk wy of clculting dynmics of oundry s rturtion nd filur of ring ccity is roosd in trms of smll rmtr mtod Crctristic qution of lstic zon criticl rdius is otind s first roximtion A formul of criticl ngulr vlocity is drivd wic dtrmins t stility loss of t disc ccording to t slf-lncd form Efficincy of t roosd mtod is sown y n illustrtiv xml considrd in Sction 7 Vlus of criticl ngulr vlocity of rottion r found numriclly for diffrnt rmtrs of t disc Kywords: Axisymmtric Elstolstic Prolm; Mtod of Boundry S Prturtion; Rotting Inomognous Circulr Disc; Stility Loss; Filur of Bring Ccity; Criticl Angulr Vlocity Introduction T filur of ring ccity of quickly rotting lstic disc [-3] ovrlodd y cntrifugl dilting forcs is ssocitd wit t dynmics of its oundry s rturtion [4] Aftr t disc tks u nw lncd s du to considrl growt of lstic zons [5] t instility [6] dvlos tontilly noug wit t incrs of rottion vlocity [7] Tis is stiultd y t rsons of t intrnl oints to t disc contour rsing nd outrunning growt of vril rdius of t rturd lstolstic oundry s comrd wit t vrition of its cunt rdius for stl disc [89] To study t stility loss nd vlocity dynmics of rotting disc t rturtion mtod cn lid [-] In t nlysis of ln strss strin stt tis mtod ws mloyd to otin roximt criticl vlus of t lstic zon dimnsions nd ngulr vlocity of continuous omognous circulr discs [34] ring-sd discs [5] including tos lodd long t contour y dditionl rdil forcs [6] std discs nd som rity rofil discs [7] s wll s simlst inomognous discs Tis rovs fficincy of t nlyticl mtod of oundry s rturtion (wit t us of simlst numricl rocdurs t crtin stg) wic rducs ssntilly t mount of clcultions nd t t sm tim fcilitts fruitful liction of vrious numricl tcniqus [8-] for stility nd strngt clcultion of turin nd otr mssiv discs Mnwil tr is still n on rolm of stlising y t smll rmtr mtod t rltionsi twn t vlu of oundry s rturtion lstic zon rdius nd rottion vlocity of unstl con- tinuous inomognous circulr disc cosonding to t indictd stt of rturd lstolstic oundry Tis is t sujct of our rsnt invstigtion Sttmnt of t Prolm W considr disc D consisting of two omognous nd isotroic ln discs D nd D Continuous circulr disc D osssss rdius wic coincids wit t intrnl rdius of t ring-sd circulr disc D T xtrnl rdius of disc D quls to Discs D nd D md from diffrnt mtrils r rigidly connctd into on disc D long t circumfrnc r W dsignt y s t mtril yild limit of disc D E is t lsticity modulus is t dnsity nd is t Poisson cofficint T cosonding mtril rmtrs of disc D r dsigntd y s E nd rsctivly It is ssumd tt constnt ngulr rottion vlocity of disc D is igr tn its criticl vlocity Tis mns t rsnc of rturtion of t initil contour circumfrnc r rturtion of t cunt Coyrigt SciRs
2 45 D М LILA А А MARTYNYUK rdius of lstolstic oundry r r nd in gnrl rturtion of strss strin stt of t wol (unstl) disc W focus our ttntion on t slf-lncd form of t stility loss of disc D wic is littl diffrnt from t circulr form T disc oundry qution u to t first ordr infinitsiml is rsntd in t form r = dcosn d const n or = cosn () wr = r is dimnsionlss cunt rdius is smll rmtr n is olr ngl On tis sis lt us dtrmin criticl vlus r = r nd = wic ccomny rcing of t ov mntiond circumfrnc r = y t rturd lstolstic oundry in t lstic zon of disc D T criticl vlus cosonding to rcing of t disc dg y t lstolstic oundry i its contct wit curv () sould scilly clcultd W rcll tt for solution of ts rolms it is ncssry first of ll to nlyticlly stlis t condition of contct of t lstolstic oundry nd circumfrnc of givn rdius i to construct crctristic qution wit t rmtr wit rsct to r ving solvd first t systm of linr qutions d u =for r = dr d u r =for r = d =for r = r r =for r = r d u =fo = r dr wit rsct to ur nd rity constnts found in t xrssions for strss nd dislcmnt comonnts r nd u dtrmining rturd strss strin stt of t rotting disc D T ov mntiond linrizd rturtions of t first ordr of smllnss stisfy diffrntil lnc qutions of ln rolm nd rtil diffrntil qutions of rltionsi twn strsss nd dislcmnts [] Unrturd strss stt (dsigntd y t ur indx ) is dtrmind y ordinry diffrntil qutions of qusisttic quilirium nd constrint qutions in t lstic zon or y t yild Sint-Vnnt condition [5] in t lstic zon In viw of t instility dvlomnt mcnism of t inomognous disc undr considrtion t sttd rolm will solvd for c of t four css: () DD (Figur ()); (s) DD (Figur ()); () DD (Figur (c)); (c) DD (Figur (d)) 3 Solution in t Cs DD In ordr to us oundry nd conjugtion conditions Au =for = () du A =for = (3) d =for = (4) =for = (5) Au 3 =for = (6) for rturtions of t first ordr of smllnss nd of rdil contct nd tngntil strsss rltd to t yild limit s w rcll tt in D (Figur ()) nd in D II = I cos n III IV = c ( ) c ( ) I II c ( ) c ( ) sin n III IV = I II III IV = I II III IV = ci c II ciii civ nd sids = q q q 3 q 4 = q q q q cos n cos n sin n Hr = r = nd r indfinit cofficints nd q q 8 r t cofficints xrssd vi n nd = E E ; I IV I IV ci civ r known functions [6] Morovr Coyrigt SciRs
3 D М LILA А А MARTYNYUK 453 r r () () r r r (c) (d) Figur Prturd lstolstic oundry rcing givn circumfrnc r = A = C 6 3 x A = A 4 x (7) A3 = 8 3 x C = s m 3 x x = 4q = s k m 3 l 3 k k s = s s = q = Coyrigt SciRs s k = k 3 3 m = wr l= For = rturtion of t first ordr of smllnss of t rdil dislcmnt rltd to is known from () u = cos n Trfor du d = n sin n
4 454 D М LILA А А MARTYNYUK Conditions ()-(6) in t xtndd form [6] r wr A = na = q q q q = 3 4 q q q q = w w w w cos n 3 4 Au 3 = IV IV w = II q q5 w = q q 6 I II IV w3 = II q3 q7 w4 = III II q4 IV q 8 = Hnc u = Ucosn wr U= w ww 3 w4 A 3 nd sids = A = na = q q q q q q qq qq = q q q q q q q q q q As consqunc t crctristic qution wit rsct to t lstic zon rdius cosonding to t momnt of contct of t rturd lstolstic oundry nd t mntiond circumfrnc = = coms U = (8) T criticl vlu of ngulr vlocity cosonding to t criticl vlu of rdius of t lstic domin = ( is criticl rdius of t lstic zon D for wic t disc loss its stility) is otind in trms of (7) 4 Solution in t Cs DD Now in contrst to Sction 3 t lstic domin is omognous nd snts zon D (Figur ()) trfor [45] = cos n n n n na nb n C n D n = n n na nb n n C n n D c n os n n n n = na nb nc nd sin n wr A B C nd D r indfinit cofficints Coltions (7) r writtn s wr of A =C6 3 x A = A 4 x A = C 6 3 x 3 3 x C = s x= = r (9) Trfor t systm of qutions for dtrmintion u ( ) s t form na nb n C n D A = A BC D A = n An Bn Cn D= n n n n A B C D n n n n = n An B n C n D cosn Au n n n n 3 Hnc wr U = u = U cosn = na nb n C n D A nd morovr n n n n 3 n A= A n n A n n n n n N n B= A n n n A n n n n N n C = A n ( n) n An ( n) ( n) N n D= A n n n An n n N Coyrigt SciRs
5 D М LILA А А MARTYNYUK 455 N = n n n n Tus crctristic Eqution (8) is constructd T crctristic qution wit rmtr wit rsct to criticl rdius of t lstic domin wic rcd t xtrnl dg of t disc D rds [9] wr U = () x= k5 k k k 3 = r U for 6 Solution in t Cs DD 5 Solution in t Cs DD Hving comrd strss stts (unrturd nd rof t disc D in css (s) nd () (Figur (c)) turd) of instility dvlomnt w conclud out t ncs- 4 ving sity to rsrv r ll clcultions of Sction x = 4q cngd t xrssion for x = In ordr to follow t rturtion dynmics of lstolstic oundry twn D nd D (Figur (d)) w will tk into ccount (s Sction 4) t fct tt x C = = r s k 3 k k 3 3 k 3 wr c c cc c = 4 3 c = 3 s k k c = 3 k k k c3 =3 3 3 s s k Similrly to Sction 5 t rst of clcultions including gnrl form of crctristic Equtions (8) nd () coincid wit t rsults rsntd in Sction 4 7 Exmls nd Concluding Rmrks For inomognous disc wit t rmtrs n = =9 =93 =3 =3 = =99 s =99 nd = s E wic loss its stility ccording to cs () for =748 nd q =685 t vlus of criticl rdius of lstic zon D nd rltiv criticl rottion vlocity q r rsntd in Tl Tl rsnts crctristic criticl vlus otind in trms of solution of crctristic Eqution () for t disc wit rmtrs n = = =4 =3 = = s =8 nd E = s wic loss its stility ccording to cs (s) for = = = 767 nd q =6674 T sm rolm is solvd for t disc wit n = =5 =3 = = s = nd = s E wos instility dvlos ccording to () (Tl 3) for =8 =76 nd q = 73 nd ccording to (c) (T l 4) for = =889 = 7 nd q = 76 Tl Vlus of criticl rdius nd rltiv criticl vloc- ity dnding on δ δ q Tl Vlus of criticl rdius nd rltiv criticl vlocity dnding on δ δ q Tl 3 Vlus of criticl rdius nd rltiv criticl vlocity dnding on δ δ q Coyrigt SciRs
6 456 D М LILA А А MARTYNYUK Tl 4 Vlus of criticl rdius nd rltiv criticl vlocity dnding on δ δ q T rltionsis stlisd twn t vlu of oundry s rturtion loction nd ty of r- of turd lstolstic oundry nd rottion vlocity unstl continuous circulr disc llow qulittiv nd quntittiv conclusions to md out culiritis of t disc sur-ig-s d dynmics T liction of t otind rsults nls us to forcst t dvlomnt of unstl stt nd to clcult ossil loss of stility nd filur of ring ccity of rotting discs It sould notd tt sic qutions of stility tory of stil dforml odis drivd y linriztion of nonlinr qutions contin trms scifid vi t comonnts of unrturd ground stt Tis cuss som difficultis in t rolm on loss of stility sinc loding rmtr ssocitd wit t criticl fforts ntrs t sic qutions Aliction of t roximtd roc rsntd in t r for stility invstigtion of stil lstic odis simlifis t rolm cus ot t rturtions ij stisfy t initil lnc qutions nd t loding rmtr is introducd into oundry conditions on t rturd initil surfc of t ody T loding rmtr is dtrmind y ssntilly mor siml crctristic qutions REFERENCES [] K B Bitsno nd R Grmml Tcnicl Dynmics Vol Gosudrstvnno Izdtlstvo Tkniko-Torticskoy Litrtury Moscow nd Lningrd 95 [] A E H Lov A Trtis on t Mtmticl Tory of Elsticity Dovr Pulictions Nw York 97 [3] S P Timosnko nd J N Goodir Tory of Elsticity McGrw-Hill Nw York 934 [4] А N Guz nd Yu N Nmis Mtod of Boundry Form Prturtion in t Mcnics of Continu Vysc Skol Kiv 989 [5] V V Sokolovsky Plsticity Tory Vyssy Skol Moscow 969 [6] A N Guz nd I Yu Bic Tr-Dimnsionl Stility Tory of Dforml Bodis Nukov Dumk Kiv 985 [7] A Ndi Plsticity nd Frctur of Solid Bodis Vol Izdtlstvo Inostrnnoy Litrtury Moscow 954 [8] D D Ivlv Continuum Mcnics Vol Pismtlit Moscow [9] D D Ivlv On t Loss of Bring Ccity of Rotting Discs Clos to Circulr Ons Izvstiy Akdmii Nuk SSSR Otdlni Tknicskik Nuk No [] D V Gorgivskii Smll Prturtions of n Undformd Stt in Mdi wit Yild Strss Dokldy Pysics Vol 48 No doi:34/63545 [] D D Ivlv nd L V Yrsov Prturtion Mtod in t Tory of Elstolstic Body Nuk Moscow 978 [] L V Yrsov nd D D Ivlv On t Stility Loss of Rotting Discs Izvstiy Akdmii Nuk SSSR Otdlni Tknicskik Nuk No [3] D M Lil Eccntric Form of Stility Loss of Rotting Elstolstic Disc Rorts of t Ntionl Acdmy of Scincs of Ukrin No [4] D M Lil nd А А Mrtynyuk Aout t Stility Loss of Rotting Elstolstic Circulr Disc Rorts of t Ntionl Acdmy of Scincs of Ukrin No 44-5 [5] D M Lil nd А A Mrtynyuk Dvlomnt of Instility in Rotting Elstolstic Annulr Disk Intrntionl Alid Mcnics Vol 48 No 4-33 [6] D M Lil On t Instility of Rotting Elstolstic Std Annulr Disc Lodd ovr t Boundry in t Middl Pln Intrntionl Alid Mcnics (to ulisd) [7] D M Lil nd А A Mrtynyuk Stility Loss of Rotting Elstolstic Discs of t Scific Form Alid Mtmtics Vol No doi:436/m577 [8] I V Dminusko nd I A Birgr Strss Clcultion of Rotting Discs Msinostroyniy Moscow 978 [9] M Mzièr J Bsson S Forst B Tnguy H Clons nd F Vogl Ovrsd Burst of Elstoviscolstic Rotting Disks Prt I: Anlyticl nd Numricl Stility Anlyss Euron Journl of Mcnics A/Solids Vol 8 No doi:6/juromcsol878 [] M Mzièr J Bsson S Forst B Tnguy H Clons nd F Vogl Ovrsd Burst of Elstoviscolstic Rotting Disks: Prt II Burst of Surlloy Turin Disk Euron Journl of Mcnics A/Solids Vol 8 No doi:6/juromcsol8 Coyrigt SciRs
22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 8: Effect of a Vertical Field on Tokamak Equilibrium
.65, MHD Thory of usion Systms Prof. ridrg Lctur 8: Effct of Vrticl ild on Tokmk Equilirium Toroidl orc lnc y Mns of Vrticl ild. Lt us riw why th rticl fild is imortnt. 3. or ry short tims, th cuum chmr
More informationThe Angular Momenta Dipole Moments and Gyromagnetic Ratios of the Electron and the Proton
Journl of Modrn hysics, 014, 5, 154-157 ublishd Onlin August 014 in SciRs. htt://www.scir.org/journl/jm htt://dx.doi.org/.436/jm.014.51415 Th Angulr Momnt Diol Momnts nd Gyromgntic Rtios of th Elctron
More informationProblem 1. Solution: = show that for a constant number of particles: c and V. a) Using the definitions of P
rol. Using t dfinitions of nd nd t first lw of trodynis nd t driv t gnrl rltion: wr nd r t sifi t itis t onstnt rssur nd volu rstivly nd nd r t intrnl nrgy nd volu of ol. first lw rlts d dq d t onstnt
More informationELASTOPLASTIC ANALYSIS OF PLATE WITH BOUNDARY ELEMENT METHOD
Intrntionl Journl of chnicl nginring nd Tchnology (IJT) olum 9, Issu 6, Jun 18,. 864 87, Articl ID: IJT_9_6_97 Avilbl onlin t htt://.im.com/ijmt/issus.s?jty=ijt&ty=9&ity=6 IN Print: 976-64 nd IN Onlin:
More informationCIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7
CIVL / -D Boundr Vlu Prolms - Rctngulr Elmnts / RECANGULAR ELEMENS - In som pplictions, it m mor dsirl to us n lmntl rprsnttion of th domin tht hs four sids, ithr rctngulr or qudriltrl in shp. Considr
More informationElliptical motion, gravity, etc
FW Physics 130 G:\130 lctur\ch 13 Elliticl motion.docx g 1 of 7 11/3/010; 6:40 PM; Lst rintd 11/3/010 6:40:00 PM Fig. 1 Elliticl motion, grvity, tc minor xis mjor xis F 1 =A F =B C - D, mjor nd minor xs
More informationChapter 11 Calculation of
Chtr 11 Clcultion of th Flow Fild OUTLINE 11-1 Nd for Scil Procdur 11-2 Som Rltd Difficultis 11-3 A Rmdy : Th stggrd Grid 11-4 Th Momntum Equtions 11-5 Th Prssur nd Vlocity Corrctions 11-6 Th Prssur-Corrction
More informationThe Theory of Small Reflections
Jim Stils Th Univ. of Knss Dt. of EECS 4//9 Th Thory of Smll Rflctions /9 Th Thory of Smll Rflctions Rcll tht w nlyzd qurtr-wv trnsformr usg th multil rflction viw ot. V ( z) = + β ( z + ) V ( z) = = R
More informationFunctions and Graphs 1. (a) (b) (c) (f) (e) (d) 2. (a) (b) (c) (d)
Functions nd Grps. () () (c) - - - O - - - O - - - O - - - - (d) () (f) - - O - 7 6 - - O - -7-6 - - - - - O. () () (c) (d) - - - O - O - O - - O - -. () G() f() + f( ), G(-) f( ) + f(), G() G( ) nd G()
More informationCh 1.2: Solutions of Some Differential Equations
Ch 1.2: Solutions of Som Diffrntil Equtions Rcll th fr fll nd owl/mic diffrntil qutions: v 9.8.2v, p.5 p 45 Ths qutions hv th gnrl form y' = y - b W cn us mthods of clculus to solv diffrntil qutions of
More informationLecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:
Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS
VSRT MEMO #05 MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS 01886 Fbrury 3, 009 Tlphon: 781-981-507 Fx: 781-981-0590 To: VSRT Group From: Aln E.E. Rogrs Subjct: Simplifid
More informationChapter 16. 1) is a particular point on the graph of the function. 1. y, where x y 1
Prctic qustions W now tht th prmtr p is dirctl rltd to th mplitud; thrfor, w cn find tht p. cos d [ sin ] sin sin Not: Evn though ou might not now how to find th prmtr in prt, it is lws dvisl to procd
More informationJournal of System Design and Dynamics
Journl of Systm Dsign nd Dynmics Vol. 1, No. 3, 7 A Numricl Clcultion Modl of Multi Wound Foil Bring with th Effct of Foil Locl Dformtion * Ki FENG** nd Shighiko KANEKO** ** Dprtmnt of Mchnics Enginring,
More information, between the vertical lines x a and x b. Given a demand curve, having price as a function of quantity, p f (x) at height k is the curve f ( x,
Clculus for Businss nd Socil Scincs - Prof D Yun Finl Em Rviw vrsion 5/9/7 Chck wbsit for ny postd typos nd updts Pls rport ny typos This rviw sht contins summris of nw topics only (This rviw sht dos hv
More informationLagrangian Analysis of a Class of Quadratic Liénard-Type Oscillator Equations with Exponential-Type Restoring Force function
agrangian Analysis of a Class of Quadratic iénard-ty Oscillator Equations wit Eonntial-Ty Rstoring Forc function J. Akand, D. K. K. Adjaï,.. Koudaoun,Y. J. F. Komaou,. D. onsia. Dartmnt of Pysics, Univrsity
More informationMiscellaneous open problems in the Regular Boundary Collocation approach
Miscllnous opn problms in th Rgulr Boundry Colloction pproch A. P. Zilińsi Crcow Univrsity of chnology Institut of Mchin Dsign pz@mch.p.du.pl rfftz / MFS Confrnc ohsiung iwn 5-8 Mrch 0 Bsic formultions
More informationINTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)
Chptr 7 INTEGRALS 7. Ovrviw 7.. Lt d d F () f (). Thn, w writ f ( ) d F () + C. Ths intgrls r clld indfinit intgrls or gnrl intgrls, C is clld constnt of intgrtion. All ths intgrls diffr y constnt. 7..
More informationLecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9
Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:
More informationIntegration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals
Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion
More informationStress and Strain Analysis of Notched Bodies Subject to Non-Proportional Loadings
World Acdmy of Scinc Enginring nd Tchnology Intrntionl Journl of Mchnicl nd Mchtronics Enginring Strss nd Strin Anlysis of Notchd Bodis Subjct to Non-Proportionl Lodings A. Inc Intrntionl Scinc Indx Mchnicl
More informationLecture 4. Conic section
Lctur 4 Conic sction Conic sctions r locus of points whr distncs from fixd point nd fixd lin r in constnt rtio. Conic sctions in D r curvs which r locus of points whor position vctor r stisfis r r. whr
More informationHomogenisation procedure to evaluate the effectiveness of masonry strengthening by CFRP repointing technique
PPLIED nd TEORETICL MECNICS. Ccci nd. riri omognistion procdur to lut t ffctinss of msonry strngtning y CFRP rpointing tcniqu. CECCI,. RIERI Diprtimnto di Costruzion dll rcitttur Unirsità IUV di Vnzi Dorsoduro,
More informationCase Study 1 PHA 5127 Fall 2006 Revised 9/19/06
Cas Study Qustion. A 3 yar old, 5 kg patint was brougt in for surgry and was givn a /kg iv bolus injction of a muscl rlaxant. T plasma concntrations wr masurd post injction and notd in t tabl blow: Tim
More informationCHAPTER 12. Finite-Volume (control-volume) Method-Introduction
CHAPR 12 Finit-Volum (control-volum) Mthod-Introduction 12-1 Introduction (1) In dvloing ht hs bcom knon s th finit-volum mthod, th consrvtion rincils r lid to fixd rgion in sc knon s control volum, r
More informationTOPIC 5: INTEGRATION
TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function
More informationCONTINUITY AND DIFFERENTIABILITY
MCD CONTINUITY AND DIFFERENTIABILITY NCERT Solvd mpls upto th sction 5 (Introduction) nd 5 (Continuity) : Empl : Chck th continuity of th function f givn by f() = + t = Empl : Emin whthr th function f
More informationTheoretical Study on the While Drilling Electromagnetic Signal Transmission of Horizontal Well
7 nd ntrntionl Confrnc on Softwr, Multimdi nd Communiction Enginring (SMCE 7) SBN: 978--6595-458-5 Thorticl Study on th Whil Drilling Elctromgntic Signl Trnsmission of Horizontl Wll Y-huo FAN,,*, Zi-ping
More informationA physical solution for solving the zero-flow singularity in static thermal-hydraulics
A ysicl solution for solving t zro-flow singulrity in sttic trml-ydrulics miing modls Dnil Bouskl Blig El Hfni EDF R&D 6, qui Wtir F-784 Ctou Cd, Frnc dnil.ouskl@df.fr lig.l-fni@df.fr Astrct For t D-D
More informationMulti-Section Coupled Line Couplers
/0/009 MultiSction Coupld Lin Couplrs /8 Multi-Sction Coupld Lin Couplrs W cn dd multipl coupld lins in sris to incrs couplr ndwidth. Figur 7.5 (p. 6) An N-sction coupld lin l W typiclly dsign th couplr
More informationI. The Connection between Spectroscopy and Quantum Mechanics
I. Th Connction twn Spctroscopy nd Quntum Mchnics On of th postults of quntum mchnics: Th stt of systm is fully dscrid y its wvfunction, Ψ( r1, r,..., t) whr r 1, r, tc. r th coordints of th constitunt
More informationCONIC SECTIONS. MODULE-IV Co-ordinate Geometry OBJECTIVES. Conic Sections
Conic Sctions 16 MODULE-IV Co-ordint CONIC SECTIONS Whil cutting crrot ou might hv noticd diffrnt shps shown th dgs of th cut. Anlticll ou m cut it in thr diffrnt ws, nml (i) (ii) (iii) Cut is prlll to
More informationMethod of Localisation and Controlled Ejection of Swarms of Likely Charged Particles
Method of Loclistion nd Controlled Ejection of Swrms of Likely Chrged Prticles I. N. Tukev July 3, 17 Astrct This work considers Coulom forces cting on chrged point prticle locted etween the two coxil,
More informationFSA. CmSc 365 Theory of Computation. Finite State Automata and Regular Expressions (Chapter 2, Section 2.3) ALPHABET operations: U, concatenation, *
CmSc 365 Thory of Computtion Finit Stt Automt nd Rgulr Exprssions (Chptr 2, Sction 2.3) ALPHABET oprtions: U, conctntion, * otin otin Strings Form Rgulr xprssions dscri Closd undr U, conctntion nd * (if
More informationFloating Point Number System -(1.3)
Floting Point Numbr Sstm -(.3). Floting Point Numbr Sstm: Comutrs rrsnt rl numbrs in loting oint numbr sstm: F,k,m,M 0. 3... k ;0, 0 i, i,...,k, m M. Nottions: th bs 0, k th numbr o igts in th bs xnsion
More informationFloating Point Number System -(1.3)
Floting Point Numbr Sstm -(.3). Floting Point Numbr Sstm: Comutrs rrsnt rl numbrs in loting oint numbr sstm: F,k,m,M 0. 3... k ;0, 0 i, i,...,k, m M. Nottions: th bs 0, k th numbr o igits in th bs xnsion
More informationChem 104A, Fall 2016, Midterm 1 Key
hm 104A, ll 2016, Mitrm 1 Ky 1) onstruct microstt tl for p 4 configurtion. Pls numrt th ms n ml for ch lctron in ch microstt in th tl. (Us th formt ml m s. Tht is spin -½ lctron in n s oritl woul writtn
More informationMinimum Spanning Trees
Minimum Spnning Trs Minimum Spnning Trs Problm A town hs st of houss nd st of rods A rod conncts nd only houss A rod conncting houss u nd v hs rpir cost w(u, v) Gol: Rpir nough (nd no mor) rods such tht:
More informationPhysics 43 HW #9 Chapter 40 Key
Pysics 43 HW #9 Captr 4 Ky Captr 4 1 Aftr many ours of dilignt rsarc, you obtain t following data on t potolctric ffct for a crtain matrial: Wavlngt of Ligt (nm) Stopping Potntial (V) 36 3 4 14 31 a) Plot
More informationHowever, many atoms can combine to form particular molecules, e.g. Chlorine (Cl) and Sodium (Na) atoms form NaCl molecules.
Lctur 6 Titl: Fundmntls of th Quntum Thory of molcul formtion Pg- In th lst modul, w hv discussd out th tomic structur nd tomic physics to undrstnd th spctrum of toms. Howvr, mny toms cn comin to form
More informationSOLVED EXAMPLES. be the foci of an ellipse with eccentricity e. For any point P on the ellipse, prove that. tan
LOCUS 58 SOLVED EXAMPLES Empl Lt F n F th foci of n llips with ccntricit. For n point P on th llips, prov tht tn PF F tn PF F Assum th llips to, n lt P th point (, sin ). P(, sin ) F F F = (-, 0) F = (,
More informationInstructions for Section 1
Instructions for Sction 1 Choos th rspons tht is corrct for th qustion. A corrct nswr scors 1, n incorrct nswr scors 0. Mrks will not b dductd for incorrct nswrs. You should ttmpt vry qustion. No mrks
More informationTrigonometric functions
Robrto s Nots on Diffrntial Calculus Captr 5: Drivativs of transcndntal functions Sction 5 Drivativs of Trigonomtric functions Wat you nd to know alrady: Basic trigonomtric limits, t dfinition of drivativ,
More informationNEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA
NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals
More informationJOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (JMET)
JOURNAL OF MECHANICAL ENGINEERING AND ECHNOLOGY (JME) Journl of Mchnicl Enginring nd chnology (JME) ISSN 47-94 (Print) ISSN 47-9 (Onlin) Volum Issu July -Dcmbr () ISSN 47-94 (Print) ISSN 47-9 (Onlin) Volum
More informationLast time: introduced our first computational model the DFA.
Lctur 7 Homwork #7: 2.2.1, 2.2.2, 2.2.3 (hnd in c nd d), Misc: Givn: M, NFA Prov: (q,xy) * (p,y) iff (q,x) * (p,) (follow proof don in clss tody) Lst tim: introducd our first computtionl modl th DFA. Tody
More informationGeneralized quaternions and their relations with Grassmann- Clifford procedure of doubling
UDC 9 Ykiv O Klinovsky, Drc, nior Rsrchr, Institut or Inormtion Rcordin Ntionl Acdmy o cinc o Ukrin, Kyiv, hk str,, Ukrin, E-mil: klinovsky@iu Yuliy E Boyrinov, PhD, Associt Prossor, Ntionl Tchnicl Univrsity
More informationMASTER CLASS PROGRAM UNIT 4 SPECIALIST MATHEMATICS SEMESTER TWO 2014 WEEK 11 WRITTEN EXAMINATION 1 SOLUTIONS
MASTER CLASS PROGRAM UNIT SPECIALIST MATHEMATICS SEMESTER TWO WEEK WRITTEN EXAMINATION SOLUTIONS FOR ERRORS AND UPDATES, PLEASE VISIT WWW.TSFX.COM.AU/MC-UPDATES QUESTION () Lt p ( z) z z z If z i z ( is
More informationCIE3109 : Structural Mechanics 4
CI3109 CI3109 : Structural echanics 4 13-14 Unsmmetrical and/or inhomogeneous cross sections Introduction General theor for extension and bending Unsmmetrical cross sections example : curvature versus
More informationA Study of the Solutions of the Lotka Volterra. Prey Predator System Using Perturbation. Technique
Inrnionl hmil orum no. 667-67 Sud of h Soluions of h o Volrr r rdor Ssm Using rurion Thniqu D.Vnu ol Ro * D. of lid hmis IT Collg of Sin IT Univrsi Vishnm.. Indi Y... Thorni D. of lid hmis IT Collg of
More informationCSE303 - Introduction to the Theory of Computing Sample Solutions for Exercises on Finite Automata
CSE303 - Introduction to th Thory of Computing Smpl Solutions for Exrciss on Finit Automt Exrcis 2.1.1 A dtrministic finit utomton M ccpts th mpty string (i.., L(M)) if nd only if its initil stt is finl
More informationThis Week. Computer Graphics. Introduction. Introduction. Graphics Maths by Example. Graphics Maths by Example
This Wk Computr Grphics Vctors nd Oprtions Vctor Arithmtic Gomtric Concpts Points, Lins nd Plns Eploiting Dot Products CSC 470 Computr Grphics 1 CSC 470 Computr Grphics 2 Introduction Introduction Wh do
More information6-6 Linear-Elastic Fracture Mechanics Method. Stress Life Testing: R. R. Moore Machine
6-6 Linr-Elstic Frctur Mchnics Mthod tg I Initition o micro-crck du to cyclic plstic dormtion tg II Progrsss to mcrocrck tht rptdly opns nd closs, crting nds clld ch mrks tg III Crck hs propgtd r nough
More informationFormal Concept Analysis
Forml Conpt Anlysis Conpt intnts s losd sts Closur Systms nd Implitions 4 Closur Systms 0.06.005 Nxt-Closur ws dvlopd y B. Gntr (984). Lt M = {,..., n}. A M is ltilly smllr thn B M, if B A if th smllst
More informationA ROTATING DISC IN CONSTANT PURE SHEAR BY S. KUMAR AND C. V. JOGA RAO
A ROTATING DISC IN CONSTANT PURE SHEAR BY S. KUMAR AND C. V. JOGA RAO (Deprtment of Aeronuticl Engineering, Indin Institute of Science, Bnglore-3) Received April 25, 1954 SUMMARY The disc of constnt pure
More informationWeighted Graphs. Weighted graphs may be either directed or undirected.
1 In mny ppltons, o rp s n ssot numrl vlu, ll wt. Usully, t wts r nonntv ntrs. Wt rps my tr rt or unrt. T wt o n s otn rrr to s t "ost" o t. In ppltons, t wt my msur o t lnt o rout, t pty o ln, t nry rqur
More informationTHE DETERMINATION of the signal magnitude at the
IEEE TANSACTIONS ON ELECTOMAGNETIC COMPATIBILITY, VOL 50, NO 3, AUGUST 2008 Clcultion of Elctricl Prmtrs of Two-Wir Lins in Multiconductor Cbls Boris M Lvin Abstrct A rigorous mthod for th clcultions of
More informationME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören
ME 522 PINCIPLES OF OBOTICS FIST MIDTEM EXAMINATION April 9, 202 Nm Lst Nm M. Kml Özgörn 2 4 60 40 40 0 80 250 USEFUL FOMULAS cos( ) cos cos sin sin sin( ) sin cos cos sin sin y/ r, cos x/ r, r 0 tn 2(
More informationHIGHER ORDER DIFFERENTIAL EQUATIONS
Prof Enriqu Mtus Nivs PhD in Mthmtis Edution IGER ORDER DIFFERENTIAL EQUATIONS omognous linr qutions with onstnt offiints of ordr two highr Appl rdution mthod to dtrmin solution of th nonhomognous qution
More informationC-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)
An ltntiv to th us of hypolic dclin cuvs Ppd y: Sfim Ltd S E R A F I M info@sfimltd.com P. +44 (02890 4206 www.sfimltd.com Contnts Contnts... i Intoduction... Initil ssumptions... Solving fo cumultiv...
More informationSection 3: Antiderivatives of Formulas
Chptr Th Intgrl Appli Clculus 96 Sction : Antirivtivs of Formuls Now w cn put th is of rs n ntirivtivs togthr to gt wy of vluting finit intgrls tht is ct n oftn sy. To vlut finit intgrl f(t) t, w cn fin
More informationThe model proposed by Vasicek in 1977 is a yield-based one-factor equilibrium model given by the dynamic
h Vsick modl h modl roosd by Vsick in 977 is yild-bsd on-fcor quilibrium modl givn by h dynmic dr = b r d + dw his modl ssums h h shor r is norml nd hs so-clld "mn rvring rocss" (undr Q. If w u r = b/,
More informationMathematics. Area under Curve.
Mthemtics Are under Curve www.testprepkrt.com Tle of Content 1. Introduction.. Procedure of Curve Sketching. 3. Sketching of Some common Curves. 4. Are of Bounded Regions. 5. Sign convention for finding
More information10. The Discrete-Time Fourier Transform (DTFT)
Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w
More informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More informationStatically indeterminate examples - axial loaded members, rod in torsion, members in bending
Elsticity nd Plsticity Stticlly indeterminte exmples - xil loded memers, rod in torsion, memers in ending Deprtment of Structurl Mechnics Fculty of Civil Engineering, VSB - Technicl University Ostrv 1
More informationGUC (Dr. Hany Hammad) 9/28/2016
U (r. Hny Hd) 9/8/06 ctur # 3 ignl flow grphs (cont.): ignl-flow grph rprsnttion of : ssiv sgl-port dvic. owr g qutions rnsducr powr g. Oprtg powr g. vill powr g. ppliction to Ntwork nlyzr lirtion. Nois
More informationPROBLEM SOLUTION
PROLEM 15.11 The 18-in.-rdius flywheel is rigidly ttched to 1.5-in.-rdius shft tht cn roll long prllel rils. Knowing tht t the instnt shown the center of the shft hs velocity of 1. in./s nd n ccelertion
More informationSolutions to Problems Integration in IR 2 and IR 3
Solutions to Problems Integrtion in I nd I. For ec of te following, evlute te given double integrl witout using itertion. Insted, interpret te integrl s, for emple, n re or n verge vlue. ) dd were is te
More informationANALYSIS OF MECHANICAL PROPERTIES OF COMPOSITE SANDWICH PANELS WITH FILLERS
ANALYSIS OF MECHANICAL PROPERTIES OF COMPOSITE SANDWICH PANELS WITH FILLERS A. N. Anoshkin *, V. Yu. Zuiko, A.V.Glezmn Perm Ntionl Reserch Polytechnic University, 29, Komsomolski Ave., Perm, 614990, Russi
More informationis an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h
For t BWR oprating paramtrs givn blow, comput and plot: a) T clad surfac tmpratur assuming t Jns-Lotts Corrlation b) T clad surfac tmpratur assuming t Tom Corrlation c) T clad surfac tmpratur assuming
More informationLinear Algebra Existence of the determinant. Expansion according to a row.
Lir Algbr 2270 1 Existc of th dtrmit. Expsio ccordig to row. W dfi th dtrmit for 1 1 mtrics s dt([]) = (1) It is sy chck tht it stisfis D1)-D3). For y othr w dfi th dtrmit s follows. Assumig th dtrmit
More informationu x A j Stress in the Ocean
Strss in t Ocan T tratmnt of strss and strain in fluids is comlicatd and somwat bond t sco of tis class. Tos rall intrstd sould look into tis rtr in Batclor Introduction to luid Dnamics givn as a rfrnc
More information(9) P (x)u + Q(x)u + R(x)u =0
STURM-LIOUVILLE THEORY 7 2. Second order liner ordinry differentil equtions 2.1. Recll some sic results. A second order liner ordinry differentil eqution (ODE) hs the form (9) P (x)u + Q(x)u + R(x)u =0
More informationCHAPTER 3 MECHANISTIC COMPARISON OF WATER CONING IN OIL AND GAS WELLS
CHAPTER 3 MECHANISTIC COMPARISON OF WATER CONING IN OIL AND GAS WELLS Wtr coning in gs lls hs n undrstood s phnomnon similr to tht in oil ll. In contrst to oil lls, rltivly f studis hv n rportd on spcts
More informationThe first practical supersonic wind tunnel, built by A. Busemann in Germany in the mid-1930s.
Introduction Th first rcticl sursonic wind tunnl, built by. Busmnn in Grmny in th mid-93s. lrg hyrsonic wind tunnl t th U.S. ir Forc Wright ronuticl Lbortory, Dyton, Ohio. Comrssibl Chnnl Flow Qusi--D
More informationContinuous Random Variables: Basics
Continuous Rndom Vrils: Bsics Brlin Chn Dprtmnt o Computr Scinc & Inormtion Enginring Ntionl Tiwn Norml Univrsit Rrnc: - D.. Brtss, J. N. Tsitsilis, Introduction to roilit, Sctions 3.-3.3 Continuous Rndom
More informationA REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007
A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H Thoms Shores Deprtment of Mthemtics University of Nebrsk Spring 2007 Contents Rtes of Chnge nd Derivtives 1 Dierentils 4 Are nd Integrls 5 Multivrite Clculus
More informationUNIT # 08 (PART - I)
. r. d[h d[h.5 7.5 mol L S d[o d[so UNIT # 8 (PRT - I CHEMICL INETICS EXERCISE # 6. d[ x [ x [ x. r [X[C ' [X [[B r '[ [B [C. r [NO [Cl. d[so d[h.5 5 mol L S d[nh d[nh. 5. 6. r [ [B r [x [y r' [x [y r'
More informationVSMN30 FINITA ELEMENTMETODEN - DUGGA
VSMN3 FINITA ELEMENTMETODEN - DUGGA 1-11-6 kl. 8.-1. Maximum points: 4, Rquird points to pass: Assistanc: CALFEM manual and calculator Problm 1 ( 8p ) 8 7 6 5 y 4 1. m x 1 3 1. m Th isotropic two-dimnsional
More informationANALYSIS OF FAST REACTORS SYSTEMS
ANALYSIS OF FAST REACTORS SYSTEMS M. Rghe 4/7/006 INTRODUCTION Fst rectors differ from therml rectors in severl spects nd require specil tretment. The prsitic cpture cross sections in the fuel, coolnt
More informationAustralian Journal of Basic and Applied Sciences. An Error Control Algorithm of Kowalsky's method for Orbit Determination of Visual Binaries
Austrlin Journl of Bsic nd Applid Scincs, 8(7) Novmbr 04, Pgs: 640-648 AENSI Journls Austrlin Journl of Bsic nd Applid Scincs ISSN:99-878 Journl hom pg: www.bswb.com An Error Control Algorithm of Kowlsky's
More informationLaboratory work # 8 (14) EXPERIMENTAL ESTIMATION OF CRITICAL STRESSES IN STRINGER UNDER COMPRESSION
Laboratory wor # 8 (14) XPRIMNTAL STIMATION OF CRITICAL STRSSS IN STRINGR UNDR COMPRSSION At action of comprssing ffort on a bar (column, rod, and stringr) two inds of loss of stability ar possibl: 1)
More informationCBSE 2015 FOREIGN EXAMINATION
CBSE 05 FOREIGN EXAMINATION (Sris SSO Cod No 65//F, 65//F, 65//F : Forign Rgion) Not tht ll th sts hv sm qustions Onl thir squnc of pprnc is diffrnt M Mrks : 00 Tim Allowd : Hours SECTION A Q0 Find th
More informationComposition and concentration dependences of electron mobility in semi-metal Hg 1 x Cd x Te quantum wells
Smiconductor Physics, Quntum Elctronics & Optolctronics, 15. V. 18, N. P. 97-1. doi: 1.1547/spqo18..97 PACS 7.1.Fg, 84.4.-x Composition nd concntrtion dpndncs of lctron mobility in smi-mtl Hg 1 x Cd x
More informationMAC-solutions of the nonexistent solutions of mathematical physics
Proceedings of the 4th WSEAS Interntionl Conference on Finite Differences - Finite Elements - Finite Volumes - Boundry Elements MAC-solutions of the nonexistent solutions of mthemticl physics IGO NEYGEBAUE
More informationSUPPLEMENTARY INFORMATION
DOI:.38/NMAT343 Hybrid Elstic olids Yun Li, Ying Wu, Ping heng, Zho-Qing Zhng* Deprtment of Physics, Hong Kong University of cience nd Technology Cler Wter By, Kowloon, Hong Kong, Chin E-mil: phzzhng@ust.hk
More informationLecture 21 : Graphene Bandstructure
Fundmnls of Nnolcronics Prof. Suprio D C 45 Purdu Univrsi Lcur : Grpn Bndsrucur Rf. Cpr 6. Nwor for Compuionl Nnocnolog Rviw of Rciprocl Lic :5 In ls clss w lrnd ow o consruc rciprocl lic. For D w v: Rl-Spc:
More informationResearch Article Mixed Initial-Boundary Value Problem for Telegraph Equation in Domain with Variable Borders
Advnces in Mthemticl Physics Volume 212, Article ID 83112, 17 pges doi:1.1155/212/83112 Reserch Article Mixed Initil-Boundry Vlue Problem for Telegrph Eqution in Domin with Vrible Borders V. A. Ostpenko
More informationThe Z transform techniques
h Z trnfor tchniqu h Z trnfor h th rol in dicrt yt tht th Lplc trnfor h in nlyi of continuou yt. h Z trnfor i th principl nlyticl tool for ingl-loop dicrt-ti yt. h Z trnfor h Z trnfor i to dicrt-ti yt
More informationPath (space curve) Osculating plane
Fo th cuilin motion of pticl in spc th fomuls did fo pln cuilin motion still lid. But th my b n infinit numb of nomls fo tngnt dwn to spc cu. Whn th t nd t ' unit ctos mod to sm oigin by kping thi ointtions
More informationPROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS
Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra
More informationLectures 2 & 3 - Population ecology mathematics refresher
Lcturs & - Poultio cology mthmtics rrshr To s th mov ito vloig oultio mols, th olloig mthmtics crisht is suli I i out r mthmtics ttook! Eots logrithms i i q q q q q q ( tims) / c c c c ) ( ) ( Clculus
More informationEXPLICIT SOLUTION TO GREEN AND AMPT INFILTRATION EQUATION
EXPLICIT SOLUTION TO GREEN AND AMPT INFILTRATION EQUATION By Srgio E. Srrno ABSTRACT: An xlicit solution of th Grn nd Amt infiltrtion qution is rsntd by constructing dcomosition sris. Siml xrssions for
More informationJournal of Constructional Steel Research
Journl of Constructionl Stl Rsrch 71 (1) 74 8 Contnts lists vill t SciVrs ScincDirct Journl of Constructionl Stl Rsrch Buckling control of cst modulr ductil rcing systm for sismic-rsistnt stl frms G. Fdrico,
More information(a) v 1. v a. v i. v s. (b)
Outlin RETIMING Struturl optimiztion mthods. Gionni D Mihli Stnford Unirsity Rtiming. { Modling. { Rtiming for minimum dly. { Rtiming for minimum r. Synhronous Logi Ntwork Synhronous Logi Ntwork Synhronous
More informationQuestions. denotes answer available in Student Solutions Manual/Study Guide; O denotes objective question
Qustions 95 Qustions dnots nswr vill in tudnt olutions Mnul/tudy Guid; O dnots ojctiv qustion. Th currnt in circuit contining coil, rsistor, nd ttry hs rchd constnt vlu. Dos th coil hv n inductnc? Dos
More informationAnalysis of Cantilever beams in Liquid Media: A case study of a microcantilever
Intrntionl Journl of Enginring Scinc Invntion (IJESI) ISSN (Onlin): 9 67, ISSN (Prin: 9 676 www.ijsi.org ǁ PP.57-6 Anlysis of Cntilvr bms in iquid Mdi: A cs study of microcntilvr S. Mnojkumr * nd J. Srinivs
More informationEffects of peripheral drilling moment on delamination using special drill bits
journl of mterils processing technology 01 (008 471 476 journl homepge: www.elsevier.com/locte/jmtprotec Effects of peripherl illing moment on delmintion using specil ill bits C.C. Tso,, H. Hocheng b Deprtment
More informationEngineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12
Enginring Bautiful HW #1 Pag 1 of 6 5.1 Two componnts of a minicomputr hav th following joint pdf for thir usful liftims X and Y: = x(1+ x and y othrwis a. What is th probability that th liftim X of th
More information