UNIT 1: Geometry of single point turning tools:
|
|
- Esther Peters
- 6 years ago
- Views:
Transcription
1 UNIT 1: Thery f Metal uttig: Sigle pit cuttig tl meclature, gemetry, Merchats circle diagram ad aalysis, Erst Merchat s sluti, shear agle relatiship, prblems f Merchat s aalysis, tl wear ad tl failure, tl life, effects f cuttig parameters tl life, tl failure criteria, Taylr s tl life equati, prblems tl life evaluati. Gemetry f sigle pit turig tls: 7 Hrs Istructial bjectives: At the ed f this less, the studet shuld be able t : (a) ceive rake agle ad clearace agle f cuttig tls (b) lassify systems f descripti f tl gemetry (c) Demstrate tl gemetry ad defie tl agles i : Machie eferece System Orthgal ake System ad Nrmal ake System (d) Desigate cuttig tl gemetry i ASA, OS ad NS Gemetry f sigle pit turig tls: Bth material ad gemetry f the cuttig tls play very imprtat rles their perfrmaces i achievig Effectiveess, Efficiecy ad Overall ecmy f machiig. uttig tls may be classified accrdig t the umber f majr cuttig edges (pits) ivlved as fllws: 1. Sigle pit: e.g., turig tls, shapig, plaig ad slttig tls ad brig tls 2. Duble (tw) pit: e.g., drills 3. Multipit (mre tha tw): e.g., millig cutters, brachig tls, hbs, gear shapig cutters etc. 1
2 (i) cept f rake ad clearace agles f cuttig tls. The wrd tl gemetry is basically referred t sme specific agles r slpe f the saliet faces ad edges f the tls at their cuttig pit. ake agle ad clearace agle are the mst sigificat fr all the cuttig tls. The ccept f rake agle ad clearace agle will be clear frm sme simple peratis shw i Fig. 1.1 Defiiti: Fig. 1.1 ake ad clearace agles f cuttig tls. ake agle (γ): Agle f icliati f rake surface frm referece plae. learace agle (α): Agle f icliati f clearace r flak surface frm the fiished surface ake agle: is prvided fr ease f chip flw ad verall machiig. ake agle may be psitive, r egative r eve zer as shw i Fig (a) psitive rake (b) zer rake (c) egative rake Fig. 1.2 Three pssible types f rake agles 2
3 elative advatages f such rake agles are: Psitive rake helps reduce cuttig frce ad thus cuttig pwer requiremet. Negative rake t icrease edge-stregth ad life f the tl Zer rake t simplify desig ad maufacture f the frm tls. learace agle: is essetially prvided t avid rubbig f the tl (flak) with the machied surface which causes lss f eergy ad damages f bth the tl ad the jb surface. Hece, clearace agle is a must ad must be psitive (3 ~ 15 depedig up tl-wrk materials ad type f the machiig peratis like turig, drillig, brig etc.) (ii) Systems f descripti f tl gemetry Tl-i-Had System where ly the saliet features f the cuttig tl pit are idetified r visualized as shw i Fig There is quatitative ifrmati, i.e., value f the agles. Fig. 1.3 Basic features f sigle pit tl (turig) i Tl-i-had system Machie eferece System ASA system 3
4 Tl eferece Systems Orthgal ake System OS Nrmal ake System NS Wrk eferece System WS (iii) Demstrati (expressi) f tl gemetry i : Machie eferece System: This system is als called ASA system; ASA stads fr America Stadards Assciati. Gemetry f a cuttig tl refers maily t its several agles r slpe f its saliet wrkig surfaces ad cuttig edges. Thse agles are expressed w.r.t. sme plaes f referece. I Machie eferece System (ASA), the three plaes f referece ad the crdiates are chse based the cfigurati ad axes f the machie tl ccered. The plaes ad axes used fr expressig tl gemetry i ASA system fr turig perati are shw i Fig Fig. 1.4 Plaes ad axes f referece i ASA system feed The plaes f referece ad the crdiates used i ASA system fr tl gemetry are : 4
5 π - π - π ad X Y - Z X Y m m m Where, π = eferece plae; plae perpedicular t the velcity vectr (shw i Fig. 1.4) π = Machie lgitudial plae; plae perpedicular t π ad take i the directi f assumed X lgitudial feed π = Machie Trasverse plae; plae perpedicular t bth π ad π [This plae is take i the directi Y X f assumed crss feed] The axes X m, Y m ad Z m are i the directi f lgitudial feed, crss feed ad cuttig velcity (vectr) respectively. The mai gemetrical features ad agles f sigle pit tls i ASA systems ad their defiitis will be clear frm Fig Fig. 1.5 Tl agles i ASA system Defiiti f: 5
6 ake agles: [Fig. 1.5] i ASA system: γ = side (axial rake: agle f icliati f the rake surface frm the referece plae (π ) ad easured x Machie ef. Plae, π. X γ = back rake: agle f icliati f the rake surface frm the referece plae ad measured Machie y Trasverse plae, π. Y learace agles: [Fig. 1.5]: α = side clearace: agle f icliati f the pricipal flak frm the machied surface (r V) ad measured x π plae. X α = back clearace: same as α but measured π plae. y x Y uttig agles: [Fig. 1.5]: φ = apprach agle: agle betwee the pricipal cuttig edge (its prjecti π ) ad π ad measured s Y π φ = ed cuttig edge agle: agle betwee the ed cuttig edge (its prjecti π ) frm π ad measured e X π Nse radius, r (i ich): r = se radius : curvature f the tl tip. It prvides stregtheig f the tl se ad better surface fiish. Tl eferece Systems Orthgal ake System OS: This system is als kw as ISO ld. The plaes f referece ad the c-rdiate axes used fr expressig the tl agles i OS are: π - π - π O ad X - Y - Z which are take i respect f the tl cfigurati as idicated i Fig
7 Fig. 1.6 Plaes ad axes f referece i O Where, π = eferece plae perpedicular t the cuttig velcity vectr, V π = cuttig plae; plae perpedicular t π ad take alg the pricipal cuttig edge π O = Orthgal plae; plae perpedicular t bth π ad π ad the axes; X = alg the lie f itersecti f π ad π O Y = alg the lie f itersecti f π ad π Z = alg the velcity vectr, i.e., rmal t bth X ad Y axes. The mai gemetrical agles used t express tl gemetry i Orthgal ake System (OS) ad their defiitis will be clear frm Fig
8 Fig. 1.7 Tl agles i OS system Defiiti f ake agles [Fig. 1.7] i OS: γ = rthgal rake: agle f icliati f the rake surface frm eferece plae, π ad measured the rthgal plae, π λ = icliati agle; agle betwee π frm the directi f assumed lgitudial feed [π ] ad measured X π learace agles [Fig. 1.7]: α = rthgal clearace f the pricipal flak: agle f icliati f the pricipal flak frm π ad measured π α = auxiliary rthgal clearace: agle f icliati f the auxiliary flak frm auxiliary cuttig plae, π ad measured auxiliary rthgal plae, π as idicated i Fig
9 uttig agles [Fig. 1.7]: φ = pricipal cuttig edge agle: agle betwee π ad the directi f assumed lgitudial feed r π X ad measured π φ 1 = auxiliary cuttig agle: agle betwee π ad π X ad measured π Nse radius, r (mm): r = radius f curvature f tl tip Fig. 1.8 Auxiliary rthgal clearace agle Nrmal ake System NS: This system is als kw as ISO ew. ASA system has limited advatage ad use like cveiece f ispecti. But OS is advatageusly used fr aalysis ad research i machiig ad tl perfrmace. But OS des t reveal the true picture f the tl gemetry whe the cuttig edges are iclied frm the referece plae, i.e., λ 0. Besides, sharpeig r resharpeig, if ecessary, f the tl by gridig i OS requires sme additial calculatis fr crrecti f agles. 9
10 These tw limitatis f OS are vercme by usig NS fr descripti ad use f tl gemetry. The basic differece betwee OS ad NS is the fact that i OS, rake ad clearace agles are visualized i the rthgal plae, π, whereas i NS thse agles are visualized i ather plae called Nrmal plae, π. The rthgal plae, π is simply rmal t π ad π irrespective f the icliati f the cuttig edges, N i.e., λ, but π (ad π fr auxiliary cuttig edge) is always rmal t the cuttig edge. The differeces betwee N N OS ad NS have bee depicted i Fig The plaes f referece ad the crdiates used i NS are: π - π - π ad X Y Z N N where, π = rmal referece plae N π = Nrmal plae: plae rmal t the cuttig edge N ad X = X Y = cuttig edge Z = rmal t X ad Y It is t be ted that whe λ = 0, NS ad OS becme same, i.e. π π N, Y N Y ad Z Z. Defiiti (i NS) f ake agles: γ = rmal rake: agle f icliati agle f the rake surface frm π ad measured rmal plae, π N α = rmal clearace: agle f icliati f the pricipal flak frm π ad measured π N α = auxiliary clearace agle: rmal clearace f the auxiliary flak (measured π plae rmal t N the auxiliary cuttig edge. The cuttig agles, φ ad φ 1 ad se radius, r (mm) are same i OS ad NS. 10
11 Fig. 1.9 Differeces f NS frm OS w.r.t. cuttig tl gemetry. (b) Desigati f tl gemetry The gemetry f a sigle pit tl is desigated r specified by a series f values f the saliet agles ad se radius arraged i a defiite sequece as fllws: Desigati (sigature) f tl gemetry i ASA System γ, γ, α, α, φ, φ, r (ich) y x y x e s OS System λ, γ, α, α, φ, φ, r (mm) 1 NS System λ, γ, α, α, φ, φ, r (mm) 1 11
12 Quiz Test: Select the crrect aswer frm the give fur ptis : 1. Back rake f a turig tl is measured its (a) machie lgitudial plae (b) machie trasverse plae (c) rthgal plae (d) rmal plae 2. Nrmal rake ad rthgal rake f a turig tl will be same whe its (a) φ = 0 (b) φ = 0 (c) λ = 0 (d) φ = Nrmal plae f a turig tl is always perpedicular t its (a) π plae (b) π plae (c) π plae (d) e f them X Y 4. Pricipal cuttig edge agle f ay turig tl is measured its (a) π (b) π (c) π Y X (d) π 5. A cuttig tl ca ever have its (a) rake agle psitive (b) rake agle egative (c) clearace agle psitive (d) clearace agle egative 6. Orthgal clearace ad side clearace f a turig tl will be same if its perpedicular cuttig edge agle is (a) φ = 30 (b) φ = 45 (c) φ = 60 (d) φ = Icliati agle f a turig tl is measured its (a) referece plae (b) cuttig plae (c) rthgal plae (d) rmal plae 8. Nrmal rake ad side rake f a turig tl will be same if its (a) φ = 0 ad λ = 0 (b) φ = 90 ad λ = 0 (c) φ = 90 ad λ = 90 (d) φ = 0 ad λ = 90 Aswer f the bjective questis 1 (b) 2 (c) 3 (c) 4 (a) 5 (d) 6 (d) 7 (b) 8 (b) 12
13 Failure f cuttig tls ad tl life: Istructial bjectives: At the ed f this less, yu will be able t i) State hw the cuttig tls fail ii) Illustrate the mechaisms ad patter f tl wear iii) Ascertai the essetial prperties f cuttig tl materials iv) Defie ad assess tl life v) Develp ad use tl life equati. (i) Failure f cuttig tls: Smth, safe ad ecmic machiig ecessitate Preveti f premature ad catastrphic failure f the cuttig tls educti f rate f wear f tl t prlg its life T accmplish the afresaid bjectives e shuld first kw why ad hw the cuttig tls fail. uttig tls geerally fail by: i) Mechaical breakage due t excessive frces ad shcks. Such kid f tl failure is radm ad catastrphic i ature ad hece are extremely detrimetal. ii) Quick dullig by plastic defrmati due t itesive stresses ad temperature. This type f failure als ccurs rapidly ad are quite detrimetal ad uwated. iii) Gradual wear f the cuttig tl at its flaks ad rake surface. The first tw mdes f tl failure are very harmful t ly fr the tl but als fr the jb ad the machie tl. Hece these kids f tl failure eed t be preveted by usig suitable tl materials ad gemetry depedig up the wrk material ad cuttig cditi. But failure by gradual wear, which is ievitable, cat be preveted but ca be slwed dw ly t ehace the service life f the tl. 13
14 The cuttig tl is withdraw immediately after it fails r, if pssible, just befre it ttally fails. Fr that e must uderstad that the tl has failed r is gig t fail shrtly. It is uderstd r csidered that the tl has failed r abut t fail by e r mre f the fllwig cditis : (a) I &D labratries Ttal breakage f the tl r tl tip(s) Massive fracture at the cuttig edge(s) Excessive icrease i cuttig frces ad/r vibrati Average wear (flak r crater) reaches its specified limit(s) (b) I machiig idustries Excessive (beyd limit) curret r pwer csumpti Excessive vibrati ad/r abrmal sud (chatter) Ttal breakage f the tl Dimesial deviati beyd tlerace apid wrseig f surface fiish Adverse chip frmati. (ii) Mechaisms ad patter (gemetry) f cuttig tl wear: Fr the purpse f ctrllig tl wear e must uderstad the varius mechaisms f wear, that the cuttig tl uderges uder differet cditis. The cmm mechaisms f cuttig tl wear are : i) Mechaical wear Thermally isesitive type; like abrasi, chippig ad delamiati Thermally sesitive type; like adhesi, fracturig, flakig etc. ii) Thermchemical wear Macr-diffusi by mass dissluti 14
15 Micr-diffusi by atmic migrati iii) hemical wear iv) Galvaic wear I diffusi wear the material frm the tl at its rubbig surfaces, particularly at the rake surface gradually diffuses it the flwig chips either i bulk r atm by atm whe the tl material has chemical affiity r slid slubility twards the wrk material. The rate f such tl wear icreases with the icrease i temperature at the cuttig ze. Diffusi wear becmes predmiat whe the cuttig temperature becmes very high due t high cuttig velcity ad high stregth f the wrk material. hemical wear, leadig t damages like grvig wear may ccur if the tl material is t eugh chemically stable agaist the wrk material ad/r the atmspheric gases. Galvaic wear, based electrchemical dissluti, seldm ccurs whe bth the wrk tl materials are electrically cductive, cuttig ze temperature is high ad the cuttig fluid acts as a electrlyte. The usual patter r gemetry f wear f turig ad face millig iserts are typically shw i Fig (a ad b) ad Fig respectively. 15
16 Fig (a) Gemetry ad majr features f wear f turig tls Fig (b) Phtgraphic view f the wear patter f a turig tl isert 16
17 Fig Schematic (a) ad actual view (b) f wear patter f face millig isert I additi t ultimate failure f the tl, the fllwig effects are als caused by the grwig tl-wear : Icrease i cuttig frces ad pwer csumpti maily due t the pricipal flak wear Icrease i dimesial deviati ad surface rughess maily due t wear f the tl-tips ad auxiliary flak wear (V s ) Odd sud ad vibrati Wrseig surface itegrity Mechaically weakeig f the tl tip. (iii) Essetial prperties fr cuttig tl materials: The cuttig tls eed t be capable t meet the grwig demads fr higher prductivity ad ecmy as well as t machie the extic materials which are cmig up with the rapid prgress i sciece ad techlgy. The cuttig tl material f the day ad future essetially require the fllwig prperties t resist r retard the phemea leadig t radm r early tl failure: 1. High mechaical stregth; cmpressive, tesile, ad TA 2. Fracture tughess high r at least adequate 17
18 3. High hardess fr abrasi resistace 4. High ht hardess t resist plastic defrmati ad reduce wear rate at elevated temperature 5. hemical stability r iertess agaist wrk material, atmspheric gases ad cuttig fluids 6. esistace t adhesi ad diffusi 7. Thermal cductivity lw at the surface t resist icmig f heat ad high at the cre t quickly dissipate the heat etered 8. High heat resistace ad stiffess 9. Maufacturability, availability ad lw cst. Tl Life: Defiiti Tl life geerally idicates, the amut f satisfactry perfrmace r service redered by a fresh tl r a cuttig pit till it is declared failed. Tl life is defied i tw ways : (a) I & D : Actual machiig time (perid) by which a fresh cuttig tl (r pit) satisfactrily wrks after which it eeds replacemet r recditiig. The mder tls hardly fail prematurely r abruptly by mechaical breakage r rapid plastic defrmati. Thse fail mstly by wearig prcess which systematically grws slwly with machiig time. I that case, tl life meas the spa f actual machiig time by which a fresh tl ca wrk befre attaiig the specified limit f tl wear. Mstly tl life is decided by the machiig time till flak wear, V reaches 0.3 mm r crater B wear, K reaches 0.15 mm. T (b) I idustries r shp flr : The legth f time f satisfactry service r amut f acceptable utput prvided by a fresh tl prir t it is required t replace r recditi. Assessmet f tl life Fr & D purpses, tl life is always assessed r expressed by spa f machiig time i miutes, 18
19 B Maufacturig Prcess II 06 ME45 Whereas, i idustries besides machiig time i miutes sme ther meas are als used t assess tl life, depedig up the situati, such as N. f pieces f wrk machied Ttal vlume f material remved Ttal legth f cut. Measuremet f tl wear The varius methds are : 1. By lss f tl material i vlume r weight, i e life time this methd is crude ad is geerally applicable fr critical tls like gridig wheels. 2. By grvig ad idetati methd i this apprximate methd wear depth is measured idirectly by the differece i legth f the grve r the idetati utside ad iside the wr area 3. Usig ptical micrscpe fitted with micrmeter very cmm ad effective methd 4. Usig scaig electr micrscpe (SEM) used geerally, fr detailed study; bth qualitative ad quatitative 5. Talysurf, specially fr shallw crater wear. Taylr s tl life equati: Wear ad hece tl life f ay tl fr ay wrk material is gvered maily by the level f the machiig parameters i.e., cuttig velcity, (V ), feed, (s ) ad depth f cut (t). uttig velcity affects maximum ad depth f cut miimum. The usual patter f grwth f cuttig tl wear (maily V B ), priciple f assessig tl life ad its depedece cuttig velcity are schematically shw i Fig
20 Fig Grwth f flak wear ad assessmet f tl life The tl life bviusly decreases with the icrease i cuttig velcity keepig ther cditis ualtered as idicated i Fig If the tl lives, T, T, T, T etc are pltted agaist the crrespdig cuttig velcities, V, V, V, V etc as shw i Fig. 1.13, a smth curve like a rectagular hyperbla is fud t appear. Whe F. W. Taylr pltted the same figure takig bth V ad T i lg-scale, a mre distict liear relatiship appeared as schematically shw i Fig With the slpe, ad itercept, c, Taylr derived the simple equati as VT = 20
21 where, is called, Taylr s tl life expet. The values f bth ad c deped maily up the tlwrk materials ad the cuttig evirmet (cuttig fluid applicati). The value f depeds als the limitig value f V udertake ( i.e., 0.3 mm, 0.4 mm, 0.6 mm etc.) B Fig uttig velcity tl life relatiship Fig uttig velcity vs tl life a lg-lg scale 21
22 Example f use f Taylr s tl life equati Prblem : If i turig f a steel rd by a give cuttig tl (material ad gemetry) at a give machiig cditi (s ad t) uder a give evirmet (cuttig fluid applicati), the tl life decreases frm 80 mi t 20 mi. due t icrease i cuttig velcity, V frm 60 m/mi t 120 m/mi., the at what cuttig velcity the life f that tl uder the same cditi ad evirmet will be 40 mi.? Sluti : Assumig Taylr s tl life equati, VT = V1T 1 = V2T2 = V3T 3 =... Here, V 1 = 60 m/mi; T 1 = 80 mi. V 2 = 120 m/mi; T 2 = 20 mi. V 3 =? (t be determied); T 3 = 40 mi. Takig, VT = VT i.e., T 1 V 2 = T2 V1 frm which, = 0.5 Agai, VT = VT i.e, V 3 T 1 = V1 T3 ad V 3 = m/mi 22
23 Mdified Taylr s Tl Life equati I Taylr s tl life equati, ly the effect f variati f cuttig velcity, V tl life has bee csidered. But practically, the variati i feed (s ) ad depth f cut (t) als play rle tl life t sme extet. Takig it accut the effects f all thse parameters, the Taylr s tl life equati has bee mdified as, TL T = x y z Vc S0 t where, TL = tl life i mi T = A cstat depedig maily up the tl wrk materials ad the limitig value f V B udertake. x, y ad z - expets s called tl life expets depedig up the tl wrk materials ad the machiig evirmet. Geerally, x > y > z as V affects tl life maximum ad t miimum. The values f the cstats, T, x, y ad z are available i Machiig Data Hadbks r ca be evaluated by machiig tests. 23
24 Quiz Test Idetify the crrect aswer frm the give fur ptis. 1. I high speed machiig f steels the teeth f millig cutters may fail by (a) mechaical breakage (b) plastic defrmati (c) wear (d) all f the abve 2. Tl life i turig will decrease by maximum extet if we duble the (a) depth f cut (b) feed (c) cuttig velcity (d) tl rake agle 3. I cuttig tls, crater wear develps at (a) the rake surface (b) the pricipal flak (c) the auxiliary flak (d) the tl se 4. T prevet plastic defrmati at the cuttig edge, the tl material shuld pssess (a) high fracture tughess (b) high ht hardess (c) chemical stability (d) adhesi resistace Prblems Prblem 1 Durig turig a metallic rd at a give cditi, the tl life was fud t icrease frm 25 mi t 50 mi. whe V was reduced frm 100 m/mi t 80 m/mi. Hw much will be the life f that tl if machiedat 90 m/mi? Prblem 2 While drillig hles i steel plate by a 20 mm diameter HSS drill at a give feed, the tl life decreased frm 40 mi. t 24 mi. whe speed was raised frm 250 rpm t 320 rpm. At what speed (rpm) the life f that drill uder the same cditi wuld be 30 mi.? Aswers f the questis f Quiz Test Q. 1 : (d) Q. 2 : (c) Q. 3 : (a) Q. 4 : (b) Sluti t Prblem 1. As mi Sluti t Prblem 2 As. 287 rpm. 24
Solutions. Definitions pertaining to solutions
Slutis Defiitis pertaiig t slutis Slute is the substace that is disslved. It is usually preset i the smaller amut. Slvet is the substace that des the disslvig. It is usually preset i the larger amut. Slubility
More informationGrade 3 Mathematics Course Syllabus Prince George s County Public Schools
Ctet Grade 3 Mathematics Curse Syllabus Price Gerge s Cuty Public Schls Prerequisites: Ne Curse Descripti: I Grade 3, istructial time shuld fcus fur critical areas: (1) develpig uderstadig f multiplicati
More informationChapter 3.1: Polynomial Functions
Ntes 3.1: Ply Fucs Chapter 3.1: Plymial Fuctis I Algebra I ad Algebra II, yu ecutered sme very famus plymial fuctis. I this secti, yu will meet may ther members f the plymial family, what sets them apart
More informationx 2 x 3 x b 0, then a, b, c log x 1 log z log x log y 1 logb log a dy 4. dx As tangent is perpendicular to the x axis, slope
The agle betwee the tagets draw t the parabla y = frm the pit (-,) 5 9 6 Here give pit lies the directri, hece the agle betwee the tagets frm that pit right agle Ratig :EASY The umber f values f c such
More informationAxial Temperature Distribution in W-Tailored Optical Fibers
Axial Temperature Distributi i W-Tailred Optical ibers Mhamed I. Shehata (m.ismail34@yah.cm), Mustafa H. Aly(drmsaly@gmail.cm) OSA Member, ad M. B. Saleh (Basheer@aast.edu) Arab Academy fr Sciece, Techlgy
More informationIntermediate Division Solutions
Itermediate Divisi Slutis 1. Cmpute the largest 4-digit umber f the frm ABBA which is exactly divisible by 7. Sluti ABBA 1000A + 100B +10B+A 1001A + 110B 1001 is divisible by 7 (1001 7 143), s 1001A is
More informationMATH Midterm Examination Victor Matveev October 26, 2016
MATH 33- Midterm Examiati Victr Matveev Octber 6, 6. (5pts, mi) Suppse f(x) equals si x the iterval < x < (=), ad is a eve peridic extesi f this fucti t the rest f the real lie. Fid the csie series fr
More informationALE 26. Equilibria for Cell Reactions. What happens to the cell potential as the reaction proceeds over time?
Name Chem 163 Secti: Team Number: AL 26. quilibria fr Cell Reactis (Referece: 21.4 Silberberg 5 th editi) What happes t the ptetial as the reacti prceeds ver time? The Mdel: Basis fr the Nerst quati Previusly,
More informationENGI 4421 Central Limit Theorem Page Central Limit Theorem [Navidi, section 4.11; Devore sections ]
ENGI 441 Cetral Limit Therem Page 11-01 Cetral Limit Therem [Navidi, secti 4.11; Devre sectis 5.3-5.4] If X i is t rmally distributed, but E X i, V X i ad is large (apprximately 30 r mre), the, t a gd
More informationQuantum Mechanics for Scientists and Engineers. David Miller
Quatum Mechaics fr Scietists ad Egieers David Miller Time-depedet perturbati thery Time-depedet perturbati thery Time-depedet perturbati basics Time-depedet perturbati thery Fr time-depedet prblems csider
More informationMATHEMATICS 9740/01 Paper 1 14 Sep hours
Cadidate Name: Class: JC PRELIMINARY EXAM Higher MATHEMATICS 9740/0 Paper 4 Sep 06 3 hurs Additial Materials: Cver page Aswer papers List f Frmulae (MF5) READ THESE INSTRUCTIONS FIRST Write yur full ame
More informationBIO752: Advanced Methods in Biostatistics, II TERM 2, 2010 T. A. Louis. BIO 752: MIDTERM EXAMINATION: ANSWERS 30 November 2010
BIO752: Advaced Methds i Bistatistics, II TERM 2, 2010 T. A. Luis BIO 752: MIDTERM EXAMINATION: ANSWERS 30 Nvember 2010 Questi #1 (15 pits): Let X ad Y be radm variables with a jit distributi ad assume
More informationPhysical Chemistry Laboratory I CHEM 445 Experiment 2 Partial Molar Volume (Revised, 01/13/03)
Physical Chemistry Labratry I CHEM 445 Experimet Partial Mlar lume (Revised, 0/3/03) lume is, t a gd apprximati, a additive prperty. Certaily this apprximati is used i preparig slutis whse ccetratis are
More informationSound Absorption Characteristics of Membrane- Based Sound Absorbers
Purdue e-pubs Publicatis f the Ray W. Schl f Mechaical Egieerig 8-28-2003 Sud Absrpti Characteristics f Membrae- Based Sud Absrbers J Stuart Blt, blt@purdue.edu Jih Sg Fllw this ad additial wrks at: http://dcs.lib.purdue.edu/herrick
More informationE o and the equilibrium constant, K
lectrchemical measuremets (Ch -5 t 6). T state the relati betwee ad K. (D x -b, -). Frm galvaic cell vltage measuremet (a) K sp (D xercise -8, -) (b) K sp ad γ (D xercise -9) (c) K a (D xercise -G, -6)
More informationD.S.G. POLLOCK: TOPICS IN TIME-SERIES ANALYSIS STATISTICAL FOURIER ANALYSIS
STATISTICAL FOURIER ANALYSIS The Furier Represetati f a Sequece Accrdig t the basic result f Furier aalysis, it is always pssible t apprximate a arbitrary aalytic fucti defied ver a fiite iterval f the
More information[1 & α(t & T 1. ' ρ 1
NAME 89.304 - IGNEOUS & METAMORPHIC PETROLOGY DENSITY & VISCOSITY OF MAGMAS I. Desity The desity (mass/vlume) f a magma is a imprtat parameter which plays a rle i a umber f aspects f magma behavir ad evluti.
More informationEvery gas consists of a large number of small particles called molecules moving with very high velocities in all possible directions.
Kietic thery f gases ( Kietic thery was develped by Berlli, Jle, Clasis, axwell ad Bltzma etc. ad represets dyamic particle r micrscpic mdel fr differet gases sice it thrws light the behir f the particles
More information5.80 Small-Molecule Spectroscopy and Dynamics
MIT OpeCurseWare http://cw.mit.edu 5.8 Small-Mlecule Spectrscpy ad Dyamics Fall 8 Fr ifrmati abut citig these materials r ur Terms f Use, visit: http://cw.mit.edu/terms. 5.8 Lecture #33 Fall, 8 Page f
More informationUnit -2 THEORY OF DILUTE SOLUTIONS
Uit - THEORY OF DILUTE SOLUTIONS 1) hat is sluti? : It is a hmgeus mixture f tw r mre cmpuds. ) hat is dilute sluti? : It is a sluti i which slute ccetrati is very less. 3) Give a example fr slid- slid
More informationENGI 4421 Central Limit Theorem Page Central Limit Theorem [Navidi, section 4.11; Devore sections ]
ENGI 441 Cetral Limit Therem Page 11-01 Cetral Limit Therem [Navidi, secti 4.11; Devre sectis 5.3-5.4] If X i is t rmally distributed, but E X i, V X i ad is large (apprximately 30 r mre), the, t a gd
More informationCh. 1 Introduction to Estimation 1/15
Ch. Itrducti t stimati /5 ample stimati Prblem: DSB R S f M f s f f f ; f, φ m tcsπf t + φ t f lectrics dds ise wt usually white BPF & mp t s t + w t st. lg. f & φ X udi mp cs π f + φ t Oscillatr w/ f
More informationMulti-objective Programming Approach for. Fuzzy Linear Programming Problems
Applied Mathematical Scieces Vl. 7 03. 37 8-87 HIKARI Ltd www.m-hikari.cm Multi-bective Prgrammig Apprach fr Fuzzy Liear Prgrammig Prblems P. Padia Departmet f Mathematics Schl f Advaced Scieces VIT Uiversity
More informationDesign and Implementation of Cosine Transforms Employing a CORDIC Processor
C16 1 Desig ad Implemetati f Csie Trasfrms Emplyig a CORDIC Prcessr Sharaf El-Di El-Nahas, Ammar Mttie Al Hsaiy, Magdy M. Saeb Arab Academy fr Sciece ad Techlgy, Schl f Egieerig, Alexadria, EGYPT ABSTRACT
More informationA Hartree-Fock Calculation of the Water Molecule
Chemistry 460 Fall 2017 Dr. Jea M. Stadard Nvember 29, 2017 A Hartree-Fck Calculati f the Water Mlecule Itrducti A example Hartree-Fck calculati f the water mlecule will be preseted. I this case, the water
More informationExamination No. 3 - Tuesday, Nov. 15
NAME (lease rit) SOLUTIONS ECE 35 - DEVICE ELECTRONICS Fall Semester 005 Examiati N 3 - Tuesday, Nv 5 3 4 5 The time fr examiati is hr 5 mi Studets are allwed t use 3 sheets f tes Please shw yur wrk, artial
More information, the random variable. and a sample size over the y-values 0:1:10.
Lecture 3 (4//9) 000 HW PROBLEM 3(5pts) The estimatr i (c) f PROBLEM, p 000, where { } ~ iid bimial(,, is 000 e f the mst ppular statistics It is the estimatr f the ppulati prprti I PROBLEM we used simulatis
More informationMarkov processes and the Kolmogorov equations
Chapter 6 Markv prcesses ad the Klmgrv equatis 6. Stchastic Differetial Equatis Csider the stchastic differetial equati: dx(t) =a(t X(t)) dt + (t X(t)) db(t): (SDE) Here a(t x) ad (t x) are give fuctis,
More informationStudy in Cylindrical Coordinates of the Heat Transfer Through a Tow Material-Thermal Impedance
Research ural f Applied Scieces, Egieerig ad echlgy (): 9-63, 3 ISSN: 4-749; e-issn: 4-7467 Maxwell Scietific Orgaiati, 3 Submitted: uly 4, Accepted: September 8, Published: May, 3 Study i Cylidrical Crdiates
More informationAP Statistics Notes Unit Eight: Introduction to Inference
AP Statistics Ntes Uit Eight: Itrducti t Iferece Syllabus Objectives: 4.1 The studet will estimate ppulati parameters ad margis f errrs fr meas. 4.2 The studet will discuss the prperties f pit estimatrs,
More informationStudy of Energy Eigenvalues of Three Dimensional. Quantum Wires with Variable Cross Section
Adv. Studies Ther. Phys. Vl. 3 009. 5 3-0 Study f Eergy Eigevalues f Three Dimesial Quatum Wires with Variale Crss Secti M.. Sltai Erde Msa Departmet f physics Islamic Aad Uiversity Share-ey rach Ira alrevahidi@yah.cm
More informationThe Acoustical Physics of a Standing Wave Tube
UIUC Physics 93POM/Physics 406POM The Physics f Music/Physics f Musical Istrumets The Acustical Physics f a Stadig Wave Tube A typical cylidrical-shaped stadig wave tube (SWT) {aa impedace tube} f legth
More informationA Study on Estimation of Lifetime Distribution with Covariates Under Misspecification
Prceedigs f the Wrld Cgress Egieerig ad Cmputer Sciece 2015 Vl II, Octber 21-23, 2015, Sa Fracisc, USA A Study Estimati f Lifetime Distributi with Cvariates Uder Misspecificati Masahir Ykyama, Member,
More informationA New Method for Finding an Optimal Solution. of Fully Interval Integer Transportation Problems
Applied Matheatical Scieces, Vl. 4, 200,. 37, 89-830 A New Methd fr Fidig a Optial Sluti f Fully Iterval Iteger Trasprtati Prbles P. Padia ad G. Nataraja Departet f Matheatics, Schl f Advaced Scieces,
More informationare specified , are linearly independent Otherwise, they are linearly dependent, and one is expressed by a linear combination of the others
Chater 3. Higher Order Liear ODEs Kreyszig by YHLee;4; 3-3. Hmgeeus Liear ODEs The stadard frm f the th rder liear ODE ( ) ( ) = : hmgeeus if r( ) = y y y y r Hmgeeus Liear ODE: Suersiti Pricile, Geeral
More informationChapter 5. Root Locus Techniques
Chapter 5 Rt Lcu Techique Itrducti Sytem perfrmace ad tability dt determied dby cled-lp l ple Typical cled-lp feedback ctrl ytem G Ope-lp TF KG H Zer -, - Ple 0, -, - K Lcati f ple eaily fud Variati f
More informationChapter 4. Problem Solutions
Chapter 4. Prblem Slutis. The great majrity f alpha particles pass thrugh gases ad thi metal fils with deflectis. T what cclusi abut atmic structure des this bservati lead? The fact that mst particles
More informationIdentical Particles. We would like to move from the quantum theory of hydrogen to that for the rest of the periodic table
We wuld like t ve fr the quatu thery f hydrge t that fr the rest f the peridic table Oe electr at t ultielectr ats This is cplicated by the iteracti f the electrs with each ther ad by the fact that the
More informationThe Excel FFT Function v1.1 P. T. Debevec February 12, The discrete Fourier transform may be used to identify periodic structures in time ht.
The Excel FFT Fucti v P T Debevec February 2, 26 The discrete Furier trasfrm may be used t idetify peridic structures i time ht series data Suppse that a physical prcess is represeted by the fucti f time,
More informationAuthor. Introduction. Author. o Asmir Tobudic. ISE 599 Computational Modeling of Expressive Performance
ISE 599 Cmputatial Mdelig f Expressive Perfrmace Playig Mzart by Aalgy: Learig Multi-level Timig ad Dyamics Strategies by Gerhard Widmer ad Asmir Tbudic Preseted by Tsug-Ha (Rbert) Chiag April 5, 2006
More informationA unified brittle fracture criterion for structures with sharp V-notches under mixed mode loading
Jural f Mechaical Sciece ad Techlgy Jural f Mechaical Sciece ad Techlgy 22 (2008) 269~278 www.sprigerlik.cm/ctet/738-494x A uified brittle fracture criteri fr structures with sharp V-tches uder mixed mde
More informationReview for cumulative test
Hrs Math 3 review prblems Jauary, 01 cumulative: Chapters 1- page 1 Review fr cumulative test O Mday, Jauary 7, Hrs Math 3 will have a curse-wide cumulative test cverig Chapters 1-. Yu ca expect the test
More informationFourier Method for Solving Transportation. Problems with Mixed Constraints
It. J. Ctemp. Math. Scieces, Vl. 5, 200,. 28, 385-395 Furier Methd fr Slvig Trasprtati Prblems with Mixed Cstraits P. Padia ad G. Nataraja Departmet f Mathematics, Schl f Advaced Scieces V I T Uiversity,
More information5.1 Two-Step Conditional Density Estimator
5.1 Tw-Step Cditial Desity Estimatr We ca write y = g(x) + e where g(x) is the cditial mea fucti ad e is the regressi errr. Let f e (e j x) be the cditial desity f e give X = x: The the cditial desity
More informationAPPLICATION OF FEM ANALYSIS METHODS TO A CYLINDER-CYLINDER INTERSECTION STRUCTURE
18th Iteratial Cferece Structural Mechaics i Reactr echlgy (SMiR 18) Beijig, Chia, August 7-12, 25 SMiR18-F7-4 APPLICAION OF FEM ANALYSIS MEHODS O A CYLINDER-CYLINDER INERSECION SRUCURE Lipig XUE G.E.O.
More informationThe Molecular Diffusion of Heat and Mass from Two Spheres
Iteratial Jural f Mder Studies i Mechaical Egieerig (IJMSME) Vlume 4, Issue 1, 018, PP 4-8 ISSN 454-9711 (Olie) DOI: http://dx.di.rg/10.0431/454-9711.0401004 www.arcjurals.rg The Mlecular Diffusi f Heat
More informationu = A Z Chemistry 110 Fall 2010 Rayleigh-Jeans Law for Blackbody SI Units SI Units Secondary Units written in terms of Primary
SI Uits Key Study Pits fr Petrucci et al., Secdary Uits writte i terms f Primary Capters 8 & 9 Nte: Fudametal cstats ad a peridic table will be prvided te midterm but equatis will t be give. Cemistry 0
More informationFourier Series & Fourier Transforms
Experimet 1 Furier Series & Furier Trasfrms MATLAB Simulati Objectives Furier aalysis plays a imprtat rle i cmmuicati thery. The mai bjectives f this experimet are: 1) T gai a gd uderstadig ad practice
More informationDirectional Duality Theory
Suther Illiis Uiversity Carbdale OpeSIUC Discussi Papers Departmet f Ecmics 2004 Directial Duality Thery Daiel Primt Suther Illiis Uiversity Carbdale Rlf Fare Oreg State Uiversity Fllw this ad additial
More information2. Before we answer the question, here are four important terms relating to redox reactions and galvanic cells.
CHAPTER SEVENTEEN ELECTROCHEMISTRY Fr Review 1. Electrchemistry is the study f the iterchage f chemical ad electrical eergy. A redx (xidati-reducti) reacti is a reacti i which e r mre electrs are trasferred.
More informationElectrochemistry Redox Half-Reactions
Electrchemistry Electrchemistry deals with the relatiship betwee chemical chage ad electricity Electrchemical s (tw types) Galvaic s use a sptaeus ( G < 0) reacti t prduce electricity (batteries) Electrlytic
More informationDEPARTMENT OF ELECTRICAL ENGINEERING DIT UNIVERSITY HIGH VOLTAGE ENGINEERING
DEPARTMENT F ELECTRICAL ENGINEERING HIGH VLTAGE ENGINEERING UNIT 1: BREAKDWN IN GASES 1.) Itrducti: I mder times, high vltages are used fr a wide variety f applicatis cverig the pwer systems, idustry ad
More informationWEST VIRGINIA UNIVERSITY
WEST VIRGINIA UNIVERSITY PLASMA PHYSICS GROUP INTERNAL REPORT PL - 045 Mea Optical epth ad Optical Escape Factr fr Helium Trasitis i Helic Plasmas R.F. Bivi Nvember 000 Revised March 00 TABLE OF CONTENT.0
More informationESWW-2. Israeli semi-underground great plastic scintillation multidirectional muon telescope (ISRAMUTE) for space weather monitoring and forecasting
ESWW-2 Israeli semi-udergrud great plastic scitillati multidirectial mu telescpe (ISRAMUTE) fr space weather mitrig ad frecastig L.I. Drma a,b, L.A. Pustil'ik a, A. Sterlieb a, I.G. Zukerma a (a) Israel
More informationRMO Sample Paper 1 Solutions :
RMO Sample Paper Slutis :. The umber f arragemets withut ay restricti = 9! 3!3!3! The umber f arragemets with ly e set f the csecutive 3 letters = The umber f arragemets with ly tw sets f the csecutive
More informationElectrostatics. . where,.(1.1) Maxwell Eqn. Total Charge. Two point charges r 12 distance apart in space
Maxwell Eq. E ρ Electrstatics e. where,.(.) first term is the permittivity i vacuum 8.854x0 C /Nm secd term is electrical field stregth, frce/charge, v/m r N/C third term is the charge desity, C/m 3 E
More informationOn the affine nonlinearity in circuit theory
O the affie liearity i circuit thery Emauel Gluski The Kieret Cllege the Sea f Galilee; ad Ort Braude Cllege (Carmiel), Israel. gluski@ee.bgu.ac.il; http://www.ee.bgu.ac.il/~gluski/ E. Gluski, O the affie
More informationClaude Elysée Lobry Université de Nice, Faculté des Sciences, parc Valrose, NICE, France.
CHAOS AND CELLULAR AUTOMATA Claude Elysée Lbry Uiversité de Nice, Faculté des Scieces, parc Valrse, 06000 NICE, Frace. Keywrds: Chas, bifurcati, cellularautmata, cmputersimulatis, dyamical system, ifectius
More informationControl Systems. Controllability and Observability (Chapter 6)
6.53 trl Systems trllaility ad Oservaility (hapter 6) Geeral Framewrk i State-Spae pprah Give a LTI system: x x u; y x (*) The system might e ustale r des t meet the required perfrmae spe. Hw a we imprve
More informationHº = -690 kj/mol for ionization of n-propylene Hº = -757 kj/mol for ionization of isopropylene
Prblem 56. (a) (b) re egative º values are a idicati f mre stable secies. The º is mst egative fr the i-ryl ad -butyl is, bth f which ctai a alkyl substituet bded t the iized carb. Thus it aears that catis
More informationCharacteristics of helical flow in slim holes and calculation of hydraulics for ultra-deep wells
6 Pet.Sci.(00)7:6-3 DOI 0.007/s8-00-006-8 Characteristics f helical flw i slim hles ad calculati f hydraulics fr ultra-deep wells Fu Jiahg, Yag Yu, Che Pig ad Zha Jihai 3 State Key Labratry f Oil ad Gas
More informationSEQUENCES AND SERIES
9 SEQUENCES AND SERIES INTRODUCTION Sequeces have may importat applicatios i several spheres of huma activities Whe a collectio of objects is arraged i a defiite order such that it has a idetified first
More informationALL INDIA TEST SERIES
AIT-FT-V-(Paper-) PM(l)-JEE(Advaced)/5 FIITJEE tudets Frm All Prgrams have agged 3 i Tp, 66 i Tp ad 7 i Tp 5 All Idia Raks. FIITJEE Perfrmace i JEE (Advaced), : 5 FIITJEE tudets frm assrm / Itegrated chl
More informationCold mirror based on High-Low-High refractive index dielectric materials
Cld mirrr based High-Lw-High refractive idex dielectric materials V.V. Elyuti.A. Butt S.N. Khia Samara Natial Research Uiversity 34 skvske Shsse 443086 Samara Russia Image Prcessig Systems Istitute Brach
More information8.0 Negative Bias Temperature Instability (NBTI)
EE650R: Reliability Physics f Naelectric Devices Lecture 8: Negative Bias Temerature Istability Date: Se 27 2006 Class Ntes: Vijay Rawat Reviewed by: Saakshi Gagwal 8.0 Negative Bias Temerature Istability
More informationChapter 1: Fundamentals
Chapter 1: Fudametals 1.1 Real Numbers Irratial umbers are real umbers that cat be expressed as ratis f itegers. That such umbers exist was a prfud embarrassmet t the Pythagrea brtherhd, ad they are said
More informationBC Calculus Review Sheet. converges. Use the integral: L 1
BC Clculus Review Sheet Whe yu see the wrds.. Fid the re f the uuded regi represeted y the itegrl (smetimes f ( ) clled hriztl imprper itegrl).. Fid the re f differet uuded regi uder f() frm (,], where
More informationThe indicative surfaces of the photoelastic effect in Cs 2 HgCl 4 biaxial crystals
Optical Materials xxx (2006) xxx xxx www.elsevier.cm/lcate/ptmat The idicative surfaces f the phtelastic effect i Cs 2 HgCl 4 biaxial crystals M.V. Kaida a, B.V. Tybika a, A.V. Zadrzha b, A.S. Adrushchak
More informationThermodynamics Partial Outline of Topics
Thermdynamics Partial Outline f Tpics I. The secnd law f thermdynamics addresses the issue f spntaneity and invlves a functin called entrpy (S): If a prcess is spntaneus, then Suniverse > 0 (2 nd Law!)
More informationFAILURE CRITERIA: MOHR S CIRCLE AND PRINCIPAL STRESSES
LECTURE Third Editio FAILURE CRITERIA: MOHR S CIRCLE AND PRINCIPAL STRESSES A. J. Clark School of Egieerig Departmet of Civil ad Evirometal Egieerig Chapter 7.4 b Dr. Ibrahim A. Assakkaf SPRING 3 ENES
More informationMean residual life of coherent systems consisting of multiple types of dependent components
Mea residual life f cheret systems csistig f multiple types f depedet cmpets Serka Eryilmaz, Frak P.A. Cle y ad Tahai Cle-Maturi z February 20, 208 Abstract Mea residual life is a useful dyamic characteristic
More informationRates and Mechanisms of Chemical Reactions
Rates ad Mechaisms f Chemical Reactis Why sme rxs prceed very fast ad thers require days, mths r eve years t prduce a detectable amt f prduct? H (g) + F (g) HF (g) (very fast) 3 H (g) + N (g) NH 3 (g)
More informationSolutions to Midterm II. of the following equation consistent with the boundary condition stated u. y u x y
Sltis t Midterm II Prblem : (pts) Fid the mst geeral slti ( f the fllwig eqati csistet with the bdary cditi stated y 3 y the lie y () Slti : Sice the system () is liear the slti is give as a sperpsiti
More informationWe will conclude the chapter with the study a few methods and techniques which are useful
Chapter : Coordiate geometry: I this chapter we will lear about the mai priciples of graphig i a dimesioal (D) Cartesia system of coordiates. We will focus o drawig lies ad the characteristics of the graphs
More informationSTRUCTURES IN MIKE 21. Flow over sluice gates A-1
A-1 STRUCTURES IN MIKE 1 Fl ver luice gate Fr a give gemetry f the luice gate ad k ater level uptream ad dtream f the tructure, the fl rate, ca be determied thrugh the equati f eergy ad mmetum - ee B Pedere,
More informationK [f(t)] 2 [ (st) /2 K A GENERALIZED MEIJER TRANSFORMATION. Ku(z) ()x) t -)-I e. K(z) r( + ) () (t 2 I) -1/2 e -zt dt, G. L. N. RAO L.
Iterat. J. Math. & Math. Scl. Vl. 8 N. 2 (1985) 359-365 359 A GENERALIZED MEIJER TRANSFORMATION G. L. N. RAO Departmet f Mathematics Jamshedpur C-perative Cllege f the Rachi Uiversity Jamshedpur, Idia
More informationThermodynamic study of CdCl 2 in 2-propanol (5 mass %) + water mixture using potentiometry
Thermdyamic study f CdCl 2 i 2-prpal (5 mass %) + water mixture usig ptetimetry Reat Tmaš, Ađelka Vrdljak UDC: 544.632.4 Uiversity f Split, Faculty f Chemistry ad Techlgy, Teslia 10/V, HR-21000 Split,
More informationAnalysis of pressure wave dynamics in fuel rail system
It. Jl. f Multiphysics Vlume Number 3 8 3 Aalysis f pressure wave dyamics i fuel rail system Basem Alzahabi ad Keith Schulz Ketterig Uiversity Siemes Autmtive ABSTRACT A mdel f a amplified cmm rail fuel
More informationFive Whys How To Do It Better
Five Whys Definitin. As explained in the previus article, we define rt cause as simply the uncvering f hw the current prblem came int being. Fr a simple causal chain, it is the entire chain. Fr a cmplex
More informationSEQUENCE AND SERIES NCERT
9. Overview By a sequece, we mea a arragemet of umbers i a defiite order accordig to some rule. We deote the terms of a sequece by a, a,..., etc., the subscript deotes the positio of the term. I view of
More informationOPTICAL SWITCH USING TOTAL REFLECTION IN LIQUID CRYSTALS
7 th teratial Cferece DEVELOPMENT AND APPLCATON SYSTEMS S u c e a v a, m a i a, M a 7 9, 0 0 4 OPTCAL SWTCH USNG TOTAL EFLECTON N LQUD CYSTALS Serge DOVGALETS 1, Yulia SEMENOVA, Vasl PYSYAZHNYUK 1 1) Departmet
More informationThe generalized marginal rate of substitution
Jural f Mathematical Ecmics 31 1999 553 560 The geeralized margial rate f substituti M Besada, C Vazuez ) Facultade de Ecmicas, UiÕersidade de Vig, Aptd 874, 3600 Vig, Spai Received 31 May 1995; accepted
More informationTHE LIFE OF AN OBJECT IT SYSTEMS
THE LIFE OF AN OBJECT IT SYSTEMS Persns, bjects, r cncepts frm the real wrld, which we mdel as bjects in the IT system, have "lives". Actually, they have tw lives; the riginal in the real wrld has a life,
More informationMotor Stability. Plateau and Mesa Burning
Mtr Stability Recall mass cservati fr steady erati ( =cstat) m eit m b b r b s r m icr m eit Is this cditi (it) stable? ly if rmally use.3
More informationDistributed Trajectory Generation for Cooperative Multi-Arm Robots via Virtual Force Interactions
862 IEEE TRANSACTIONS ON SYSTEMS, MAN, AND CYBERNETICS PART B: CYBERNETICS, VOL. 27, NO. 5, OCTOBER 1997 Distributed Trajectry Geerati fr Cperative Multi-Arm Rbts via Virtual Frce Iteractis Tshi Tsuji,
More informationPipe Networks - Hardy Cross Method Page 1. Pipe Networks
Pie Netwrks - Hardy Crss etd Page Pie Netwrks Itrducti A ie etwrk is a itercected set f ies likig e r mre surces t e r mre demad (delivery) its, ad ca ivlve ay umber f ies i series, bracig ies, ad arallel
More informationTypes of Gear Pg xxx. Spur Gear Teeth is parallel to axis of rotation Can transmit power between parallel shaft The simplest form for gear
[Pg / 2] Gears Objectives. 2. 3. 4. 5. Cmpute the frces exerted n gear teeth as they rtate and transmit pwer. Use apprpriate stress analyses t determine the relatinships amng the applied frces, the gemetry
More informationThermodynamics and Equilibrium
Thermdynamics and Equilibrium Thermdynamics Thermdynamics is the study f the relatinship between heat and ther frms f energy in a chemical r physical prcess. We intrduced the thermdynamic prperty f enthalpy,
More informationChemistry 20 Lesson 11 Electronegativity, Polarity and Shapes
Chemistry 20 Lessn 11 Electrnegativity, Plarity and Shapes In ur previus wrk we learned why atms frm cvalent bnds and hw t draw the resulting rganizatin f atms. In this lessn we will learn (a) hw the cmbinatin
More informationInternal vs. external validity. External validity. Internal validity
Secti 7 Mdel Assessmet Iteral vs. exteral validity Iteral validity refers t whether the aalysis is valid fr the pplati ad sample beig stdied. Exteral validity refers t whether these reslts ca be geeralized
More informationSuper-efficiency Models, Part II
Super-efficiec Mdels, Part II Emilia Niskae The 4th f Nvember S steemiaalsi Ctets. Etesis t Variable Returs-t-Scale (0.4) S steemiaalsi Radial Super-efficiec Case Prblems with Radial Super-efficiec Case
More informationCENTRIFUGAL PUMP SPECIFIC SPEED PRIMER AND THE AFFINITY LAWS Jacques Chaurette p. eng., Fluide Design Inc. November 2004
CENTRIFUGAL PUMP SPECIFIC SPEE PRIMER AN THE AFFINITY LAWS Jacques Chaurette p. eg., Fluide esig Ic. November 004 www.fluidedesig.com There is a umber called the specific speed of a pump whose value tells
More informationGeneral Chemistry 1 (CHEM1141) Shawnee State University Fall 2016
Geeral Chemistry 1 (CHEM1141) Shawee State Uiversity Fall 2016 September 23, 2016 Name E x a m # I C Please write yur full ame, ad the exam versi (IC) that yu have the scatr sheet! Please 0 check the bx
More informationNOT FOR A400. Urbia 103 DUNDAS CORPORATION 103 DUNDAS STREET W OAKVILLE, ONTARIO NORTH ELEVATIONS LEGEND NORTH ELEVATION 1 : 125
TES: ALL GUDS T MEET REQUIREMETS F THE BC 202 MAUFACTURER/SUPPLIER T PRVIDE EGIEERED, STAMPED SHP DRIGS CMPLETE WITH MUTIG DETAILS GUDS SHALL CMPLY WITH BC 337, 3465 AD 40 GUDS SHALL CMPLY WITH BC 436
More informationPlan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations
STAPLE Physics 201 Name Final Exam May 14, 2013 This is a clsed bk examinatin but during the exam yu may refer t a 5 x7 nte card with wrds f wisdm yu have written n it. There is extra scratch paper available.
More informationMASSIVELY PARALLEL SEQUENCING OF POOLED DNA SAMPLES-THE NEXT GENERATION OF MOLECULAR MARKERS
Geetics: Published Articles Ahead f Prit, published May 10, 2010 as 10.1534/geetics.110.114397 MASSIVELY PARALLEL SEQUENCING OF POOLED DNA SAMPLES-THE NEXT GENERATION OF MOLECULAR MARKERS Authrs ad affiliatis
More informationDifference of 2 kj per mole of propane! E = kj
Ethaly, H Fr rcesses measured uder cstat ressure cditi, the heat the reacti is q. E = q + w = q P ext V he subscrit remids is that the heat measured is uder cstat ressure cditi. hermdyamics Slve r q q
More informationPart One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review)
CHAPTER 18: THERMODYNAMICS AND EQUILIBRIUM Part One: Heat Changes and Thermchemistry This aspect f Thermdynamics was dealt with in Chapter 6. (Review) A. Statement f First Law. (Sectin 18.1) 1. U ttal
More informationLecture 18. MSMPR Crystallization Model
ecture 18. MSMPR Crystalliati Mdel MSMPR Crystalliati Mdel Crystal-Ppulati alace - Number f crystals - Cumulative umber f crystals - Predmiat crystal sie - Grwth rate MSMPR Crystalliati Mdel Mixed-suspesi,
More informationExperimental and Theoretical Investigations of PAN Molecular Weight Increase in Precipitation Polymerization as a Function of H 2 O/DMSO Ratio
Carb Letters Vl., N. March 00 pp. -7 Experimetal ad Theretical Ivestigatis f PAN Mlecular Weight Icrease i Precipitati Plymerizati as a ucti f H O/DMSO Rati Jig Zhag, egjig Bu, Ygqiag Dai, Liwei Xue, Zhixia
More information