For official use only Doc. WRD 09(489) July 2007 BUREAU OF INDIAN STANDARDS. PRELIMINARY Indian Standard

Size: px
Start display at page:

Download "For official use only Doc. WRD 09(489) July 2007 BUREAU OF INDIAN STANDARDS. PRELIMINARY Indian Standard"

Transcription

1 For official us only Doc. WRD 09(489) July 007 BUREAU OF INDIAN STANDARDS PRELIMINARY Indian Standard STRUCTURAL DESIGN OF ENERGY DISSIPATORS FOR SPILLWAYS CRITERIA (First Rvision) (Not to b rproducd without th Last dat for rcipt prmission of BIS or usd as a of commnts is STANDARD) FOREWORD (Formal claus to b addd latr on) Th dsign of downstram protction works or nrgy dissipators blow hydraulic structurs occupis a vital plac in th dsign and construction of dams, wirs barrags and outlts. Th problm of dsigning nrgy dissipators is ssntially of rducing high vlocity flow to a vlocity low nough to minimiz rosion of natural rivr bd. This rduction in vlocity may b accomplishd by any, or a combination of th following, dpnding upon th had, discharg intnsity, tail watr conditions and th typ of bd rock or th bd matrial: a) Hydraulic jump typ stilling basins: 1) Horizontal apron typ; and ) Sloping apron typ; b) Jt diffusion and fr jt stilling basins: 1) Jt diffusion basins; ) Fr jt stilling basins; 3) Hump stilling basins; and 4) Impact stilling basins; c) Buckt typ dissipators: 1) Solid and slottd rollr buckts; and ) Trajctory buckts (ski jump, flip, tc); 1

2 d) Intracting jts and othr spcial typ of stilling basins. In India, hydraulic jump typ stilling basins and buckt typ nrgy dissipators ar gnrally usd for dissipation of nrgy dpnding on condition of downstram tail watr. Indian Standards had alrady bn publishd for critria for hydraulic dsign of ths two typs of nrgy dissipators as undr: IS 4997 : 1968 Critria for dsign of hydraulic jump typ stilling basins which with horizontal and sloping apron IS 7365 : 1985 Critria for hydraulic dsign of buckt typ nrgy dissipators (first rvision) This standard covring th structural dsign of nrgy dissipators for spillways was first publishd in This rvision incorporats th latst practics bing followd in th fild, th major changs bing in rspct of dsign of flow slab anchorags, anchorag for spillway buckt and dsign of rinforcmnt for buckt tth. For th purpos of dciding whthr a particular rquirmnt of this standard is complid with th final valu, obsrvd or calculatd xprssing th rsult of tst or analysis shall b roundd off in accordanc with IS : Ruls for rounding off numrical valus (rvisd). Th numbr of significant placs rtaind in th roundd off valu should b th sam as that of th spcifid valus in this standards. 1 SCOPE This standard lays down critria for structural dsign of various componnts of hydraulic jump typ stilling basins and buckt typ nrgy dissipators blow spillways and outlt works foundd on rock. REFERENCES Th standards listd blow contain provisions which, through rfrnc in this txt, constitut provisions of this standard. At th tim of publication, th ditions indicatd wr valid. All standards ar subjct to rvision and partis to agrmnts basd on ths standards ar ncouragd to invstigat th possibility of applying th most rcnt ditions of th standards indicatd blow: IS No. Titl 1786 : 1985 Spcification for high strngth dformd stl bars and wirs for concrt rinforcmnt (Third rvision) (Suprsding IS 1139) 4410 (Pt 18) : 1983 Glossary of trms rlating to rivr vally projcts: Part 18 Enrgy dissipator dvics (Stilling basins) 4997 : 1968 Critria for dsign of hydraulic jump typ stilling basins with horizontal and sloping apron : 1994 Critria for dsign of chut and sid channl spillways (First rvision) 7365 : 1985 Critria for hydraulic dsign of buckt typ nrgy dissipators (First rvision) : 1994 Cod of practic Construction of spillways and similar ovrflow structurs (First rvision)

3 1177 : 1986 Guidlins for dsign of drainag arrangmnts of nrgy dissipators and training walls of spillways 3 TERMINOLOGY For th purpos of this standard, th dfinitions givn in IS 4410 (Part 18), IS 4997 and IS 7365 shall apply. 4 STRUCTURAL DESIGN OF STILLING BASIN FLOOR 4.1 Gnral Th basin floor lvation is gnrally dcidd on th basis of foundation conditions and th lngth of th basin is dcidd on th basis of hydraulic considrations in accordanc with IS Th width dpnds on th numbr of opnings and pirs on spillway crst. 4. Structural Dsign Th basin floor slab is subjctd to uplift, pounding and vibrations from hydrodynamic forcs in th hydraulic jump. On yilding foundation it may suffr diffrntial sttlmnt. Thrfor, th basin floor slab shall b dsignd for th strsss inducd du to abov forcs. Th important lmnts of th structural dsign of basin floor is dtrmination of thicknss of th floor and dtails of anchorags in th bd rock. Uplift forc is jointly rsistd by th slf wight of floor and contribution from th anchorags. For calculations of uplift, a thicknss of th floor is assumd initially, and is confirmd by dtaild calculations Minimum thicknss Th minimum thicknss of th floor slab dpnds on th foundation conditions and th magnitud of uplift forcs. A slab of about 600 mm thicknss is th minimum rcommndd. Actual slab thicknss shall b dtrmind by analysing uplift and diffrntial movmnt. 4.3 DESIGN PROCEDURE Th structural dsign of floor slab consists of th following stps: a) dtrmination of uplift forc b) dtails of anchorags into bd rock i.. diamtr, numbr and spacing of anchor bars. c) dtrmination of lngth of anchors considring dislodgmnt of rock mass against uplift forc, and d) working out dtails of slab rinforcmnt Uplift forc Uplift of th concrt lining of th stilling basin could b causd du to on or a combination of th following: 3

4 a) Hydrostatic uplift Th uplift causd by spag gradint blow th stilling basin. b) Hydrodynamic uplift Th propagation of fluctuating prssurs in th hydraulic jump through unsald joints or cracks in th floor such that man prssur prvails at th intrfac of th concrt and bd rock and hnc hydrodynamic uplift is causd whnvr instantanous prssur on th uppr surfac is lss than man valu of th fluctuating prssur Hydrostatic uplift Provision of ffctiv drainag systm blow th basin is ncssary. (s IS : 1177). In viw of th drainag arrangmnt providd blow th basin, it may b adquat to assum 50% rlif in th uplift prssurs, as indicatd blow. Following thr conditions may prvail and th most critical of thm should b dtrmind. Condition I Stilling basin oprating during spillway dsign flood is shown in figur. Th watr surfac ovr th slab at hydraulic jump profil for dsign discharg conditions. Unbalancd uplift prssur = 0.5 (Tw 1 W + t b W) (D 1 W + t b Wc) Tw 1 = Maximum tail watr dpth W = unit wight of watr t b = thicknss of stilling basin floor Wc = unit wight of concrt D 1 = Dpth of watr in stilling basin Condition II Rsrvoir at FRL with gats closd and stilling basin mpty i.. dwatrd (Fig. 3). Unbalancd uplift prssur = 0.5 (Tw 1 W + t b W) (t b Wc) Tw 1 = Minimum tail watr dpth Condition III Suddn drawdown condition aftr th dsign flood has just passd ovr th spillway and th gats ar closd again. In this cas th uplift blow th basin may b takn th sam as th condition I and th watr load in th basin b takn as th minimum TWL which may b th dpst rivr bd lvl, minimum watr lvl in th rivr from powr/othr considrations, tc. (Fig. 4). Unbalancd uplift prssur u = 0.5 (T W W + tb W) (Tw W + tb Wc) Hydrodynamic uplift Th hydrodynamic uplift prssur F m ovr th slab monolith according to claus is givn by 4

5 1. ρ. V F' m = Kφ p. φ1. φ ( 1 ) Whr K = factor accounting for th probability of occurrnc of fluctuating prssurs. = 3.09 corrsponding to 99.8% probability of occurrnc. φ p = Prssur cofficint givn in Fig. 5. ρ = Mass dnsity of watr, 1000 kg/cum V 1 = Vlocity of flow ntring th stilling basin L 1 = Lngth of th monolith in flow dirction L = Width of th monolith prpndicular to flow dirction. φ 1 = Cofficint of corrlation of prssur along L 1 (From Fig. 5) φ = Cofficint of corrlation of prssur along L (From Fig. 5) Th valus of prssur cofficint for various Fraud numbrs shall b rad out from Fig. 5. Th largst of th abov valus of uplift prssur shall b considrd for dsign purpos Dsign of anchors Gnrally th diamtr of th anchor bar should atlast b 5 mm. Th diamtr of th whol into which th anchors ar placd and groutd should not b lss than 1.5 tims th diamtr of th anchor bar. Th othr dtails shall b workd out as shown blow: Numbr of anchors (n) rquird pr unit ara is givn by Unbalancd uplift prssur n = a σ st Whr, a = ara of th bar σ st = Prmissibl tnsil strss of stl, kn/m Numbr of bars to b roundd to th nxt highr intgr Spacing of bars = 1 n Actual forc in ach anchor = Unbalancd uplift prssur = n µ No. of anchors rquird pr unit ara Th dpth of anchor bars in rock mass = whr d b = dia. of anchor bar Actual forc in ach anchor Actual forc in ach anchor OR π d F π d F b b1 a b 5

6 d a = dia. of anchor hol F = Prmissibl bond strss btwn stl and grout b 1 F b = Prmissibl bond strss btwn grout and rock Th gratr of th two should b adoptd as anchor dpth. Th valu of th prmissibl bond strss would vary for diffrnt sit conditions and proportion of grouts. In th absnc of data, th following valus for 1: ratio proportion of grout may b adoptd. F b 1 = 600 kn/m F b = 400 kn/m Bond lngth should b chckd for bond btwn stl and grout and also for bond btwn rock and grout Chck for dislodging of rock mass anchord against uplift prssur. Th dpth of anchor bar in th rock mass calculatd in 4.3. should b chckd for dislodgmnt of rock mass against uplift prssur. For this, th dpth of anchor bar in th rock mass should b sufficint to ngag a conical mass of rock with a vrtx angl of 45 dgrs, th wight of which should b abl to withstand th nt upward forc (S Fig. 6). Th dpth of anchor rquird from th abov considrations shall b chckd as follows: (1) Dpth of conical mass of rock at bottom, h 1 (Spacing of anchor bar)/ = mtrs tan.5º () Wight of conical mass at bottom W π h1 = ( h1 tan.5º ) Wrs.. kn 4 3 whr h 1 = dpth of anchor bar in conical portion (Fig. 6) Wrs = Submrgd wight of rock, kn (3) Dpth h rquird xcluding conical mass [ Actual forc on ach anchor Slf wight of slab covrd by ach anchor Wight of conical mass] h = (Spacing) Submrgd wight of rock. NOTE If th govrning uplift considrd is hydrostatic (i.. conditions (1) to (3), thn th trm rprsnting slf wight of slab should b omittd from th abov quation. (4) Total dpth of anchor L = h 1 + h Th abov procdur assums that no tnsion is prmissibl in th foundation rock. Howvr, in sound and hard rock som tnsion is allowd to rduc th dpth of anchor. 6

7 It should also b nsurd that th dpth of anchor bar as calculatd in 4.3. is not lss than th valu of L calculatd using th abov quations. Not withstanding th rsults of abov calculations, a minimum 3 m lngth of anchor should b providd. Th calculations should b rfind to obtain a satisfactory combination of th valus of slab thicknss and anchor bars, consistnt with th charactristics of th bd rock Annx A givs an xampl to illustrat th mthods of calculation. 4.4 BASIN FLOOR SLAB Floor Slab Thicknss Th thicknss of floor slab dpnds on th foundation conditions and magnitud of uplift forcs. A slab of about 600 mm thicknss is th minimum rcommndd. Actual slab thicknss ndd shall b dtrmind by analysing hydrostatic uplift and diffrntial foundation movmnt Floor Slab Rinforcmnt In thick slabs on rock foundations normally covrd with nominal tail watr, structural rinforcmnt is not ncssary xcpt in th appurtnancs of th stilling basin. Uplift on a slab should b takn car of by adquat anchors. Th slab is dividd into indpndnt panls by contraction joints paralll and prpndicular to channl or basin cntr lin to avoid srious shrinkag and tmpratur cracking with th us of nominal rinforcmnt which dos not xtnd across th joints. Siz of panl should b larg nough to rsist distorting hydrodynamic forcs. Panls should b cast in altrnat bays with construction joints Th indpndnt panls of slab ar rinforcd with nominal stl to prvnt harmful cracking rsulting from shrinkag and tmpratur strsss not rlivd by contraction joint and on yilding foundations to avoid possibl cracking from diffrntial sttlmnt. Usually, a slab on unyilding foundation is rinforcd in th top fac only bcaus bond btwn th concrt and rock at th bottom is rlid on to distribut shrinkag cracks and to minimiz bnding strsss in th anchord slab for th assumd uplift had. Th minimum amount of rinforcmnt for indpndnt panls on unyilding rocks is 0 mm diamtr bars at 300 mm cntr-to-cntr both ways. Additional rinforcmnt should b providd for unfavourabl foundation condition or for high hydrostatic uplift prssur Diffrntial Movmnt On rlativly yilding rock foundations, th indpndnt floor panls ar subjct to possibl diffrntial movmnt of adjacnt blocks and a ky at ach transvrs contraction joint (xtnding into foundation undr th joint attachd to th slab downstram and supporting th slab upstram from th joint) may b rquird to prvnt th downstram sid of a joint from bing raisd abov th upstram sid as watr at high vlocity striking such a projction would incras th hydrostatic prssur in th joint and hnc th uplift undr th slab. Highr th vlocity, mor srious will b th condition rsulting from such rlativ movmnt. Th kys also incras rsistanc to possibl movmnt and srv as spag cutoffs downstram from transvrs drains. Dtails of ky ar covrd in IS

8 4.4.4 Concrt and Rinforcmnt Covr Chut floor and stilling basin slab shall hav minimum 100 mm covr for rinforcmnt. 4.5 BASIN BLOCKS (STRUCTURAL PROVISION) Gnral Location and optimum shap of basin blocks shall b dcidd on th basis of IS Th dimnsions of th basin blocks ar shown in Fig. 6a. Th purpos of th block is to dissipat nrgy and thrby to rduc th lngth of basin. h b = hight of basin block S b = spacing btwn th blocks W b = width of block, and D = conjugat dpth 4.5. Forcs on Basin Blocks Dynamic forc against th upstram fac of th basin blocks is approximatly that of a Jt impinging upon a plan normal to th dirction of flow. (s fig. 6b) Forc P acting at h b / = WA (D 1 + h v1 ) whr W = unit wight of watr A = ara of upstram fac of block, and h b = Hight of basin block (D 1 + h v1 ) = spcific nrgy of th flow ntring th basin Ngativ prssur on th back fac of th blocks will furthr incras th total load. Howvr, this may b nglctd if abov quation is usd. Basin block is to b dsignd as cantilvr as shown in Fig. 6a Rinforcmnt Th rinforcmnt shall b calculatd by th following formula and placmnt of th rinforcmnt is shown in Fig. 7. Ara of stl A st M = σ st jd whr M = momnt du to forc P (s 4.5.) σ st h b = P = prmissibl tnsil strss of stl, and 8

9 d = ffctiv dpth of block. NOTE 1 Th basin block is tid into th floor slab by rinforcing stl. All rinforcing stl in a basin block is placd minimum 150 mm from th xposd surfac bcaus of th possibl rosiv and cavitation action of th high vlocity currnts. 4.6 CHUTE BLOCKS Nominal rinforcmnt of 0 mm diamtr bar at 300 mm cntr to cntr both ways may b providd on all xposd facs duly anchord in apron concrt. 5 SPILLWAY BUCKET REINFORCEMENT 5.1 Trajctory/Solid Rollr Buckt (s Fig. 8 and 9) Forcs and Momnts Horizontal forc on th buckt is du to chang in momntum and is givn by th following formula: wqv g Total horizontal forc on th lip (F) = (1 cos θ ) w = Unit wight of watr. q = Discharg intnsity. v = Vlocity of flow. θ = Exit angl of th buckt. Momnt of th horizontal forc about horizontal plan A-A passing through invrt of th buckt (s Fig. 8) is givn by F R (1 cos θ ) M = R = Radius of buckt Effctiv dpth d of buckt for rsisting momnt M may b takn as d = + R ( R sin Q + t ) R ffctiv covr. w 5. REINFORCEMENT Ara of th stl A st of rsist momnt M is givn by M A st = σ st jd Providd minimum stl (along flow) = 0 mm diamtr bar at 300 mm cntr to cntr. 9

10 Provid distribution stl = 0 prcnt of main stl with a minimum of 16 mm diamtr bar at 300 mm cntr to cntr. 5.3 ANCHORAGE OF SPILLWAY BUCKET (s fig. 10) Th following thr conditions may prvail: Condition 1 Spillway oprating condition at dsign flood, Condition Rsrvoir at FRL with gats closd and th buckt mpty (dwatrd) and Condition 3 Suddn drawdown condition Gnrally th dsign is carrid out considring uplift blow th buckt corrsponding to maximum TWL (condition 1 and 3) ignoring th wight of watr in th buckt and lip portion of th buckt on consrvativ sid. Th mthodology gnrally adoptd is givn in Howvr, th wight of watr in th buckt may b suitably considrd in dsign whn it is likly to hav a substantial ffct Provision of ffctiv drainag systm blow th buckt is ssntial (s IS 1177). In viw of th drainag arrangmnts blow th buckt, it may b adquat to assum 50 prcnt rlif in uplift prssurs Upward forc pr unit ara F u (S Fig. 10) is givn by th formula: F u = R ([0.5 βw W α W (1 0.5 (sin θ + sin θ ) + 0.5( θ + θ ]) i i (sin θ + sin θ ) i θ i = inlt angl of buckt Numbr of anchors pr unit ara = n = Fu a σ st 1 and spacing of anchors = n Anchors ar gnrally staggrd in plan Dpth of Anchors in Rock Mass Th dpth of anchors should b dtrmind by considring failur btwn anchor bar and grout and also btwn grout and rock as givn in claus SLOTTED ROLLER BUCKET (STRUCTURAL PROVISION) 6.1 Gnral Dimnsions of th slottd rollr buckt should b workd out on th basis of IS For anchor dsign 5.3 will b applicabl. Provision of ffctiv drainag systm blow th buckt is ssntial as givn in IS Som salint dimnsions to b usd in this standard ar: 10

11 b = 0.15 R b = 0.05 R L a = R sin (θ 8) R = R [sin (θ 8) ] b 1 = b + L a tan º b = b L a tan º 6.1. Discharg/mtr is calculatd by q= Q/L m 3 /s/m Whr Q= total dsign discharg at MWL in m 3 /s L = lngth of buckt spillway in m Vlocity is givn by th quation V = gh m/s Whr H = fall of watr (had) from MWL to buckt invrt. 6. Dsign of Rinforcmnt for Buckt Tth 6..1 Forc on buckt tth (Figur 1 shows dfinition sktch of buckt tth) abov plan AB and in a dirction paralll to it (s Fig. 11 and 1) is givn by Wqv [1 cos ( 8 )] b (Approximatly) g º F 1 = θ Th tth should b dsignd as a cantilvr fixd at th plan AB. F h 1 1 Bnding momnt, M = Whr h 1 is dfind in Fig. 1 and is givn as h 1 = R [1 cos ( θ 8º )] 6.. Ara of main stl A st is givn by A st = σ M stjd whr d = θ θ ( R Cos ) +( R Sin R) R ffctiv covr. Cos θ = [ Radius (Elvation of junction of 8º and 16º aprons invrt lvl )]/Radius(s fig 13) j = lvr arm factor and θ, θ and R ar indicatd in Fig

12 Th main rinforcmnt should b providd along th curv as shown in Fig. 13. Th minimum clar covr in th radial dirction should b 150 mm. It shall b nsurd that minimum rinforcmnt pr tooth is 7 numbrs 0 mm diamtr bar Dsign of Links for Tooth Provid 0 mm diamtr link rinforcmnt at 300 mm cntr to cntr around tooth in th dirction prpndicular to flow. Distribution stl for links shall b providd on thr sid facs of tooth and shall b 0 mm diamtr bar at 300 mm cntr to cntr. 6.3 Dsign of Rinforcmnt for 8º Apron Provid nominal rinforcmnt as undr: a) Along flow (main stl) = 0 mm diamtr at 300 mm cntr to cntr and b) Prpndicular to flow (distribution stl) = 16 mm diamtr at 300 mm cntr to cntr. 6.4 Dsign of Rinforcmnt for 16º Apron Horizontal forc on 16º apron. Whr wqv.. (cos 8º cos 16º ) g F = V = 1 b v b b 1 = width of slot at ntry b = width of slot at xit Rfrring to Fig 11 and Fig 1 lngth of 8º apron L a is givn as L a = RSin( θ 8º) b = 0.05 R b 1 = b + tan º R Th horizontal forc on apron is du to chang in dirction as abov and it acts lvl whr h = hight of 16º apron. Bnding momnt = F Ara of stl A st = h BM.. σ st jd whr d = ffctiv dpth for 16º apron = h cos 16º covr NOTE Minimum stl shall b providd as mntiond in 6.3 h abov apron 1

13 6.5 Sampl calculations for slottd rollr buckt ar givn in Annx B for guidanc. 13

14 ANNEX A (Claus 4.33) ILLUSTRATIVE EXAMPLE FOR DESIGN OF SLAB AND ANCHORAGE Givn: D 1 =.43 m ) V 1 = 46.1 m/s ) For th dsign discharg condition F 1 = 9.44 ) Tw = 31.5 ) TW 1 = 6 m corrsponding to min powr hous flow Siz of th slab monolith L 1 = 16 m, L = 14 m ρ = 1000 kg/m 3 (Mass dnsity of watr) W = 9.81 kn/m 3 (Spcific wight of watr) Wc =.56 kn/m 3 (Spcific wight of concrt) Wrs = kn/m 3 (Spcific wight of rock undr submrgd condition). Fb 1 = 600 kn/m Fb = 400 kn/m σ st = kn/m Stp 1: Calculat th maximum uplift prssur Assum slab thicknss t b = m Condition 1: Spillway dsign flood µ = 0.5 ( ) ( ) = Condition : Stilling basin mpty µ = 0.5 ( ) (.56) = = 5.88 Hnc thr no uplift Condition 3: Suddn drawdown following dsign flood 0.5 ( ) (6x ) = 59 kn/m Hydrodynamic uplift Ø p = 0.05 D = Tw = 31.5 mm D D 1 = = 8.8 for F 1 = 9.44 (Fig. 5) 14

15 Ø 1 = 0.76 for 1 L 16 = = (Fig. 5) D D Ø = 0.91 for L 14 = = (Fig. 5) D D Uplift prssur F m = (46.1) = kn/m Thrfor dsign uplift prssur = kn/m Stp : Dtrmin numbr of anchor bars/spacing Try 5 mm dia bars. Ara = m No. of anchor bars pr unit ara = = Say 1 bar pr squar mtr ara. Spacing at 1 mtr c/c Thrfor actual forc in ach anchor = kn. Stp 3 Dtrmin dpth of anchor bar basd on dia. of anchor bar L = π =.5 m basd on dia of hol in th rock L = ( = 40 mm) =.35 m π Stp 4 Chck against dislodgmnt of rock mass Dpth of conical rock mass at bottom (S fig. 6) h 1 = Wight of conical W 1/ 1.1 m = π 1.1 = ( ) = 4.37 kn Dpth rquird xcluding conical rockmass (.56) 4.37 = h = Thrfor, total dpth L = h 1 + h Say 5 m 15

16 = Say = 6. m Th dpth of anchorag will b 6. m Rsults: Siz of th slab monolith = 16 m 14 m Thicknss of concrt slab = m Dia. of anchor bar = 5 mm Spacing = 1 m c/c Dpth of anchorag = 6. m NOTE Any rfinmnt rquird can b don by rpating th calculations with modifid valus of slab thicknss and diamtr of anchor bar tc. 16

17 ANNEX B (Clauss 6.5) SAMPLE CALCULATIONS FOR SLOTTED ROLLER BUCKET B-1 DATA GIVEN 1) Exit angl = 45º ) Lngth of buckt = 37.0 m 3) Discharg at MWL = cumcs 4) Width of tooth of d/s nd = 1.15 m 5) Radius of buckt = 9.0 m 6) Invrt lvl of buckt = R.L m 7) Junction 8º and 16º apron = R.L m 8) MWL = R.L m Discharg q = = Say q = 6 cumcs/m according to 6.1. V = gh cumcs m = = m/s whr H = Fall of watr (had) from MWL to buckt invrt ( ) = m B- DESIGN OF REINFORCEMENT FOR BUCKET TOOTH Forc on tooth abov plan AB in a dirction paralll to it is givn by wqv g F 1 =... (1 cos ( θ 8º ) = [1 cos (45º 8º )] = KN Now, h 1 (s fig. 13) = R [1 cos (θ 8º)] = 9 [1 cos (45º 8º) = m h1 B.M. = F1 = b (s 6..1) 17

18 = KN. m Hr, cos θ (s fig. 13) = Radius ( Elvation of junction of 8º and 16º aprons invrt lvl) = 9 ( ) 9 = Effctiv dpth Radius d = θ + θ + ( R cos ) ( R sin 0.05 R) R ffctiv covr = 15 cm = 1.5 m Ara of stl rquird M A st = σ st jd (s 6..) Assuming σ st = 80% of KN/m for hydraulic structurs = KN/m A st = = cm 4 cm provid 0 mm diamtr 7 nos bars pr tooth (minimum rinforcmnt) Dsign of links Provids 0 mm diamtr link rinforcmnt at 300 mm c/c around tooth in th dirction prpndicular to flow. Distribution stl for links shall b providd on thr sid facs of tooth and shall b 0 mm diamtr bar at 300 mm c/c. B-3 DESIGN OF REINFORCEMENT FOR 8º APRON Provid nominal rinforcmnt as undr: a) 0 mm diamtr bar 300 mm c/c main stl along flow b) 16 mm diamtr bar at 300 mm c/c prpndicular to flow. B-4 DESIGN OF REINFORCEMENT FOR 16º APRON Horizontal forc on 16º apron wqv.. (cos 8º cos 16º ) g F = according to 6.4 b = 0.05 R = = 0.45 m L a = R sin (θ 8) R 18

19 = 9 sin 37º m = 0.86 m whr V = 1 bv = = m/s b f = KN h B.M. = F Whr h is ris of 16º apron = 1.3 m B.M. = = KN. m A st = BM.. σ st jd (s 6.4) Whr d = (h cos 16º covr) = ( ) = 1.15 m A st = = cm Minimum Stl providd a) Along flow = 0 mm diamtr bar at 300 mm c/c b) Prpndicular to flow = 16 mm diamtr bar at 300 mm cntr to cntr. 19

4.2 Design of Sections for Flexure

4.2 Design of Sections for Flexure 4. Dsign of Sctions for Flxur This sction covrs th following topics Prliminary Dsign Final Dsign for Typ 1 Mmbrs Spcial Cas Calculation of Momnt Dmand For simply supportd prstrssd bams, th maximum momnt

More information

Unfired pressure vessels- Part 3: Design

Unfired pressure vessels- Part 3: Design Unfird prssur vssls- Part 3: Dsign Analysis prformd by: Analysis prformd by: Analysis vrsion: According to procdur: Calculation cas: Unfird prssur vssls EDMS Rfrnc: EF EN 13445-3 V1 Introduction: This

More information

4.4 Design of Sections for Flexure (Part III)

4.4 Design of Sections for Flexure (Part III) 4.4 Dsign of Sctions for Flxur (Part ) This sction covrs th following topics. Choic of Sctions Dtrmination of Limiting Zon Post-tnsioning in Stags 4.4.1 Choic of Sctions Th typ of sction is slctd asd on

More information

Ultimate strength analysis & design of residential slabs on reactive soil

Ultimate strength analysis & design of residential slabs on reactive soil Ultimat strngth analysis & dsign of rsidntial slabs on ractiv soil This documnt prsnts an ovrviw of thory undrlying ultimat strngth analysis and dsign of stiffnd raft and waffl raft slabs, as commonly

More information

AS 5850 Finite Element Analysis

AS 5850 Finite Element Analysis AS 5850 Finit Elmnt Analysis Two-Dimnsional Linar Elasticity Instructor Prof. IIT Madras Equations of Plan Elasticity - 1 displacmnt fild strain- displacmnt rlations (infinitsimal strain) in matrix form

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

VSMN30 FINITA ELEMENTMETODEN - DUGGA

VSMN30 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 information

Module 7 Design of Springs. Version 2 ME, IIT Kharagpur

Module 7 Design of Springs. Version 2 ME, IIT Kharagpur Modul 7 Dsign of Springs Lsson Dsign of Hlical Springs for Variabl Load Instructional Objctivs: At th nd of this lsson, th studnts should b abl to undrstand: Natur of varying load on springs Modification

More information

ME311 Machine Design

ME311 Machine Design ME311 Machin Dsign Lctur 4: Strss Concntrations; Static Failur W Dornfld 8Sp017 Fairfild Univrsit School of Enginring Strss Concntration W saw that in a curvd bam, th strss was distortd from th uniform

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 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 information

INVESTIGATION ON APPLICABILITY OF SUBSTITUTE BEAM - COLUMN FRAME FOR DESIGN OF REINFORCED CONCRETE SWAY FRAMES

INVESTIGATION ON APPLICABILITY OF SUBSTITUTE BEAM - COLUMN FRAME FOR DESIGN OF REINFORCED CONCRETE SWAY FRAMES INVESTIGATION ON APPLICABILITY OF SUBSTITUTE BEAM - COLUMN FRAME FOR DESIGN OF REINFORCED CONCRETE SWAY FRAMES Abrham Ewnti and *Girma Zrayohanns School of Civil and Environmntal Enginring, Addis Ababa

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by: Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or

More information

3 Finite Element Parametric Geometry

3 Finite Element Parametric Geometry 3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,

More information

Principles of Humidity Dalton s law

Principles of Humidity Dalton s law Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):. Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions

More information

In this lecture... Subsonic and supersonic nozzles Working of these nozzles Performance parameters for nozzles

In this lecture... Subsonic and supersonic nozzles Working of these nozzles Performance parameters for nozzles Lct-30 Lct-30 In this lctur... Subsonic and suprsonic nozzls Working of ths nozzls rformanc paramtrs for nozzls rof. Bhaskar Roy, rof. A M radp, Dpartmnt of Arospac, II Bombay Lct-30 Variation of fluid

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

Laboratory work # 8 (14) EXPERIMENTAL ESTIMATION OF CRITICAL STRESSES IN STRINGER UNDER COMPRESSION

Laboratory 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 information

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

More information

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS Stig Holst ABB Automation Products Swdn Bapuji S Palki ABB Utilitis India This papr rports

More information

The Autonomous Underwater Vehicle (AUV) MAYA: General Description

The Autonomous Underwater Vehicle (AUV) MAYA: General Description Introduction h ocans and rivrs always hav bn and still ar an important sourc of rvnu and prosprity for mankind. Du to th grat importanc of ocans and rivrs, th scintific community maks us of Autonomous

More information

15. Stress-Strain behavior of soils

15. Stress-Strain behavior of soils 15. Strss-Strain bhavior of soils Sand bhavior Usually shard undr draind conditions (rlativly high prmability mans xcss por prssurs ar not gnratd). Paramtrs govrning sand bhaviour is: Rlativ dnsity Effctiv

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

More information

Part 7: Capacitance And Capacitors

Part 7: Capacitance And Capacitors Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.

More information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

PHYS-333: Problem set #2 Solutions

PHYS-333: Problem set #2 Solutions PHYS-333: Problm st #2 Solutions Vrsion of March 5, 2016. 1. Visual binary 15 points): Ovr a priod of 10 yars, two stars sparatd by an angl of 1 arcsc ar obsrvd to mov through a full circl about a point

More information

Hydrogen Atom and One Electron Ions

Hydrogen Atom and One Electron Ions Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial

More information

Math 34A. Final Review

Math 34A. Final Review Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right

More information

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA * 17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High

More information

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE 13 th World Confrnc on Earthquak Enginring Vancouvr, B.C., Canada August 1-6, 2004 Papr No. 2165 INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

More information

Strength of Materials

Strength of Materials Strngth of Matrials Sssion Column 08 ctur not : ramudiyanto, M.Eng. Strngth of Matrials STBIITY OF STRUCTURE In th dsign of columns, oss-sctional ara is slctd such that - allowabl strss is not xcdd all

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination Univrsity of Illinois at Chicago Dpartmnt of hysics hrmodynamics & tatistical Mchanics Qualifying Eamination January 9, 009 9.00 am 1:00 pm Full crdit can b achivd from compltly corrct answrs to 4 qustions.

More information

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt

More information

An Investigation on the Effect of the Coupled and Uncoupled Formulation on Transient Seepage by the Finite Element Method

An Investigation on the Effect of the Coupled and Uncoupled Formulation on Transient Seepage by the Finite Element Method Amrican Journal of Applid Scincs 4 (1): 95-956, 7 ISSN 1546-939 7 Scinc Publications An Invstigation on th Effct of th Coupld and Uncoupld Formulation on Transint Spag by th Finit Elmnt Mthod 1 Ahad Ouria,

More information

INTEGRATION BY PARTS

INTEGRATION BY PARTS Mathmatics Rvision Guids Intgration by Parts Pag of 7 MK HOME TUITION Mathmatics Rvision Guids Lvl: AS / A Lvl AQA : C Edcl: C OCR: C OCR MEI: C INTEGRATION BY PARTS Vrsion : Dat: --5 Eampls - 6 ar copyrightd

More information

High Energy Physics. Lecture 5 The Passage of Particles through Matter

High Energy Physics. Lecture 5 The Passage of Particles through Matter High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

Extraction of Doping Density Distributions from C-V Curves

Extraction of Doping Density Distributions from C-V Curves Extraction of Doping Dnsity Distributions from C-V Curvs Hartmut F.-W. Sadrozinski SCIPP, Univ. California Santa Cruz, Santa Cruz, CA 9564 USA 1. Connction btwn C, N, V Start with Poisson quation d V =

More information

Introduction to Condensed Matter Physics

Introduction to Condensed Matter Physics Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at

More information

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of

More information

Finite element discretization of Laplace and Poisson equations

Finite element discretization of Laplace and Poisson equations Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018 Propositional Logic Combinatorial Problm Solving (CPS) Albrt Olivras Enric Rodríguz-Carbonll May 17, 2018 Ovrviw of th sssion Dfinition of Propositional Logic Gnral Concpts in Logic Rduction to SAT CNFs

More information

Differential Equations

Differential Equations UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs

More information

Principles of LEV Design. Duct friction losses Friction losses increase linearly with duct length increasing air density, typical form: L

Principles of LEV Design. Duct friction losses Friction losses increase linearly with duct length increasing air density, typical form: L Typs of losss Entry losss, ducts and hoods Friction Losss: Fluid in motion ncountrs drag along th surfac Enrgy is ndd to ovrcom th drag forc Th drag forc is du to th fluid viscosity Dynamic losss Turbulnc

More information

General Notes About 2007 AP Physics Scoring Guidelines

General Notes About 2007 AP Physics Scoring Guidelines AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

Sec 2.3 Modeling with First Order Equations

Sec 2.3 Modeling with First Order Equations Sc.3 Modling with First Ordr Equations Mathmatical modls charactriz physical systms, oftn using diffrntial quations. Modl Construction: Translating physical situation into mathmatical trms. Clarly stat

More information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw

More information

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle CHPTER 1 Introductory Concpts Elmnts of Vctor nalysis Nwton s Laws Units Th basis of Nwtonian Mchanics D lmbrt s Principl 1 Scinc of Mchanics: It is concrnd with th motion of matrial bodis. odis hav diffrnt

More information

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

More information

Flocculator Design. Overview. Top View. Side View. Design Considerations. More Design Considerations 1/10/2017

Flocculator Design. Overview. Top View. Side View. Design Considerations. More Design Considerations 1/10/2017 1/10/017 Flocculator sign Ovrviw Analysis of hydraulic flocculators Ratio of maximum to avrag nrgy dissipation rat Infficincy of nrgy us du to nonuniformity of nrgy dissipation rat Th grat transition at

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

Massachusetts Institute of Technology Department of Mechanical Engineering

Massachusetts Institute of Technology Department of Mechanical Engineering Massachustts Institut of Tchnolog Dpartmnt of Mchanical Enginring. Introduction to Robotics Mid-Trm Eamination Novmbr, 005 :0 pm 4:0 pm Clos-Book. Two shts of nots ar allowd. Show how ou arrivd at our

More information

ELECTRON-MUON SCATTERING

ELECTRON-MUON SCATTERING ELECTRON-MUON SCATTERING ABSTRACT Th lctron charg is considrd to b distributd or xtndd in spac. Th diffrntial of th lctron charg is st qual to a function of lctron charg coordinats multiplid by a four-dimnsional

More information

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.

More information

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

Classical Magnetic Dipole

Classical Magnetic Dipole Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg

More information

Sundials and Linear Algebra

Sundials and Linear Algebra Sundials and Linar Algbra M. Scot Swan July 2, 25 Most txts on crating sundials ar dirctd towards thos who ar solly intrstd in making and using sundials and usually assums minimal mathmatical background.

More information

Flow Switch Diaphragm Type Flow Switch IFW5 10 N Diaphragm type flow switch. Thread type. Model Body size Set flow rate

Flow Switch Diaphragm Type Flow Switch IFW5 10 N Diaphragm type flow switch. Thread type. Model Body size Set flow rate Flo Sitch Diaphragm Typ Flo Sitch IFW5 Sris [Option] Th flo sitch, IFW sris is usd for dtction and confirmation of th flo as a rlaying dvic for th gnral atr applications in som various uipmnt such as cooling

More information

TEMASEK JUNIOR COLLEGE, SINGAPORE. JC 2 Preliminary Examination 2017

TEMASEK JUNIOR COLLEGE, SINGAPORE. JC 2 Preliminary Examination 2017 TEMASEK JUNIOR COLLEGE, SINGAPORE JC Prliminary Eamination 7 MATHEMATICS 886/ Highr 9 August 7 Additional Matrials: Answr papr hours List of Formula (MF6) READ THESE INSTRUCTIONS FIRST Writ your Civics

More information

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea 2017 Watr Ractor Ful Prformanc Mting Sptmbr 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jju Jju Island, Kora Study of Ful Rod Bhavior with Missing Pllt Surfac Dfct Zhnhai Liu 1, Yi Zhou 1, Ping Chn 1, Yuanming

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

Mor Tutorial at www.dumblittldoctor.com Work th problms without a calculator, but us a calculator to chck rsults. And try diffrntiating your answrs in part III as a usful chck. I. Applications of Intgration

More information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

PHA 5127 Answers Homework 2 Fall 2001

PHA 5127 Answers Homework 2 Fall 2001 PH 5127 nswrs Homwork 2 Fall 2001 OK, bfor you rad th answrs, many of you spnt a lot of tim on this homwork. Plas, nxt tim if you hav qustions plas com talk/ask us. Thr is no nd to suffr (wll a littl suffring

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

de/dx Effectively all charged particles except electrons

de/dx Effectively all charged particles except electrons de/dx Lt s nxt turn our attntion to how chargd particls los nrgy in mattr To start with w ll considr only havy chargd particls lik muons, pions, protons, alphas, havy ions, Effctivly all chargd particls

More information

STRESSES FROM LOADING ON RIGID PAVEMENT COURSES

STRESSES FROM LOADING ON RIGID PAVEMENT COURSES bartosova.qxd 16.8.004 14:34 StrÆnka 3 003/1 PAGES 3 37 RECEIVED 5. 6. 00 ACCEPTED 15. 11. 00 ¼. BARTOŠOVÁ STRESSES FROM LOADING ON RIGID PAVEMENT COURSES ¼udmila Bartošová, Ing., PD. Assistant lcturr

More information

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna 1 Journal of Microwavs, Optolctronics and Elctromagntic Applications, Vol. 6, No. 2, Dcmbr 2007 406 Koch Fractal Boundary Singl fd Circularly Polarizd Microstrip Antnna P. Nagswara Rao and N. V. S.N Sarma

More information

A General Thermal Equilibrium Discharge Flow Model

A General Thermal Equilibrium Discharge Flow Model Journal of Enrgy and Powr Enginring 1 (216) 392-399 doi: 1.17265/1934-8975/216.7.2 D DAVID PUBLISHING A Gnral Thrmal Equilibrium Discharg Flow Modl Minfu Zhao, Dongxu Zhang and Yufng Lv Dpartmnt of Ractor

More information

Preliminary Fundamentals

Preliminary Fundamentals 1.0 Introduction Prliminary Fundamntals In all of our prvious work, w assumd a vry simpl modl of th lctromagntic torqu T (or powr) that is rquird in th swing quation to obtain th acclrating torqu. This

More information

NTHU ESS5850 Micro System Design F. G. Tseng Fall/2016, 7-2, p1. Lecture 7-2 MOSIS/SCNA Design Example- Piezoresistive type Accelerometer II

NTHU ESS5850 Micro System Design F. G. Tseng Fall/2016, 7-2, p1. Lecture 7-2 MOSIS/SCNA Design Example- Piezoresistive type Accelerometer II F. G. Tsng Fall/016, 7-, p1 ctur 7- MOSIS/SCNA Dsign Exampl-!! Pizorsistivity Pizorsistiv typ Acclromtr II a Considr a conductiv lock of dimnsion a as shown in th figur. If a currnt is passd through th

More information

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions. Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind

More information

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007 Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

Why is a E&M nature of light not sufficient to explain experiments?

Why is a E&M nature of light not sufficient to explain experiments? 1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt

More information

EFFECT OF CONSOLIDATION RATIOS ON MAXIMUM DYNAMIC SHEAR MODULUS OF SANDS

EFFECT OF CONSOLIDATION RATIOS ON MAXIMUM DYNAMIC SHEAR MODULUS OF SANDS Octobr 12-17, 28, Bijing, China EFFECT OF CONSOLIDATION RATIOS ON MAXIMUM DYNAMIC SHEAR MODULUS OF SANDS Xiaoming YUAN 1 Jing SUN 2 and Rui SUN 3 1 Profssor, Dpt. of otchnical Enginring, Institut of Enginring

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

are given in the table below. t (hours)

are given in the table below. t (hours) CALCULUS WORKSHEET ON INTEGRATION WITH DATA Work th following on notbook papr. Giv dcimal answrs corrct to thr dcimal placs.. A tank contains gallons of oil at tim t = hours. Oil is bing pumpd into th

More information

Abstract Interpretation. Lecture 5. Profs. Aiken, Barrett & Dill CS 357 Lecture 5 1

Abstract Interpretation. Lecture 5. Profs. Aiken, Barrett & Dill CS 357 Lecture 5 1 Abstract Intrprtation 1 History On brakthrough papr Cousot & Cousot 77 (?) Inspird by Dataflow analysis Dnotational smantics Enthusiastically mbracd by th community At last th functional community... At

More information

Symmetric centrosymmetric matrix vector multiplication

Symmetric centrosymmetric matrix vector multiplication Linar Algbra and its Applications 320 (2000) 193 198 www.lsvir.com/locat/laa Symmtric cntrosymmtric matrix vctor multiplication A. Mlman 1 Dpartmnt of Mathmatics, Univrsity of San Francisco, San Francisco,

More information

MCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems

MCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems MCE503: Modling and Simulation o Mchatronic Systms Discussion on Bond Graph Sign Convntions or Elctrical Systms Hanz ichtr, PhD Clvland Stat Univrsity, Dpt o Mchanical Enginring 1 Basic Assumption In a

More information

SUMMER 17 EXAMINATION

SUMMER 17 EXAMINATION (ISO/IEC - 7-5 Crtifid) SUMMER 7 EXAMINATION Modl wr jct Cod: Important Instructions to aminrs: ) Th answrs should b amind by ky words and not as word-to-word as givn in th modl answr schm. ) Th modl answr

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information