Flexural Behaviour of Precast, Prestressed Ribbed RPC Bottom Panels
|
|
- Warren Owen
- 5 years ago
- Views:
Transcription
1 Send Orders for Reprins o reprins@benhamsiene.ae 98 The Open Civil Engineering Journal Open Aess Flexural Behaviour of Preas Presressed Ribbed RPC Boom Panels Zheng Wenzhong* Lu Xueyuan and Wang Ying Key Lab of Sruures Dynami Behavior and Conrol of he Minisry Eduaion Harbin Insiue of Tehnology Harbin P.R. China Absra: This sudy inrodues a new ype of preas presressed reaive powder onree (RPC) boom panel for a large-span omposie slab. The boom panels whih have one or wo invered ribs wih openings a as formwork during he onsruion sage. The paper experimenally invesigaed he rak haraerisis defleion and normal seion bearing apaiy of four preas presressed ribbed RPC boom panels under flexural load. The resuls indiaed ha he RPC ulimae srain under non-uniform ompression is and he plasi influene oeffiien of he seion modulus is linear wih he longiudinal reinforemen raio. The ensile sress of RPC a he raked seion should be onsidered while alulaing he flexural siffness; he equaion used o deermine he nominal ensile sress of RPC as a major variable for alulaing he rak widh a he boom of panels was proposed. The boom panels generally exhibi an over-reinfored failure mode behaviour wihou he omposie layer; he alulaion mehod of he normal seion bearing apaiy of his mode was esablished. Keywords: Crak widh flexural siffness normal seion bearing apaiy preas presressed ribbed RPC boom panel reaive powder onree. 1. INTRODUCTION The omposie slab is a semi-fabriaed sysem ha onsiss of a preas boom panel and a omposie layer. The preas boom panel as as formwork during he onsruion sage and hen forms an inegral par of he omposie layer afer he solidifiaion of as-in-plae onree. Compared wih as-in-plae slabs omposie slabs have he advanages of low os rapid onsruion and improved qualiy onrol whih have led o is widespread appliaion hroughou he world [1 ]. To improve he inegriy of he wo layers a preas boom panel wih rough surfaes [2 3] or wih laie seel russ projes a he op [4-6] an be used. Preas boom panels wih a rough surfae are easy o produe bu have small spans. Preas boom panels wih laie seel russ projes a he op have beer inegriy and larger spans; however seel russes are expensive if hey are applied in large spans. To overome hese problems Jiang Qingqing [7] proposed a preas boom slab wih an invered rib ha has beer flexural siffness and bearing apaiy whih an be applied in larger spans and an redue os. To produe wo-way omposie slabs and furher improve he inegriy of he wo layers Wu Fangbo [8 9] and Zhou Youxiang [10] proposed he use of solid and hollow omposie slabs wih preas presressed ribbed boom panels respeively. The preas boom panels and heir omposie slabs are shown in Fig. (1). A row of invered ribs on whih reangular openings are se is loaed in he middle of he preas boom panel of a solid omposie slab (Fig. (1). *Address orrespondene o his auhor a he Key Lab of Sruures Dynami Behavior and Conrol of he Minisry Eduaion Harbin Insiue of Tehnology Harbin P.R. China; Tel: ; Fax: ; lv_xueyuan@126.om (a1)). Following he assembly of he boom panel ransverse reinforemens an be arranged in he reangular openings and a wo-way solid omposie slab ha has good inegriy is formed afer he as-in-plae onree is poured and hardened (Fig. (1). (a2)). A double-rib preas boom panel is applied in hollow omposie slabs (Fig. (1). (b1)). Eah side of he boom panel onains a row of invered ribs wih reangular openings. Lighweigh maerials an be plaed beween he wo rows of ribs during onsruion. Following assembly ransverse reinforemens an be arranged in he openings and a wo-way hollow omposie slab ha has good inegriy is formed afer solidifiaion of he as-in-plae onree (Fig. (1). (b2)). The appliable spans of boh omposie slabs menioned above are generally less han 8 m. One reason for he limied span is ha he presressing wires in preas boom panels provide mos of he reinforemen of a omposie slab; as a resul as he span of a omposie slab inreases he amoun of presressing in he boom panel mus be inreased whih leads o he exessive elasi ompression and reeping loss of he presress. Anoher reason is ha he flexural rak srain of an ordinary onree is relaively low so he rak widh and defleion mos likely anno saisfy he servieabiliy requiremens. To avoid hese problems we proposed using reaive powder onree (RPC) insead of ordinary onree o manufaure he preas presressed ribbed boom panels menioned above. RPC is a relaively new emen marix omposie ha was invened in he 1990 s [11 12]; RPC has ulra-high mehanial properies (he ompressive srengh is generally in he range of MPa) and superior durabiliy [13 14] and i an be used as an exellen building maerial. Currenly RPC is used in many ypes of onsruion inluding / Benham Open
2 Flexural Behaviour of Preas Presressed Ribbed RPC Boom Panels The Open Civil Engineering Journal 2015 Volume 9 99 (a1) Single-rib preas boom panel (b1) Double-rib preas boom panel (a2) Solid omposie slab Fig. (1). Preas ribbed boom panels and omposie slabs. (b2) Hollow omposie slab Table 1. Speimen parameers. Speimens Number of Presressing Wires Calulaion Span/mm b/mm b 1/mm h 1/mm h/mm B B B B Table 2. Speimen parameers. Cemen SF GBFS Quarz sand Superplasiizer W/B Seel fibre (by Volume) bridges [15] faory buildings [16] oean engineering and rehabiliaion [17]. A he servieabiliy limi sae and he ulimae limi sae he sress of he RPC in he ension zone of he flexural members should no be negleed [18]. Therefore i is neessary o sudy he flexural behaviour of hese members inluding he disribuion and developmen of raks he developmen of he alulaion mehods of he raking momen he flexural siffness and he normal seion bearing apaiy. 2. EXPERIMENTAL DETAIL 2.1. Speimen Design Four preas presressed ribbed RPC boom panels were designed and fabriaed of whih B1 and B2 were single-rib preas boom panels and B3 and B4 were double-rib preas boom panels. Eah of he speimens had a lengh of 2600 mm and he widh and hikness of he preas boom panel s flange was 500 mm and 40 mm respeively. The size of eah of he reangular openings in he invered ribs was 75 mm 25 mm and he spaing was 125 mm. Preensioned ehnology was used o produe he preas boom panel and he presressing wires were loaed a he middle of he preas boom panel s flange. The he parameers are presened in Table 1 and deails of speimens are shown in Fig. (2) Maerials The emeniious maerials used in his paper are as follows: P O 42.5 Porland emen (Chinese ode sandard ompressive > 42.5 MPa a he age of 28 days). The silia fume (SF) SiO 2 onen exeeds 92% and has a speifi surfae area of m 2 /kg. The granulaed blas furnae slag (GBFS) has a speifi surfae area of 475 m 2 /kg. Quarz sand: pariles of fineness of 70 holes and 140 holes were mixed in a raio of 1:1. Superplasiizer: polyarboxylae was used as a superplasiizer in he RPC mixes. Copperized seel fibres ha were 13 mm in lengh and 0.22 mm in diameer were used. The speimens remained in he formwork for 24 h and were auolaved a C for 12 h o aelerae he uring afer demoulding as presened in Table 2.
3 100 The Open Civil Engineering Journal 2015 Volume 9 Wenzhong e al. (a) Single-rib preas boom panel Fig. (2). Deails of he speimens. (b) Double-rib preas boom panel Table 3. Mehanial haraerisis of RPC in speimens. Speimen B1 B2 B3 B4 Compressive srengh /MPa Axial ensile srengh /MPa Noe: he RPC elasi modulus was 41.2 GPa and he RPC ompressive srain orresponding o he peak sress was Fig. (3). RPC dumbbell-shaped speimen. The speimens used for he ompression ess were 70.7 mm 70.7 mm 228 mm prisms and dumbbell-shaped (shown in Fig. (3) speimens were used for he axial ensile ess. The mehanial haraerisis of he RPC used in he speimens is presened in Table 3. The equaion of he ompressive sress-srain relaionship is given by Equaion (1):
4 Flexural Behaviour of Preas Presressed Ribbed RPC Boom Panels The Open Civil Engineering Journal 2015 Volume P/2 LVDT P/2 LVDT Blok LVDT Fig. (4). Experimenal devie. Fig. (5). Measuremen of he effeive presress. * 1.55 " #1.2 " 4 $ ' $ " & 0 %" ) " ' & 0 ( %" ) 0 ( "! f = + " 0 $ 6 & " 2 ' #1 %" ) + " - 0 ( " 0 where! is he ompressive sress of he RPC prism; f is he ompressive srengh of he RPC prism;! is he ompressive srain of he RPC prism; and! 0 is he ompressive srain orresponding o he peak sress of RPC. The reinforemen in he speimens onsised of low relaxaion spiral ribbed wires wih an elasi modulus of 193 GPa a srengh of 1588 MPa and a yield srengh of 1451 MPa. The onrolled sress for he srehing was 1020 MPa Experimenal Devie Speimens were simply suppored and esed under woonenraed line loads applied a he middle-hird of he slabs. To onvenienly observe he raks he boom faes of he speimens were oriened upward. To avoid he shear lag effe [19] rigidiy bloks were used o level he ribs and flange of eah of he speimens. The mid-span defleion was moniored using linear variable differenial ransformers (LVDTs). Resisane srain gauges were oninuously aahed a he op of ribs and he boom surfae of speimens of he pure bending seion; he experimenal devie is shown in Fig. (4). A eah level of load he widh of eah rak a he inerseion poins wih presressing wires were moniored using a rak-widh measuremen insrumen (0.002 mm) and he new raks were marked. 5 (1) 2.4. Measuremen of he Effeive Presress To auraely deermine he effeive presress of he presressing wires in he speimens he booms of he ribbed RPC boom panels (whih were fabriaed under he same ondiions) were grooved o expose he presressing wires and resisane srain gauges were aahed as shown in Fig. (5). The hanges in srain were measured by a srain olleion sysem and hen he effeive presress in he presressing wires was alulaed. 3. STRUCTURAL RESPONSE The raking momens of B1 B2 B3 and B4 were 7.67 kn m kn m kn m and kn m respeively. The firs rak of eah of he speimens appeared a he seion wih he opening. The raks exended and widened wih loading and some of he raks exended o he upper fae of he flange of eah speimen; however no rak was found on he ribs. Craks disappeared afer exending aross some disane and hen randomly appeared again a a nearby loaion and oninued o exend in he same direion. The raks on he boom fae of he flange of eah speimen were fine dense and disoninuous and no onsisen rak spaing was observed. The rak widh was obviously narrower han ha of an ordinary onree flexural member: a he mid-span momen of 0.95 imes he ulimae bending momen (M u ) he observed maximum rak widh was 0.2 mm. New raks were onsanly emerging unil he ulimae bending momen; he rak paerns of he pure bending seion on he boom fae of speimens are shown in Fig. (6). The mid-span load-defleion urves of all of he speimens are shown in Fig. (7). The mid-span defleions were approximaely linear wih he load before raking and beame larger gradually afer raking. When he load ex-
5 102 The Open Civil Engineering Journal 2015 Volume 9 Wenzhong e al. (a) B1 (b) B2 () B3 Fig. (6). Crak paerns on he boom fae of he speimens. eeded 0.8 M u he mid-span load-defleion urves ended o be horizonal and failure ourred due o he rushing of he RPC on he op of rib while he presressing wires did no yield. The ulimae bending momens of B1 B2 B3 and B4 were kn m kn m kn m and kn m respeively. The rushed area of he RPC was limied o he seion of he reangular opening for B1; however no relaionship wih he seion of reangular openings was found for he oher speimens. Only one of he ribs failed for speimens B3 and B4. The RPC ompressive srain on he op of he rib was found o inrease approximaely linearly wih loading before raking and o inrease gradually afer raking and he RPC ompressive srain was found o inrease subsanially while approahing failure. The RPC ompressive srain on he op of he rib was approximaely a he momen before failure ourred whih is onsisen wih he resul of he RPC beam [20]. All of he speimens exhibied he over-reinfored failure mode behaviour. In he ype of boom panel onsidered here he presressing wires are he major reinforemen of he omposie slabs in praial engineering. When suh a boom panel is a he ulimae limi sae he ompressive area of onree is muh greaer han ha of he RPC rib; herefore his ype of boom panel wihou omposie onree layer generally exhibis over-reinfored failure mode behaviour. 4. RESULTS AND DISCUSSION The seion wih openings was hosen as he alulaing seion in his paper beause i is he weakes seion of a preas presressed ribbed RPC boom panel. (d) B4 Fig. (7). Mid-span load-defleion urves Effeive Sress in he Presressing Wires The experimenal resuls indiaed ha he average effeive presress in he presressing wires of B1 B2 B3 and B4 under no-load ondiions were MPa MPa MPa and MPa respeively. The alulaions in he elasi analysis deermined ha he RPC ompressive sress on he op of he ribs for B1 B2 B3 and B4 were 6.13 MPa 9.46 MPa 9.79 MPa and MPa respeively and he sress levels (! p f R ) for B1 B2 B3 and B4 were and respeively.
6 Flexural Behaviour of Preas Presressed Ribbed RPC Boom Panels The Open Civil Engineering Journal 2015 Volume Fig. (8). Sress and srain disribuions a he raked seion Craking Momen The flexural raking ensile srains of B1 B2 B3 and B4 were and respeively whih were muh greaer han he srain orresponding o he RPC peak ensile sress [21]. Under he raking momens of he speimens he ompressive srains of RPC on he op of ribs are relaively small and in he elasi region bu he par of he RPC in he ension zone beame plasi. To alulae he raking momen of speimen he plasi influene oeffiien of he seion modulus! was inrodued. Aording o referene [22]! an be alulaed as follows:! = M r "# W p 0 f R (2) where M r is he raking momen and W 0 is he ransformed elasi seion modulus a he exreme ension fibre (he elasi modulus raio of presressing wires o RPC is α E =E p /E R =193000/41200=4.68). Based on he experimenal daa! of B1 B2 B3 and B4 was and 1.51 respeively. The bond beween presressing wires and RPC an inhibi raking; herefore! inreased wih he inrease of presressing wire amoun. Fiing he resuls generaed Equaion (3).! = 24.75" e (3) where! e is he raio of he area of he presressing wires o he area of he preas presressed ribbed RPC boom panels flange. The mean raio of fied values o experimenal derived values of! is 1.01 and he oeffiien of variaion is Defleion Calulaion The flexural siffness of all speimens dereased wih he inrease of he mid-span momen. Under he raking momen he flexural siffness values of B1 B2 B3 and B4 were 0.84E R I 0.84E R I 0.85E R I and 0.88E R I respeively whih were onsisen wih ha of an ordinary onree flexural member [22]. To simplify he alulaion 0.85E R I was aken as he flexural siffness of he speimens before raking ourred. In he pos-raking sage based on plane ross-seion assumpion he heigh of he neural axis an be alulaed aording o he daa measured by resisane srain gauges aahed a he op of ribs and he boom of he speimens. For he mid-span momen beween M r -0.8 M u he heighs of he neural axis of he speimens remain approximaely onsan. The mean heighs of he neural axis of B1 B2 B3 and B4 were 34.8 mm 65.9 mm 53.7 mm and 62.3 mm respeively. The formula o alulae he mean heigh of he neural axis in pos-raking sage (M r -0.8 M u ) was deermined by fiing o be he following: x 91.2 Ar = + A 22.1 (4) f where A r is he ross-seional area of ribs wihou opening and A f is he ross-seional area of he flange of he speimen. The mean raio of he fied values o he experimenally derived values of he heigh of he neural axis is 1.0 and he oeffiien of variaion is To onsider he ensile sress of RPC a a raked seion he RPC ensile sress of he preas boom panel flange is assumed o be uniformly disribued he reduion oeffiien of he RPC elasi modulus ( k! ) is inrodued and he RPC ensile sress on he ribs is assumed o be negligible. The pos-raking flexural siffness model of he speimens is shown in Fig. (8). When he neural axis passes hrough he openings and above he openings he momens of ineria ( I r ) a he raked seions an be alulaed using Equaions (5-1). and (5-2). I r = ( ) b r x 3! x" # E A p x k" bh f x I r = b r x3 3 +! E A p x k" bh f x (5-1) (5-2) where x! is he disane from he neural axis o he op of he openings. The effeive momen of ineria an be alulaed using Equaion (6).
7 104 The Open Civil Engineering Journal 2015 Volume 9 Wenzhong e al.! I e = # " M r M 3 $ (! & I g + * 1' # % * ) " where I g =0.85I. M r M 3 $ + - & % - I r (6) On he basis of mehanis knowledge he pos-raking defleion of mid-span an be alulaed as follows: 23pl 3! = (7) 1296E R I e Aording o he analysis i an be deermined ha k! = The alulaed flexural siffness (! ) agreed well wih he experimenally derived flexural siffness (! ) (M r M u )!! is shown in Fig. (9) for whih he mean value is 1.02 and he oeffiien of variaion is Fig. (9). Raio of he fied value o he experimenally derived value of he mid-span defleion Crak Widh Calulaion Reinforing seel sress is used as he major variable in mos equaions [22-24] used for alulaing he rak widhs in he flexural members. However he differene beween he disane from he neural axis o he presressing wires and he disane from he neural axis o he boom fae was relaively large; herefore he reinforing seel sress a he raked seion anno auraely predi he rak widh. In his paper he ross-seions of speimens were assumed o be elasi hus enabling he nominal ensile sress (! R ) a boom fae o be alulaed. The reinforemen raio should also be onsidered for he bond beween presressing wires o enable he RPC o inhibi he rak widh. For mid-span momen values of M r -0.8 M u he rak widh was found o be linear wih loading; he fiing resul in Equaion (8). ( ) w m = $ % 2.52! R " # f R & ' (10"3 (8) The experimenal and alulaed resuls of he rak widh are shown in Fig. (10). The mean value of he alulaed rak widh o he measured raked widh was 1.02 and he oeffiien of variaion was Fig. (10). Measured and alulaed values of he average rak widh. The maximum rak widh an be obained by Equaion (8). muliplied by an amplifiaion oeffiien! s : w =! w (9) max s m The amplifiaion oeffiien! s an be deermined using he probabiliy disribuion of he rak widhs. Saisial analysis indiaed ha for he mid-span momen values in he range of M r -0.8 M u wi w m follows he lognormal disribuion wih a mean ( µ ) and sandard deviaion (! ) of and respeively ( w i is he rak widh a a erain load level w m is he average rak widh a he load level). The frequeny disribuion and probabiliy densiy urve of wi w m are shown in Fig. (11). The alulaions indiaed ha he amplifiaion oeffiien (! s ) of he rak widh wih 95% onfidene is 1.9. As a resul he maximum rak widh wih 95% onfidene an be alulaion using Equaion (10). w # 3 (! " f ) = $ ' 4.78 # % ( & 10 (10) m R R Fig. (11). Crak widh frequeny disribuion Normal Seion Bearing Capaiy In onras wih an ordinary onree flexural member he effe of RPC ensile sress should be onsidered a he
8 Flexural Behaviour of Preas Presressed Ribbed RPC Boom Panels The Open Civil Engineering Journal 2015 Volume (a) Aual sress disribuion Fig. (12). Sress disribuion on a ross seion of he speimen a he ulimae momen. (b) Equivalen sress disribuion ulimae momen [20]. The failure mode of all speimens was rushing of he RPC on he op of rib wihou he yielding of he presressing wires; herefore he normal seion bearing apaiy should be alulaed by he mehod of an over-reinfored flexural member. To deermine he normal seion bearing apaiy of a preas presressed ribbed RPC boom panel he follows assumpions are made: 1 he plane seion remains plane afer bending; 2 he ensile sress of he RPC in he boom panel flange has a reangular disribuion wih a heigh of kf R ; and 3 he ensile sress of he RPC in he rib is negleed. To simplify he alulaion he aual sress disribuion an be simplified by an equivalen reangular sress diagram (he remaining ompressive resulan fore and is applied poin onsan) as shown in Fig. (12).). Based on he RPC ompressive sress-srain relaionship he equivalen oeffiiens! and! an be deermined as 0.9 and 0.77 [20] respeively. For he srain of seion ha remains plane afer bending when he yielding of presressing wires and he failure of RPC ourred simulaneously he relaive deph of limiing ompression zone! b an be alulaed aording o following equaion: " 1! b = x b = h p # u + f py $% p0 where ( ) E s # u (11) h p is he effeive deph of he seion f py is he yield srengh of he presressing wires! is he sress in he presressing wire while he normal sress of RPC a he deph of presressing wire is equal o 0 and! u is he RPC ulimae srain under non-uniform ompressive ( ). The values of! b of B1 B2 B3 and B4 were and respeively. To simplify he alulaion and provide a margin of safey he value of! b = was hosen. Based on momen equilibrium he normal seion bearing apaiy is alulaed using Equaion (12). M u =! 1 f bh 2 R p " b ( 1# 0.5" b ) (12) p0 The alulaed value of he normal seion bearing apaiy M u and he experimenally derived value M u were found o agree well: he mean of M M is 0.99 and he oeffiien of variaion is CONCLUSION This paper inrodued preas presressed single-rib and double-rib preas RPC boom panels and invesigaed heir flexural behaviour under flexural load. Based on he resuls he following onlusions an be derived. 1) For a seel fibre mix proporion of 2% by volume he RPC ulimae srain under non-uniform ompressive is whih is greaer han ha of ordinary onree (approximaely ); he RPC bend raking ensile srain is whih is greaer han ha of ordinary onree ( ). 2) The proposed alulaion formula for raking momen onsiders he reinforemen raio when alulaing he plasi influene oeffiien of he seion modulus. 3) The raks a he boom of a preas presressed ribbed RPC boom panel were fine dense and disoninuous and no onsisen rak spaing was found. The proposed alulaion formula used he RPC nominal ensile sress as major variable and onsidered he effe of he reinforemen raio. 4) The flexural siffness gradually redued wih loading. Under he raking momen of he speimens he flexural siffness was deermined o be 0.85ER I. For values of he mid-span momen in he range of M r ~0.8 M u he effe of he RPC ensile sress should be onsidered when alulaing he flexural siffness and he RPC reduion oeffiien of he elasi modulus k! = 0.35 should be used in he alulaion. 5) In a preas presressed ribbed RPC boom panel he primary bearing reinforemens of he omposie slab he speimens exhibied over-reinfored failure mode behaviour. Based on he experimenal resuls he normal seion bearing apaiy of his mode was deermined. CONFLICT OF INTEREST The auhors onfirm ha his arile onen has no onfli of ineres. u u
9 106 The Open Civil Engineering Journal 2015 Volume 9 Wenzhong e al. ACKNOWLEDGEMENTS Delared none. REFERENCES [1] A. A. Yee and D. Hon. Sruural and eonomi benefis of preas / pressressed onree onsruion. PCI Journal vol. 46 pp [2] J.G. Hou and C. X. He. Composiion plane behaviour of presressed omposie slab. Journal of WuHan Universiy of Hydrauli and Elerial Engineering vol. 26 pp [3] E.N.B.S. Julio A. B. Fernando B. V. D. Silva Conree-oonree bond srengh. Influene of he roughness of he subsrae surfae Consruion and Building Maerials vol. 18 pp [4] A.I. Tenhovuori and M.V. Leskela. Longiudinal shear resisane of omposie slab Consru Seel Researh vol. 46 pp [5] M Peni and Y Sun. The longiudinal shear behaviour of a new seel sheeing profile for omposie floor slab Consru Seel Researh vol. 49 pp [6] W.A. Thanoon Y Yardim M.S. Jaafar and J. Noorzaei Sruural behaviour of ferroemen brik omposie floor slab panel Consruion and Building Maerials vol. 24 pp [7] Q.Q. Jiang X.M. Wang H.C. Liu and S.C. Huang Calulaion mehod of omposie slab wih invered-t boom panel Journal of Cenral Souh Universiy and ehnology vol. 34 pp [8] F.B. Wu L Chen and Y.M. Liu. Experimen on Presressed Conree Hollow-ore Composie Slabs. Journal of Arhieure and Civil Engineering vol. 25 pp [9] F.B. Wu H.L. Huang W Chen and X.H. Zhou. Experimenal Analysis on he Mehanial Properies of Conree Composie Slabs wih Preas Presressed Reangular Rib Panels. Journal of Civil Arhieural & Environmenal Engineering. vol. 33 pp [10] Y.X. Zhou and F.P. Wang A Researh on he Floor Cover of Reinfored Conree Core Clip Plank wih Two-Way Dense Ribs Journal of Nanhua Universiy vol. 19 pp [11] P. Rihard and M. Cheyrezy Composiion of Reaive Powder Conrees" Cemen and Conree Researh vol. 25 pp [12] H Yazıı M Yüel S. Aydın and A. S. Karabulu Mehanial properies of reaive powder onree onaining mineral admixures under differen uring regimes Consruion and Building Maerials vol. 23 pp [13] A Cwirzen V Penala and C Vornanen Reaive powder based onrees: Mehanial properies durabiliy and hybrid use wih OPC Cemen and Conree Researh vol. 38 pp [14] N. Roux C. Andrade and M.A. Sanjuan Experimenal Sudy of Durabiliy of Reaive Powder Conrees Journal of Maerials in Civil Engineering vol. 8 pp [15] P.Y. Blais and M. Couure Presressed Pedesrian Bridge- World s Firs Reaive Powder Conree Sruure PCI Journal vol. 44 pp [16] C.J. Ao Conruion ehniques of applying RPC preas unis in ex-ension of indusrial building Shanxi Arhieure vol. 31 pp [17] B.A. Tayeh and B.H.A. Bakar Uilizaion of Ulra-high Performane Fibre Conree (UHPFC) for Rehabiliaion A Review Proedia Engineering vol. 54 pp [18] A.K. Azad and I.Y. Hakeem Flexural behavior of hybrid onree beams reinfored wih ulra-high performane onree bars Consruion and Building Maerials vol. 49 pp [19] C.Y. Tian and J.G. Nie Shear lag analysis of simply suppored omposie seel-onree beams Journal of Tsinghua Universiy. vol. 45 pp [20] W.Z. Zheng L. Li and S.S. Lu Experimenal researh on mehanial performane of normal seion of reinfored reaive powder onree beam Journal of Building Sruures vol. 32 pp [21] X.Y. Lu Y. Wang C.J. Fu and W.Z. Zheng Basi mehanial propery indexes of reaive powder onree Journal of Harbin Insiue of Tehnology vol. 46 pp [22] China. People s Republi of China Minisry of Consruion Code for Design of Conree Sruures 7 Vols. Beijing: People s Republi of China Minisry of Consruion [23] P. Gergely and L.A. Luz Maximum Crak Widh in Reinfored Conree Flexural Members ACI Journal. vol. SP-20 pp [24] E.G. Nawy and P.T. Huang Crak and Defleion Conrol of Preensioned Presressed Beams PCI Journal vol. 22 pp Reeived: Sepember Revised: Deember Aeped: Deember Wenzhong e al.; Liensee Benham Open. This is an open aess arile liensed under he erms of he Creaive Commons Aribuion Non-Commerial Liense (hp://reaiveommons.org/lienses/ by-n/3.0/) whih permis unresried non-ommerial use disribuion and reproduion in any medium provided he work is properly ied.
5.2 Design for Shear (Part I)
5. Design or Shear (Par I) This seion overs he ollowing opis. General Commens Limi Sae o Collapse or Shear 5..1 General Commens Calulaion o Shear Demand The objeive o design is o provide ulimae resisane
More informationNonlinear Finite Element Analysis of Shotcrete Lining Reinforced with Steel Fibre and Steel Sets
IACSIT Inernaional Journal of Engineering and Tehnology, Vol. 5, No. 6, Deember 2013 Nonlinear Finie Elemen Analysis of Shoree Lining Reinfored wih Seel Fibre and Seel Ses Jeong Soo Kim, Moon Kyum Kim,
More informationConcrete damaged plasticity model
Conree damaged asiiy model Conree damaged asiiy model is a maerial model for he analysis of onree sruures mainly under dynami loads suh as earhquakes(only aes an be analyzed under he dynami loads like
More information1.054/1.541 Mechanics and Design of Concrete Structures (3-0-9) Outline 5 Creep and Shrinkage Deformation
1.54/1.541 Mehanis and Design of Conree ruures pring 24 Prof. Oral Buyukozurk Massahuses Insiue of Tehnology Ouline 5 1.54/1.541 Mehanis and Design of Conree ruures (3--9 Ouline 5 and hrinkage Deformaion
More informationNumerical Simulation of Thermal Stresses in Prismatic Concrete Beams Reinforced with FRP Bars under Low Temperatures
Cemisry and Maerials Resear, Vol.5 013 Speial Issue for Inernaional Congress on Maerials & Sruural Sabiliy, Raba, Moroo, 7-30 November 013 Numerial Simulaion of Termal Sresses in Prismai Conree Beams Reinfored
More informationHybrid probabilistic interval dynamic analysis of vehicle-bridge interaction system with uncertainties
1 APCOM & SCM 11-14 h Deember, 13, Singapore Hybrid probabilisi inerval dynami analysis of vehile-bridge ineraion sysem wih unerainies Nengguang iu 1, * Wei Gao 1, Chongmin Song 1 and Nong Zhang 1 Shool
More informationCalculation of Initial Stiffness of Semirigid Connections with Consideration of Rotational Constraint on Angle from Beam Contact Surface
Calulaion of Iniial Siffness of Semirigid Conneions wih Consideraion of Roaional Consrain on Angle from Beam Cona Surfae X.G. Lin Osaka Insiue of Tehnology, Japan K. Asada Oayashi Corporaion, Japan SUMMARY:
More informationANALYSIS OF REINFORCED CONCRETE BUILDINGS IN FIRE
ANALYSIS OF REINFORCED CONCRETE BUILDINGS IN FIRE Dr Zhaohui Huang Universiy of Sheffield 6 May 2005 1 VULCAN layered slab elemens: connecion o beam elemens Plae Elemen Slab nodes y x Reference Plane h
More informationEffect of Aggregate Gradation on Compressive Strength and Elastic Modulus of Cement Treated Aggregate Base Material for Highway Pavement
IOSR Journal of Engineering (IOSRJEN) ISSN (e): 2250-3021, ISSN (p): 2278-8719 Vol. 07, Issue 10 (Oober. 2017), V2 PP 79-89 www.iosrjen.org Effe of Aggregae Gradaion on Compressive Srengh and Elasi Modulus
More informationMECHANICS OF MATERIALS Poisson s Ratio
Poisson s Raio For a slender bar subjeced o axial loading: ε x x y 0 The elongaion in he x-direcion i is accompanied by a conracion in he oher direcions. Assuming ha he maerial is isoropic (no direcional
More informationERRATA. Figure GL. 2 TRANSVERSE CROSS SECTION OF A SCREW SLOT
srew slo: a semi-hollow in an exrusion inended o reain a srew arallel o he axis of he exrusion. (See Figure GL.). Figure GL. TRANSVERSE CROSS SECTION OF A SCREW SLOT self-drilling srew: a srew ha drills
More informationProperties of Two Carbon Composite Materials Using LTM25 Epoxy Resin
NASA Tehnial Memorandum 110286 Properies of Two Carbon Composie Maerials Using LTM25 Epoxy Resin Juan R. Cruz Langley Researh Cener, Hampon, Virginia C. H. Shah and A. S. Posyn Norhrop Grumman Corporaion,
More informationAt the end of this lesson, the students should be able to understand
Insrucional Objecives A he end of his lesson, he sudens should be able o undersand Sress concenraion and he facors responsible. Deerminaion of sress concenraion facor; experimenal and heoreical mehods.
More informationShear failure of plain concrete in strain localized area
Shear failure of plain onree in srain loalized area Y. Kaneko & H. Mihashi Tohoku Universiy, Sendai, Miyagi, Japan S. Ishihara Asanuma Corporaion, Takasuki, Osaka, Japan ABSTRACT: The objeive of his paper
More informationAmit Mehra. Indian School of Business, Hyderabad, INDIA Vijay Mookerjee
RESEARCH ARTICLE HUMAN CAPITAL DEVELOPMENT FOR PROGRAMMERS USING OPEN SOURCE SOFTWARE Ami Mehra Indian Shool of Business, Hyderabad, INDIA {Ami_Mehra@isb.edu} Vijay Mookerjee Shool of Managemen, Uniersiy
More informationBoyce/DiPrima 9 th ed, Ch 6.1: Definition of. Laplace Transform. In this chapter we use the Laplace transform to convert a
Boye/DiPrima 9 h ed, Ch 6.: Definiion of Laplae Transform Elemenary Differenial Equaions and Boundary Value Problems, 9 h ediion, by William E. Boye and Rihard C. DiPrima, 2009 by John Wiley & Sons, In.
More informationMass Transfer Coefficients (MTC) and Correlations I
Mass Transfer Mass Transfer Coeffiiens (MTC) and Correlaions I 7- Mass Transfer Coeffiiens and Correlaions I Diffusion an be desribed in wo ways:. Deailed physial desripion based on Fik s laws and he diffusion
More informationSIMULATION STUDY OF STOCHASTIC CHANNEL REDISTRIBUTION
Developmens in Business Simulaion and Experienial Learning, Volume 3, 3 SIMULATIO STUDY OF STOCHASTIC CHAEL REDISTRIBUTIO Yao Dong-Qing Towson Universiy dyao@owson.edu ABSTRACT In his paper, we invesigae
More informationLinear Quadratic Regulator (LQR) - State Feedback Design
Linear Quadrai Regulaor (LQR) - Sae Feedbak Design A sysem is expressed in sae variable form as x = Ax + Bu n m wih x( ) R, u( ) R and he iniial ondiion x() = x A he sabilizaion problem using sae variable
More informationAnalysis of Tubular Linear Permanent Magnet Motor for Drilling Application
Analysis of Tubular Linear Permanen Magne Moor for Drilling Appliaion Shujun Zhang, Lars Norum, Rober Nilssen Deparmen of Eleri Power Engineering Norwegian Universiy of Siene and Tehnology, Trondheim 7491
More informationLorentz Transformation Properties of Currents for the Particle-Antiparticle Pair Wave Functions
Open Aess Library Journal 17, Volume 4, e373 ISSN Online: 333-971 ISSN Prin: 333-975 Lorenz Transformaion Properies of Currens for he Parile-Aniparile Pair Wave Funions Raja Roy Deparmen of Eleronis and
More informationTensile and Compressive Damage Coupling for Fully-reversed Bending Fatigue of Fibre-reinforced Composites
Van Paepegem, W. and Degriek, J. (00. Tensile and Compressive Damage Coupling for Fully-reversed Bending Faigue of Fibrereinfored Composies. Faigue and Fraure of Engineering Maerials & Sruures, 5(6, 547-56.
More informationCombined Bending with Induced or Applied Torsion of FRP I-Section Beams
Combined Bending wih Induced or Applied Torsion of FRP I-Secion Beams MOJTABA B. SIRJANI School of Science and Technology Norfolk Sae Universiy Norfolk, Virginia 34504 USA sirjani@nsu.edu STEA B. BONDI
More informationShear Strength of Reinforced Concrete Columns Strengthened with Carbon Fiber Reinforced Plastic Sheet
Shear Srengh of Reinforced Concree Columns Srenghened wih Carbon Fiber Reinforced Plasic Shee Lieping Ye 1 Qingrui Yue 2 Deparmen of Civil Engineering Naional Engineering Technical Tsinghua Universiy Technique
More informationDesign of Air Turbine Flow Passage and Analysis of Energy Efficiency
Available online a www.sienedire.om Energy Proedia 7 (0 ) 7 0 Inernaional Conferene on Fuure Elerial Power and Energy Sysems Design of Air Turbine Flow Passage and Analysis of Energy Effiieny PAN Hong-gang
More informationNavneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi
Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec
More informationCurling Stress Equation for Transverse Joint Edge of a Concrete Pavement Slab Based on Finite-Element Method Analysis
TRANSPORTATION RESEARCH RECORD 155 35 Curling Sress Equaion for Transverse Join Edge of a Concree Pavemen Slab Based on Finie-Elemen Mehod Analysis TATSUO NISHIZAWA, TADASHI FUKUDA, SABURO MATSUNO, AND
More informationmywbut.com Lesson 11 Study of DC transients in R-L-C Circuits
mywbu.om esson Sudy of DC ransiens in R--C Ciruis mywbu.om Objeives Be able o wrie differenial equaion for a d iruis onaining wo sorage elemens in presene of a resisane. To develop a horough undersanding
More informationOPTIMUM DESIGN OF STIFFENED PANEL USING THE METHOD OF MATHEMATICAL PROGRAMMING
ICA 000 COGRE OPTIMUM EIG OF TIFFEE PAEL UIG THE METHO OF MATHEMATICAL PROGRAMMIG o. Ing. Anonín Píš!k C. Ing. P"esl Hobza Insiue of Aerospae Engineering Faul of Mehanial Engineering rno Universi of Tehnolog
More informationUltrasonic sound speed of hydrating calcium sulphate hemihydrate; part 1, the calculation of sound speed of slurries and hardened porous material
A.C.J. de ore and H.J.H. Brouwers Ulrasoni sound speed of hydraing alium sulphae hemihydrae; par, he alulaion of sound speed of slurries and hardened porous maerial Absra This arile fouses on he ompuaion
More information(Radiation Dominated) Last Update: 21 June 2006
Chaper Rik s Cosmology uorial: he ime-emperaure Relaionship in he Early Universe Chaper he ime-emperaure Relaionship in he Early Universe (Radiaion Dominaed) Las Updae: 1 June 006 1. Inroduion n In Chaper
More informationGeneralized electromagnetic energy-momentum tensor and scalar curvature of space at the location of charged particle
Generalized eleromagnei energy-momenum ensor and salar urvaure of spae a he loaion of harged parile A.L. Kholmeskii 1, O.V. Missevih and T. Yarman 3 1 Belarus Sae Universiy, Nezavisimosi Avenue, 0030 Minsk,
More informationDESIGN OF TENSION MEMBERS
CHAPTER Srcral Seel Design LRFD Mehod DESIGN OF TENSION MEMBERS Third Ediion A. J. Clark School of Engineering Deparmen of Civil and Environmenal Engineering Par II Srcral Seel Design and Analysis 4 FALL
More informationκt π = (5) T surrface k BASELINE CASE
II. BASELINE CASE PRACICAL CONSIDERAIONS FOR HERMAL SRESSES INDUCED BY SURFACE HEAING James P. Blanhard Universi of Wisonsin Madison 15 Engineering Dr. Madison, WI 5376-169 68-63-391 blanhard@engr.is.edu
More informationAn Inventory Model for Weibull Time-Dependence. Demand Rate with Completely Backlogged. Shortages
Inernaional Mahemaial Forum, 5, 00, no. 5, 675-687 An Invenory Model for Weibull Time-Dependene Demand Rae wih Compleely Baklogged Shorages C. K. Tripahy and U. Mishra Deparmen of Saisis, Sambalpur Universiy
More informationRobust estimation based on the first- and third-moment restrictions of the power transformation model
h Inernaional Congress on Modelling and Simulaion, Adelaide, Ausralia, 6 December 3 www.mssanz.org.au/modsim3 Robus esimaion based on he firs- and hird-momen resricions of he power ransformaion Nawaa,
More informationNumerical simulation of damage in glass subjected to static indentation
8 ème Congrès Français de Méanique Grenoble, 7- aoû 007 Numerial simulaion of damage in glass subjeed o sai indenaion Jewan Ismail, Fahmi Zaïri, Moussa Naï-Abdelaziz & Ziouni Azari Laboraoire de Méanique
More informationThe Nottingham eprints service makes this work by researchers of the University of Nottingham available open access under the following conditions.
Hyde, Chrisopher J. and Hyde, T.H. and Sun, Wei and Beker, A.A. () Damage mehanis based prediions of reep rak growh in 36 sainless seel. Engineering Fraure Mehanis, 77 (). pp. 385-4. ISSN 3-7944 Aess from
More informationIntroduction. σ 2 (1)
Holzforshung 2018; aop Yuxin Wen, Ping Yang, Jian Zhao and Dong Zhao* Theoreial and experimenal onsideraions on he neural axis of wood beams wih a hole in differen loaions hps://doi.org/10.1515/hf-2017-0174
More informationLIGHT and SPECIAL RELATIVITY
VISUAL PHYSICS ONLINE MODULE 7 NATURE OF LIGHT LIGHT and SPECIAL RELATIVITY LENGTH CONTRACTION RELATIVISTIC ADDITION OF VELOCITIES Time is a relaie quaniy: differen obserers an measuremen differen ime
More informationTeacher Quality Policy When Supply Matters: Online Appendix
Teaher Qualiy Poliy When Supply Maers: Online Appendix Jesse Rohsein July 24, 24 A Searh model Eah eaher draws a single ouside job offer eah year. If she aeps he offer, she exis eahing forever. The ouside
More informationA Numerical Hydraulic Fracture Model Using the Extended Finite Element Method
nernaional Conferene on Mehanial and ndusrial Engineering (CME'2013) Augus 28-29, 2013 Penang (Malaysia) A Numerial Hydrauli Fraure Model Using he Exended Finie Elemen Mehod Ashkan. Mahdavi, and Soheil.
More informationLoad carrying capacity of masonry bridges: numerical evaluation of the influence of fill and spandrels
Load arrying apaiy of masonry bridges: numerial evaluaion of he influene of fill and spandrels A. Cavihi and L. Gambaroa Deparmen of Sruural and Geoehnial Engineering, Universiy of Genova, Ialy ABSTRACT.
More informationProblem Set 9 Due December, 7
EE226: Random Proesses in Sysems Leurer: Jean C. Walrand Problem Se 9 Due Deember, 7 Fall 6 GSI: Assane Gueye his problem se essenially reviews Convergene and Renewal proesses. No all exerises are o be
More informationEquilibrium equations at particle: Mx = 0 Summation of Moments about the axis of the member (torque) internal moment = external moment
1/8 5.1 Torsion of Cirular Safs Equilirium equaions a arile: Mx 0 Summaion of Momens aou e axis of e memer (orque) inernal momen exernal momen geomeri assumions for e derivaion of e sear formula on a irular
More information236 CHAPTER 3 Torsion. Strain Energy in Torsion
36 CHAPER 3 orsion Srain Energy in orsion Problem 3.9-1 A solid circular bar of seel (G 11. 1 6 psi) wih lengh 3 in. and diameer d 1.75 in. is subjeced o pure orsion by orques acing a he ends (see figure).
More informationSolutions to Exercises in Chapter 5
in 5. (a) The required inerval is b ± se( ) b where b = 4.768, =.4 and se( b ) =.39. Tha is 4.768 ±.4.39 = ( 4.4, 88.57) We esimae ha β lies beween 4.4 and 85.57. In repeaed samples 95% of similarly onsrued
More informationBoundary Control of a Tensioned Elastic Axially Moving String
ICCAS5 June -5 KINTEX Gyeonggi-Do Korea Boundary Conrol of a Tensioned Elasi Aially Moving Sring Chang-Won Kim* Keum-Shik Hong** and Hahn Park* *Deparmen of Mehanial and Inelligen Sysems Engineering Pusan
More informationAnalysis of composite T beam composed of timber, concrete and carbon strip
WSEAS TRANSACTONS on APPLED and THEORETCAL ECHANCS Analysis o omposie T beam omposed o imber onree and arbon srip ATJAŽ TAJNK PETER DOBRLA ROSLAV PREROV Fauly o ivil engineering Universiy o aribor Smeanova
More information1.8-MHz, 48-V Resonant VRM: Analysis, Design, and Performance Evaluation
1.8-MHz, 48- Resonan RM: Analysis, Design, Performane Evaluaion aszlo Huber 1, Kevin Hsu, Milan M. Jovanović 1, Dennis Solley 3, Gennady Gurov 3, Rober Porer 3 1 Dela Produs Corporaion Dela Eleronis, In.
More informationExponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits
DOI: 0.545/mjis.07.5009 Exponenial Weighed Moving Average (EWMA) Char Under The Assumpion of Moderaeness And Is 3 Conrol Limis KALPESH S TAILOR Assisan Professor, Deparmen of Saisics, M. K. Bhavnagar Universiy,
More informationTRANSMISSION LINES AND WAVEGUIDES. Uniformity along the Direction of Propagation
TRANSMISSION LINES AND WAVEGUIDES Uniformi along he Direion of Propagaion Definiion: Transmission Line TL is he erm o desribe ransmission ssems wih wo or more mealli onduors eleriall insulaed from eah
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationInverted Pendulum-type Personal Mobility Considering Human Vibration Sensitivity
(IJACSA) Inernaional Journal of Advaned Compuer Siene and Appliaions, Vol. 5, No. 3, 14 Invered Pendulum-ype Personal Mobiliy Considering Human Vibraion Sensiiviy Misaki Masuda Shool of Siene for Open
More informationJOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO. 1, JANUARY
JOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO., JANUARY 08 9 Visoelasi Modeling o he Reovery Behavior o Cu Pile Carpe Aer Sai Loading: A Comparison Beween Linear and Nonlinear Models Sahar Jaari * and Mohammad
More informationAN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING
Yugoslav Journal of Operaions Researh 5 (005) Number 77-88 AN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING Liang-Yuh OUYANG Deparmen of Managemen Sienes
More informationInfluence of High Axial Tension on the Shear Strength of non-shear RC Beams
Influence of High Axial Tension on he Shear Srengh of non-shear RC Beams Henrik B. JOERGENSEN PhD candidae Univ. of Souhern Denmark hebj@ii.sdu.dk Joergen MAAGAARD Associae Professor Univ. of Souhern Denmark
More informationDerivation of longitudinal Doppler shift equation between two moving bodies in reference frame at rest
Deriaion o longiudinal Doppler shi equaion beween wo moing bodies in reerene rame a res Masanori Sao Honda Eleronis Co., d., Oyamazuka, Oiwa-ho, Toyohashi, ihi 44-393, Japan E-mail: msao@honda-el.o.jp
More informationProgram: RFEM 5, RSTAB 8, RF-DYNAM Pro, DYNAM Pro. Category: Isotropic Linear Elasticity, Dynamics, Member
Verificaion Example Program: RFEM 5, RSTAB 8, RF-DYNAM Pro, DYNAM Pro Caegory: Isoropic Linear Elasiciy, Dynamics, Member Verificaion Example: 0104 Canilever Beam wih Periodic Exciaion 0104 Canilever Beam
More informationEntropy ISSN
Enropy 003, 5, 467 48 Enropy ISSN 099-4300 www.mdpi.org/enropy/ Full paper CONVECIVE HEAING OF SOLID SURFACE: ENROPY GENERAION DUE O EMPERAURE FIELD AND HERMAL DISPLACEMEN Yagoub Nassar Al-Nassar Mehanial
More informationWrinkling Analysis of Rectangular Soft-Core Composite Sandwich Plates
Wrinkling Analysis of Reangular Sof-Core Composie Sandwih Plaes Mohammad Mahdi Kheirikhah and Mohammad Reza Khalili Absra In he presen haper, a new improved higher-order heory is presened for wrinkling
More information3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon
3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of
More informationCONSIDERATIONS REGARDING THE OPTIMUM DESIGN OF PRESTRESSED ELEMENTS
Bullein of e Transilvania Universiy of Braşov CIBv 5 Vol. 8 (57) Special Issue No. - 5 CONSIDERTIONS REGRDING THE OPTIU DESIGN OF PRESTRESSED ELEENTS D. PRECUPNU C. PRECUPNU bsrac: Engineering educaion
More informationOn Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature
On Measuring Pro-Poor Growh 1. On Various Ways of Measuring Pro-Poor Growh: A Shor eview of he Lieraure During he pas en years or so here have been various suggesions concerning he way one should check
More informationCumulative Damage Evaluation based on Energy Balance Equation
Cumulaive Damage Evaluaion based on Energy Balance Equaion K. Minagawa Saiama Insiue of Technology, Saiama S. Fujia Tokyo Denki Universiy, Tokyo! SUMMARY: This paper describes an evaluaion mehod for cumulaive
More informationThe Asymptotical Behavior of Probability Measures for the Fluctuations of Stochastic Models
The Asympoial Behavior of Probabiliy Measures for he Fluuaions of Sohasi Models JUN WANG CUINING WEI Deparmen of Mahemais College of Siene Beijing Jiaoong Universiy Beijing Jiaoong Universiy Beijing 44
More informationt is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...
Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger
More informationNew effective moduli of isotropic viscoelastic composites. Part I. Theoretical justification
IOP Conference Series: Maerials Science and Engineering PAPE OPEN ACCESS New effecive moduli of isoropic viscoelasic composies. Par I. Theoreical jusificaion To cie his aricle: A A Sveashkov and A A akurov
More informationMechanical Fatigue and Load-Induced Aging of Loudspeaker Suspension. Wolfgang Klippel,
Mechanical Faigue and Load-Induced Aging of Loudspeaker Suspension Wolfgang Klippel, Insiue of Acousics and Speech Communicaion Dresden Universiy of Technology presened a he ALMA Symposium 2012, Las Vegas
More informationv A Since the axial rigidity k ij is defined by P/v A, we obtain Pa 3
The The rd rd Inernaional Conference on on Design Engineering and Science, ICDES 14 Pilsen, Czech Pilsen, Republic, Czech Augus Republic, 1 Sepember 1-, 14 In-plane and Ou-of-plane Deflecion of J-shaped
More informationR t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t
Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,
More informationStochastic Model for Cancer Cell Growth through Single Forward Mutation
Journal of Modern Applied Saisical Mehods Volume 16 Issue 1 Aricle 31 5-1-2017 Sochasic Model for Cancer Cell Growh hrough Single Forward Muaion Jayabharahiraj Jayabalan Pondicherry Universiy, jayabharahi8@gmail.com
More informationEE40 Summer 2005: Lecture 2 Instructor: Octavian Florescu 1. Measuring Voltages and Currents
Announemens HW # Due oday a 6pm. HW # posed online oday and due nex Tuesday a 6pm. Due o sheduling onflis wih some sudens, lasses will resume normally his week and nex. Miderm enaively 7/. EE4 Summer 5:
More informationExcel-Based Solution Method For The Optimal Policy Of The Hadley And Whittin s Exact Model With Arma Demand
Excel-Based Soluion Mehod For The Opimal Policy Of The Hadley And Whiin s Exac Model Wih Arma Demand Kal Nami School of Business and Economics Winson Salem Sae Universiy Winson Salem, NC 27110 Phone: (336)750-2338
More informationThermomechanical Response of a Thin Sandwich Composite Structure
Thermomechanical Response of a Thin Sandwich Composie Srucure Horaiu Teodorescu-Draghicescu, Sorin Vlase, Dana Luca Mooc, and Anghel Chiru Absrac The paper presens a siffness evaluaion as well as hermal
More information1.054/1.541 Mechanics and Design of Concrete Structures (3-0-9) Outline 10 Torsion, Shear, and Flexure
.54/.54 Mehani and Deign of Conree Srre Spring 4 Prof. Oral Bkozrk Maahe Inie of ehnolog Oline.54/.54 Mehani and Deign of Conree Srre (3--9) Oline orion, Shear, and Flere orion o Sre diribion on a ro eion
More informationSoil Moisture Measurement by Using Seismic Wave
oil Moisure Measuremen by Using eismi Wae F. Adamo, G. Andria, F. Aiissimo, L. Fabbiano, N. Giaquino Laboraory for Eleri and Eleroni Measuremens Deparmen of Eleris and Eleronis (DEE) Polyehni of Bari Via
More informationEnergy Momentum Tensor for Photonic System
018 IJSST Volume 4 Issue 10 Prin ISSN : 395-6011 Online ISSN : 395-60X Themed Seion: Siene and Tehnology Energy Momenum Tensor for Phooni Sysem ampada Misra Ex-Gues-Teaher, Deparmens of Eleronis, Vidyasagar
More informationDynamic System In Biology
Compuaional Siene and Engineering Dnami Ssem In Biolog Yang Cao Deparmen of Compuer Siene hp://ourses.s.v.edu/~s644 Ouline Compuaional Siene and Engineering Single Speies opulaion Model Malhus Model Logisi
More informationBias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé
Bias in Condiional and Uncondiional Fixed Effecs Logi Esimaion: a Correcion * Tom Coupé Economics Educaion and Research Consorium, Naional Universiy of Kyiv Mohyla Academy Address: Vul Voloska 10, 04070
More informationDesigning Information Devices and Systems I Spring 2019 Lecture Notes Note 17
EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive
More informationCorrelating EUV TMOKE and ARPES measurements to understand the temporal
Correlaing EUV TMOKE and ARPES measuremens o undersand he emporal and spaial lengh sales underlying ulrafas demagneizaion in ferromagnes Wenjing You 1, Phoebe Tengdin 1, Cong Chen 1, Xun Shi 1 *, Dmiriy
More informationHall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2
Page of 6 all effec Aim :- ) To deermine he all coefficien (R ) ) To measure he unknown magneic field (B ) and o compare i wih ha measured by he Gaussmeer (B ). Apparaus :- ) Gauss meer wih probe ) Elecromagne
More informationBUCKLING AND REDUCED STIFFNESS CRITERIA FOR FRP CYLINDRICAL SHELLS UNDER COMPRESSION
Asia-Paifi Conferene on FRP in Sruures (APFIS 7) S.T. Smih (ed) 7 Inernaional Insiue for FRP in Consruion BUCKLIG AD REDUCED STIFFESS CRITERIA FOR FRP CYLIDRICAL SHELLS UDER COMPRESSIO K. Masumoo 1, S.
More informationA comparative Study of Contact Problems Solution Based on the Penalty and Lagrange Multiplier Approaches
Journal of he Serbian Soiey for ompuaional Mehanis / Vol. / o., 2007 / pp. 74-83 A omparaive Sudy of ona Problems Soluion Based on he Penaly and Lagrange Muliplier Approahes S. Vulovi, M. Zivovi,. Grujovi,
More informationElectrical and current self-induction
Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of
More informationPolymer Engineering (MM3POE)
Polymer Engineering (MM3POE) VISCOELASTICITY hp://www.noingham.ac.uk/~eazacl/mm3poe Viscoelasiciy 1 Conens Wha is viscoelasiciy? Fundamenals Creep & creep recovery Sress relaxaion Modelling viscoelasic
More informationLecture 4 Kinetics of a particle Part 3: Impulse and Momentum
MEE Engineering Mechanics II Lecure 4 Lecure 4 Kineics of a paricle Par 3: Impulse and Momenum Linear impulse and momenum Saring from he equaion of moion for a paricle of mass m which is subjeced o an
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationMahgoub Transform Method for Solving Linear Fractional Differential Equations
Mahgoub Transform Mehod for Solving Linear Fraional Differenial Equaions A. Emimal Kanaga Puhpam 1,* and S. Karin Lydia 2 1* Assoiae Professor&Deparmen of Mahemais, Bishop Heber College Tiruhirappalli,
More informationComparing Means: t-tests for One Sample & Two Related Samples
Comparing Means: -Tess for One Sample & Two Relaed Samples Using he z-tes: Assumpions -Tess for One Sample & Two Relaed Samples The z-es (of a sample mean agains a populaion mean) is based on he assumpion
More informationVehicle Arrival Models : Headway
Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where
More informationA First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18
A Firs ourse on Kineics and Reacion Engineering lass 19 on Uni 18 Par I - hemical Reacions Par II - hemical Reacion Kineics Where We re Going Par III - hemical Reacion Engineering A. Ideal Reacors B. Perfecly
More informationSTRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN
Inernaional Journal of Applied Economerics and Quaniaive Sudies. Vol.1-3(004) STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN 001-004 OBARA, Takashi * Absrac The
More informationDevelopment of a new metrological model for measuring of the water surface evaporation Tovmach L. Tovmach Yr. Abstract Introduction
Developmen of a new merological model for measuring of he waer surface evaporaion Tovmach L. Tovmach Yr. Sae Hydrological Insiue 23 Second Line, 199053 S. Peersburg, Russian Federaion Telephone (812) 323
More informationTesting for a Single Factor Model in the Multivariate State Space Framework
esing for a Single Facor Model in he Mulivariae Sae Space Framework Chen C.-Y. M. Chiba and M. Kobayashi Inernaional Graduae School of Social Sciences Yokohama Naional Universiy Japan Faculy of Economics
More information20. Applications of the Genetic-Drift Model
0. Applicaions of he Geneic-Drif Model 1) Deermining he probabiliy of forming any paricular combinaion of genoypes in he nex generaion: Example: If he parenal allele frequencies are p 0 = 0.35 and q 0
More informationFrom a detailed model of porous catalytic washcoat to the effective model of entire catalytic monolith
Insiue of Chemial ehnology Prague Ceh Republi From a deailed model of porous aalyi washoa o he effeive model of enire aalyi monolih Per Kočí Vladimír Nová Franiše Šěpáne Miloš Mare Milan Kubíče hp://www.vsh./monolih
More informationAppendix to Creating Work Breaks From Available Idleness
Appendix o Creaing Work Breaks From Available Idleness Xu Sun and Ward Whi Deparmen of Indusrial Engineering and Operaions Research, Columbia Universiy, New York, NY, 127; {xs2235,ww24}@columbia.edu Sepember
More information2002 November 14 Exam III Physics 191
November 4 Exam III Physics 9 Physical onsans: Earh s free-fall acceleraion = g = 9.8 m/s ircle he leer of he single bes answer. quesion is worh poin Each 3. Four differen objecs wih masses: m = kg, m
More information