YIELD DISPLACEMENT ESTIMATES FOR DISPLACEMENT-BASED SEISMIC DESIGN OF DUCTILE REINFORCED CONCRETE STRUCTURAL WALL BUILDINGS
|
|
- Giles Underwood
- 6 years ago
- Views:
Transcription
1 3 th World Conerene on Earthqake Engineering Vanover, B.C., Canada Agst -6, 2004 Paper No. 035 YIELD DISPLACEMENT ESTIMATES FOR DISPLACEMENT-BASED SEISMIC DESIGN OF DUCTILE REINFORCED CONCRETE STRUCTURAL WALL BUILDINGS Tjen N. TJHIN, Mark A. ASCHHEIM, 2 and John W. WALLACE 3 SUMMARY This paper presents the reslts o an analtial std on ield rvatre or estimating eetive ield displaements or the design o dtile reinored onrete antilever strtral all bildings. Improved estimates o eetive ield rvatre ere obtained or retanglar and barbell ross setions based on standard moment rvatre analses. Variables onsidered inlde bondar and eb reinorement ratios, onrete ompressive and reinoring steel strengths, and axial load ratio. Formlas or estimating eetive ield rvatres and displaements are also presented, and an example is provided to illstrate the appliation o these estimates to the design o dtile reinored strtral all bildings. INTRODUCTION Ne displaement-based methods or seismi design [, 2, 3] rel on an estimate o the eetive ield displaement orresponding to the ndamental mode response o the strtre to be designed. The ield displaement is a relativel stable parameter that an be estimated based on kinemati relationships earl in the design proess, aonting or the strtral geometr, approximate distribtion o mass, material properties, and the nominal member dimensions o the strtral sstem []. In ontrast, onventional design approahes are based on the period o vibration, hih is prone to greater variation bease the stiness o the strtre is not knon initiall and tpiall ill var as the strengths o the strtral members are adjsted to obtain a strtre having the intended seismi perormane harateristis. The variation o the period ith hanges in strength tends to ase period-based seismi design approahes to reqire a larger nmber o iterations than are needed ith ield displaement approahes. Estimates o ield displaement sed or the design o dtile reinored onrete strtral all bildings are rrentl based on ield rvatre estimates that range beteen / l and / l or higher, here l is the length o the all in plan [4]. An analtial std as ndertaken in order to improve the preision o this estimate or retanglar setion and barbell setion alls having a large range o bondar and eb reinorement ratios, onrete ompressive strengths, and axial load ratios. This paper Gradate Researh Assistant, Universit o Illinois at Urbana-Champaign, Urbana, IL, USA 2 Assoiate Proessor, Santa Clara Universit, Santa Clara, CA, USA 3 Assoiate Proessor, Universit o Caliornia at Los Angeles, Los Angeles, CA, USA
2 presents the reslts o this analtial std on ield rvatre. Formlas or estimating eetive ield rvatres and displaements are presented together ith an example illstrating the appliation o these estimates to the design o dtile reinored onrete strtral all bildings. The disssion is limited to ll-height prismati antilever all sstems exhibiting dtile lexral response, or hih onl lexral deormations o the alls are onsidered. YIELD DISPLACEMENT OF DUCTILE REINFORCED CONCRETE WALLS Fig. (a) shos a tpial antilever all having height h and length l. Under lateral inertial ores (Fig. (b)), the roo displaement o this all at ield,, aonting or lexral deormations onl (Fig. ()) an be expressed b = κ h, () 2 here κ = ield displaement oeiient, and = eetive ield rvatre o the all ross setion at the base. The ield displaement oeiient, κ, depends on the rvatre distribtion along the height o the all (Fig. (e)), hih in trn depends on the lateral load distribtion and stiness distribtion over the all height. It also depends on seondar eets, sh as ondation rotation, shear distortion, and tension shit mehanism. The rvatre distribtion over the height o the all an be estimated sing simple beam theor as M ( x) / E I( x), here M (x) = moment at a setion loated x rom the base (Fig. (d)), and E I (x) = lexral rigidit at a setion loated x rom the base. n-th l i-th stor st V M h (a) Wall Elevation h e V (b) Lateral Fore Distribtion () Deleted Shape x Mx ( ) M (d) Moment Distribtion Fig. Response o a single all sstem at ield. (e) Idealized Crvatre Distribtion Vales o κ, ompted assming niorm E I(x) over the height o the all, niorm loor masses, niorm stor heights, and response in the ndamental mode, are given in Table. For irreglar all sstems, κ ma be determined b an elasti strtral analsis sing raked setion properties ith lateral ores applied in proportion to the ndamental mode shape amplitde and mass at eah loor. The eetive ield rvatre,, in Eq. () ideall orresponds to M / E I r, here M = eetive ield moment at the base o the all, and E I r = raked-setion lexral rigidit at the base o the all, rather than the instant hen the ield strain is reahed at the extreme tension reinorement. Varios estimates o the eetive ield rvatre,, have been proposed [e.g., 4, 5, 6], oten in the orm
3 κ =, (2) l here κ = eetive ield rvatre oeiient that depends primaril on the ross setional shape o the all, axial load level, and the amont, onigration, and ield strength o the longitdinal reinorement. Table Properties o Prismati Walls Responding in the Fndamental Mode n κ Γ α h e /h For retanglar ross setions, Wallae and Moehle [4] have reommended vales o κ in the range o to or Grade 60 (44 MPa) steel, or tpial levels o axial load and reinorement ratio. Vales or other ross setions have also been sggested b other researhers [e.g., 5, 6]. More generall, κ an be obtained rom a moment-rvatre analsis b linearl extrapolating the ield rvatre orresponding to the irst ield o longitdinal reinorement to the eetive ield moment, M, hih is the moment resistane orresponding to a predetermined rvatre, as illstrated in Fig. 2. The predetermined rvatre old orrespond to the development o the nominal lexral strength, as determined sing bilding odes sh as ACI-38 [7]. Moment, M EI r M M First Yield Point Predetermined Crvatre Crvatre, Fig. 2 General deinition o eetive ield rvatres. ESTIMATES OF EFFECTIVE YIELD CURVATURES Methodolog An analtial std as ondted to improve the preision o eetive ield rvatre estimates or retanglar and barbell all ross setions (Fig. 3(a)). Variables onsidered inlde axial load level, longitdinal bondar reinorement ratios, longitdinal eb reinorement ratio, speiied onrete
4 ompressive strength, and speiied steel reinorement ield strength. Common ranges o variables ere seleted or the std, as smmarized in Table 2. t ρt l 2d ρt l t l kd ε Paraboli Shape ρ t ρt l 2d l ρ t ρt l t l Centroid o Tension Steel d Gross-Setion Centroid (a) Idealized Cross Setions ε (b) Assmed Strain Proile at First Yield () Assmed Conrete Stress Distribtion at First Yield Fig. 3 Idealization and assmptions sed or determining eetive ield rvatres. Table 2 Smmar o the Variables Used ( ksi = MPa) Parameter Vale Cross Setion Retanglar, Barbell End (Bondar) Longitdinal Steel Ratio, ρ Retanglar: 0.25%, 0.5%, %, 2%, 3% Barbell: %, 2%, 3%, 4%, 5% Web Reinoring Steel Ratio, ρ" 0.25%, 0.3%, 0.4%, 0.5% Speiied Compressive Strength o Conrete, (ksi) 4, 5, 6 Speiied Yield Strength o Reinoring Steel, (ksi) 40, 60, 75 Axial Load Ratio, P/( A ) 0 to 0.2 Normalized Centroid o Bondar Reinorement, d/l 0.05, 0., 0.5 Normalized Flange Thikness, t /t (or Barbell onl) 2 Normalized Flange Depth, l /t (or Barbell onl),.5, 2 The eetive ield rvatre estimates ere determined sing standard moment-rvatre analses satising strain ompatibilit, material stress-strain relationships, and eqilibrim. The longitdinal bondar reinorement as assmed to be lmped at its entroid, and the longitdinal eb reinorement as assmed to be niorml distribted as a thin sheet (Fig. 3(a)). For barbell setions, the entroid o bondar reinorement oinides ith the entroid o the bondar region. The strain distribtion as assmed to be linear aross the setion (Fig. 3(b)). The stress-strain rve or onrete in ompression as assmed to be paraboli (Figs. 3() or 4(a)). The modls o elastiit o onrete in ompression, E, as 57,000 (in psi), as deined in ACI [7]. This modls is a seant modls representing the slope o line passing throgh the onrete stressstrain rve at 0.45, as illstrated in Fig. 4(a). The strain at the instant that the stress reahes, denoted ε, that orresponds to this deinition is , , and or eqal to 4, 5, and 6 ksi (28, 35, 42 MPa), respetivel. The onrete tensile strength as negleted. An elasto-plasti stress-
5 strain rve as sed or reinoring steel in both ompression and tension (Fig. 4(b)). The modls o elastiit o the steel, E, as taken as 29,000 ksi (200,000 MPa). s Conrete Stress, E ε = 2 ε - ε 2 ε Steel Stress, s E s 0.45 Note: No tension properties Note: Tension and ompression are deined properties are the same 0 ε Conrete Strain, ε E ε Steel Strain, ε s (a) Conrete (b) Reinoring Steel Fig. 4 Stress-strain relationships or onrete and reinoring steel sed in this std. The irst-ield rvatre,, as established based on the strain ondition shon in Fig. 3(b) as ε + ε =, () d here ε = / Es = steel ield strain, ε = onrete strain at the extreme ompression iber at the time longitdinal bondar reinorement strain reahes ε, and d = the distane rom the extreme onrete ompression iber to the entroid o the bondar reinorement. For higher axial load levels, the steel ield strain, ε, ma or at a ver high vale o ε. For these ases, the irst-ield rvatre is deined as rvatre orresponding to ε, i.e., the strain at the time the stress reahes. The eetive ield rvatre,, as obtained rom extrapolating the irst-ield rvatre to a point here the moment reahes ltimate strength, M, assming elasto-plasti response (Fig. 5), or M =, (2) M here M = moment resistane hen longitdinal bondar reinorement strain reahes ε. The ltimate lexral strength, M, is deined as the moment resistane orresponding to a onrete strain o at the extreme ompression iber.
6 Moment, M M EI r Idealized Observed M Eetive Yield Point First Yield Point Crvatre, Fig. 5 Deinition o eetive ield rvatres sed in this std. Reslts Charts ere generated to allo the eetive ield rvatre o retanglar and barbell all ross setions to be estimated diretl. Eah hart plots the ield rvatre oeiient as a ntion o the axial load level in a dimensionless orm or a nmber o longitdinal bondar reinorement ratios, a speiied longitdinal eb reinorement ratio, speiied onrete ompressive strength, and steel reinorement ield strength. Tpial harts are given in Fig. 6 or both retanglar and barbell ross setions. Given the ross setional shape, the axial load level, the longitdinal bondar reinorement ratio, ρ, and the longitdinal eb reinorement ratio, ρ ", the eetive ield rvatre oeiient an be interpolated beteen the rves. From the moment-rvatre analses, it is observed that eetive ield rvatre is nearl insensitive to onrete strength and eb reinorement ratio. It is also observed that both the retanglar and barbell ross setions exhibit similar reslts or the range o vales overed in the std. At earl stage o the design proess, the bondar and eb steel reinorement steel is sall not knon et. For design prposes, it is thereore pratial to deine eetive ield rvatre as a ntion o axial load level and steel reinorement grade; at a later stage the neessit o a onined bondar element an be addressed. The eetive ield rvatre oeiient or retanglar or barbell ross setions ma be estimated ith the olloing ormla ith errors tpiall less than 5 to 0%: P κ =.8ε (5) A It shold be noted that Eq. (5) is valid or ases here the axial load ratio, P /( A ), is not more than 0.2. In addition, Eq. (5) is appliable or barbell ross setions in hih l / t 2 and t / t 2. The same eqation proposed or both the retanglar and barbell ross setions provides lexibilit in satising the detailing reqirements or speial transverse bondar reinorement presribed in the perormane objetives or reqired b ode strain ompatibilit analsis provisions.
7 Yield Crvatre Coeiient, κ = l d = 0.05l, ρ = 0.25% = 4 ksi, = 40 ksi t tl 2d Yield Crvatre Coeiient, κ = l t = 2t, l = t, d = 0.05l, ρ = 0.25% = 4 ksi, = 40 ksi tl t l ρ = 0.25% ρ = 0.5% ρ = % ρ = 2% ρ = 3% Axial Load Level, P /( A ) t tl 2d l ρ = % ρ = 2% ρ = 3% ρ = 4% ρ = 5% Axial Load Level, P /( A ) t tl t l Yield Crvatre Coeiient, κ = l d = 0.05l, ρ = 0.25% = 5 ksi, = 60 ksi t tl 2d Yield Crvatre Coeiient, κ = l t = 2t, l = t, d = 0.05l, ρ = 0.25% = 5 ksi, = 60 ksi tl t l t ρ = 0.25% ρ = 0.5% ρ = % ρ = 2% ρ = 3% Axial Load Level, P /( A ) t tl 2d l ρ = % ρ = 2% ρ = 3% ρ = 4% ρ = 5% Axial Load Level, P /( A ) t tl l Yield Crvatre Coeiient, κ = l d = 0.05l, ρ = 0.25% = 6 ksi, = 75 ksi t tl 2d Yield Crvatre Coeiient, κ = l t = 2t, l = t, d = 0.05l, ρ = 0.25% = 6 ksi, = 75 ksi tl t l t ρ = 0.25% ρ = 0.5% ρ = % ρ = 2% ρ = 3% Axial Load Level, P /( A ) t tl 2d l ρ = % ρ = 2% ρ = 3% ρ = 4% ρ = 5% Axial Load Level, P /( A ) t tl l Fig. 6 Tpial harts o eetive ield rvatre oeiients ( ksi = MPa). APPLICATION TO DESIGN APPROACHES BASED ON YIELD DISPLACEMENT ESDOF Sstem or Approximating Dnami Response o Strtres Eqivalent Single-Degree-o-Freedom (ESDOF) representations have been sed in seismi evalation proedres, sh as the displaement oeiient and apait spetrm methods [8, 9], to estimate inelasti seismi demands o the strtre nder onsideration. In these proedres, the response o a mlti-degree-o-reedom (MDOF) model o the strtre is assmed to be predominantl in a single deleted shape throghot the response histor. ESDOF representations have also reentl been
8 emploed or determining the reqired strength and stiness to limit the maximm displaement response to a desired vale. The latter se ill be demonstrated b a design example presented in the next setion. Fig. 7 smmarizes an ESDOF ormlation adapted rom ATC-40 [8]. This ormlation ses the elasti irst mode shape onsidering raked-setion lexral stiness properties, reslting in a math beteen the ndamental period o the all sstem, T, assoiated ith the raked setion stiness, k, (Fig. 7(a)) and the initial period o the ESDOF model, T. Also, the height o the lateral ore resltant o the MDOF sstem, h e, is the same as the eetive height o the ESDOF sstem. m n n = m= m i Σ i = h he i k n m i i Base Shear, V Base Shear, V k Idealized V = C W V = W Observed m C k T = T = 2π W= n Σ i = m i g C g = C C α W = m g = µ µ = = Roo Displaement, Γ Displaement, (a) MDOF Sstem (b) ESDOF Sstem Fig. 7 Idealized load-deormation responses o a all sstem and the ESDOF sstem. As indiated in Fig. 7, the relationship beteen the roo displaement o a MDOF model o the all sstem at ield,, and the ield displaement o the orresponding ESDOF sstem,, is given as =, (6) Γ here Γ = the irst mode partiipation ator, allated ith the mode shape normalized sh that the mode shape amplitde at the roo, n, is eqal to one. The base shears o the ESDOF sstem, V, and the MDOF sstem, V, at ield are related b V V, (7) = α
9 here α is the irst mode eetive mass oeiient. Normalizing Eq. (7) b the orresponding eights o the sstems gives C C, (8) = α here C = shear oeiient o the MDOF sstem. V / W = the ield strength oeiient o the ESDOF sstem and C = V / W = the base For bildings onsisting o prismati alls having niorm stor heights and niorm loor masses and responding in lexre onl, Γ, α, and h e have the vales given in Table. For other ases, the vales o these terms an be determined sing standard ormlas. While not reqired or design, the period o vibration o the all sstem oten is o interest. Corresponding to raked-setion stiness o the all sstem, k, as deined in Fig. 7(a), this period ma be allated based on the properties o the ESDOF sstem as T = T = 2π. (9) C g The displaement response and peak drit o an ESDOF sstem,, sbjeted to grond motion exitation ma be estimated sing a dnami analsis sing a simpliied hstereti model. For slender reinored onrete strtral all bildings, an elasto-plasti model ith stiness degradation oten is siientl arate. For ases here onl smoothed ode spetra are available, the peak drit demand ma be estimated sing a sitable R-µ -T relationship developed or stiness-degrading osillators. Given the ESDOF drit estimate, the roo drit o the all sstem an be estimated as = Γ implies that the displaement dtilit o the ESDOF and MDOF sstems is eqal and is given as. This µ = =. (0) Yield Point Spetra or Estimating Seismi Demands and Reqired Lateral Strengths Yield Point Spetra (YPS) [0] plot rves o onstant displaement dtilit on the axes o ield strength oeiient and ield displaement, or SDOF osillators having a range o initial (elasti) periods o vibration, a speiied hstereti propert, and a speiied level o visos damping (Fig. 8). An one point on a YPS plot represents or qantities:, C, T, and µ. The irst three o these qantities are related aording to Eq. (9). Frthermore, knoledge o the ESDOF dtilit, µ, allos the peak displaements, and, to be estimated sing Eq. (0). YPS ma diretl be ompted or speii grond motion reords or estimated b appling previosl established R-µ -T relationships to elasti design response spetra. YPS ma be sed to estimate the peak displaement response o a SDOF sstem (or an ESDOF sstem) having a knon ield point. YPS ma also be sed or an inverse proess, i.e., to determine the ield point
10 or a ne design or to determine the level o strengthening and stiening reqired to rehabilitate an existing strtre to have aeptable seismi perormane. The inverse proess, or determining aeptable ield points or a desired perormane, is shematiall illstrated in Fig. 8. Yield Strength Coeiient, C µ = µ o T = 2π C o µ o = o o (given) o µ = µ = 4 µ = 2 µ = o (given) Yield Displaement, (mm) o o C o g Fig. 8 Example o YPS and its se or estimating ield strength oeiient (25.4 mm = in.). Design Example Bilding Desription The design o to barbell alls in an eight-stor strtral all bilding is presented to illstrate the se o the estimated ield displaement in design. To idential barbell setion alls are sed as the lateral load arring sstem or the N-S diretion, as indiated in Fig. 9. All loor-to-loor heights are 2 t (3.65 m). The onrete ompressive strength,, and the reinoring steel ield strength,, are 5 ksi (35 MPa) and 60 ksi (44 MPa), respetivel. Floor dead and live loads are 75 ps (8.4 kn/m 2 ) and 50 ps (2.4 kn/m 2 ), respetivel. The axial load at the base o the alls as estimated to be 0.5 A. Seismi eight, W, as assmed to ome rom the dead load onl, hih is 8(75 ps)(80 t)(60 t) = 5,20 kips (67,254 kn). 24 t (7.32 m) W 4 in. (356 mm) W 60 t (8.3 m) N 80 t (54.9 m) Fig. Tpial loor o the design example. Design Perormane Objetive The N-S diretion as designed to satis a lie saet perormane objetive, hih is somehat arbitraril assoiated ith a peak roo displaement limit eqal to 0.83% o the height o the bilding. The design earthqake assoiated ith this perormane objetive is represented b the smoothed elasti design spetrm shon in Fig. 0(a). This spetrm has the olloing parameters per IBC 2000 [] terminolog: T = 0.40 se, T o = 0. 2T = 0.08 se, S Ds = g, and S D = g. The simple R-µ -T s
11 relationships shon in Fig. 0(b) are sed to derive inelasti seismi demands rom the design spetrm. Onl translational response is onsidered in this design; the potential eets o aidental eentriit and rotational omponents o the grond motion on torsional response are negleted. Spetral Psedo Aeleration, S pa (g ) S DS = 0.937g 0.8 Response Modiiation Fator, R 0 8 µ = T o = 0.08 se T s = 0.40 se S DS = 0.377g T s = 0.40 se µ = 4 µ = 2 µ = Period, T (se) (a) Design Spetrm Period, T (se) (b) R-µ-T Relationships Fig. 0 Design spetrm and R-µ -T relationships sed in the design example. Design Callations The design approah desribed in the previos setions is sed to determine the seismi demand and reqired base shear or determining the reqired lexral strength at the base o eah all. For brevit, onl allations or reqired base shear and base moment o the alls are presented. The distribtion o lateral ores over the height o the bilding and to eah all at eah loor level ma ollo ode or other established proedres [e.g., 6, 2]. The reqired shear and moment apaities over the height o eah all shold be determined onsidering higher mode eets sing an o several established proedres [e.g., 3-6]. The eetive ield rvatre oeiient or the alls is estimated sing Eq. (5), as.8(60 ksi/29,000 ksi) (0.5) = B Eq. (2), the estimated ield rvatre is /(24 t) = rad/in. ( rad/mm). For an eight-stor bilding, the estimated ield displaement oeiient, κ, is aording to Table. Using Eq. (), the ield displaement,, is 0.295( rad/in.)(96 t) 2 = 6.0 in. (52 mm). Based on the design perormane objetive, the roo displaement limit,, is (0.83%)(96 t) = 9.6 in. (244 mm). Ths, the displaement dtilit limit, µ, is 9.6/6.0 =.6. From Table, the modal partiipation ator, Γ, mass oeiient, α, and eetive height, h e, or an eight-stor bilding are.445, 0.653, and 0.770, respetivel. The ESDOF displaement,, is (6.0 in.)/.445 = 4.5 in. (05 mm). The YPS or this design are shon in Fig., established b appling R-µ -T relationships to the design spetrm. The minimm ield strength oeiient, C, or µ =.6 and = 4.5 in. is obtained rom YPS as 0.3 (Fig. ). B Eq. (8), the reqired base shear oeiient, C, is 0.653(0.3) = Thereore, the base shear o the bilding is (5,20 kips) = 293 kips (5752 kn), the reqired base
12 shear o eah all is (293 kips)/2 = 646 kips (2876 kn), and the reqired moment at the base o eah all is 0.770(293 kips)(96 t)/2 = 47,790 k-t (64,790 kn-m). Yield Strength Coeiient, C C = 0.3 µ = 0. = 4.5 in. µ = µ = 2 µ = 4 µ = Yield Displaement, (in.) Fig. 2 YPS or the design example ( in. = 25.4 mm). CONCLUSION Improved estimates o eetive ield rvatre or retanglar and barbell ross setions ere presented or se in design o dtile reinored onrete antilever strtral alls. These estimates ere derived based on onsistent standard moment rvatre analses overing variation in bondar reinorement, eb reinorement, steel reinorement ield strength, onrete ompressive strength, axial load ratio, relative dimensions o the ross setion. A set o harts as developed to allo the eetive ield rvatre to be estimated diretl. Simple expression derived in terms o parameters sall knon at the earl design stage axial load and steel reinorement grade as also presented. A design example based on eqivalent single-degree-o reedom in onjntion ith Yield Point Spetra as provided to illstrate the appliation o these estimates to the design o dtile reinored strtral all bildings. REFERENCES. Ashheim, M. A., Blak, E. F. Yield point spetra or seismi design and rehabilitation, Earthqake Spetra, EERI, 2000; 6(2): Ashheim, M. A. The prima o the ield displaement in seismi design. Seond US-Japan Workshop on Perormane Based Design o Reinored Conrete Bildings, Sapporo, Japan, September 0-2, Pala, T. A displaement-osed seismi design o mixed bilding sstems. Earthqake Spetra, 2002; 8(4): Wallae, J. W., Moehle, J. P. Dtilit and detailing reqirements o bearing all bildings. Jornal o Strtral Engineering, 992; 8(6): Priestle, M. J. N., Koalsk, M. J. (998). Aspets o drit and dtilit apait o retanglar antilever strtral alls. Blletin o the Ne Zealand National Soiet or Earthqake Engineering, 998; 3(2): Pala, T. An estimation o displaement limits or dtile sstems. Earthqake Engineering and Strtral Dnamis, 2002; 3(3): ACI Committee 38. Bilding ode reqirements or strtral onrete (ACI 38-02) and ommentar (ACI 38R-02). Amerian Conrete Institte, Farmington Hills, MI, 2002.
13 8. ATC-40. Seismi evalation and retroit o onrete bildings. Applied Tehnolog Conil, Redood Cit, CA, FEMA 273. NEHRP gidelines or the seismi rehabilitation o bildings. Report No. FEMA 273, Federal Emergen Management Agen, Washington, DC, Ashheim, M. A., Blak, E. F. Yield point spetra or seismi design and rehabilitation. Earthqake Spetra, 2000; 6(2): International Conerene o Bilding Oiials (ICBO). International bilding ode. Whittier, CA, Tjhin, T. N., M. A. Ashheim, Wallae, J. W. Perormane-based seismi design o dtile reinored onrete all bildings. Report (nder revie), Universit o Illinois at Urbana- Champaign, Urbana, IL, Pala, T. The design o dtile reinored onrete strtral alls or earthqake resistane. Earthqake Spetra, EERI, 986; 2(4): Eberhard, M. O., Sozen, M. A. A behavior-based method to determine design shear in earthqakeresistant alls. Jornal o Strtral Engineering, ASCE, 993; 9(2): ACI Committee 368. Drat ommittee report: reommendations or proportion and design o reinored onrete sstems and elements. Amerian Conrete Institte, Detroit, MI, Ashheim, M., Tjhin, T., Comartin, C., Hambrger, R., Inel, M. The saled nonlinear dnami proedre. ASCE Strtres Congress, Nashville, TN, Ma 22-26, NOTATION A s = Area o longitdinal bondar (end) reinorement o a all. A = Cross setion area o a all. C = Base shear strength o a all or a all sstem, V, normalized b its seismi eight, W (sall termed base shear strength oeiient). C = Yield strength oeiient o the ESDOF model o a all sstem. d = Distane rom the extreme ompression iber to the entroid o longitdinal bondar reinorement. d = Distane rom the extreme onrete iber to the entroid o longitdinal bondar reinorement. E I(x) = Flexral rigidit at a all setion loated at a distane x rom the base. E I r = raked-setion lexral stiness at the base. E = Modls o elastiit o steel reinorement. g s = Conrete ompressive stress hen the extreme ompression iber reahes ε. = Speiied ompressive strength o onrete. = Speiied ield strength o longitdinal reinorement. = Aeleration o gravit. h e = Resltant o lateral ores measred rom the base o a all sstem (sall termed eetive h k height). = Total height o a all or a all sstem. = Lateral elasti raked-setion stiness o a all or a all sstem in elasti region hen sbjeted to a lateral ore distribtion proportional to the prodt o the ndamental mode shape amplitde and loor mass at eah loor.
14 k d = Netral axis or ompression zone depth o a all ross setion at ield. k = Lateral stiness o the ESDOF model o a all sstem. l = Depth o the bondar part o a bar-bell all ross setion. This dimension is parallel to the horizontal length, l. l = Horizontal length o a all. m i = Lmped mass o the i-th loor o an n-stor bilding. m = Seismi mass o the ESDOF model o a all sstem. M = Moment resistane orresponding to eetive ield rvatre o a all setion at the base,. M M = Moment resistane orresponding to irst-ield rvatre o a all setion at the base,. = Moment resistane orresponding to a onrete strain o at the extreme ompression iber. M (x) = Moment o a all at a setion loated at a distane x rom the all base. n = Nmber o stories. P = Axial load o a all. R = Ratio o the elasti strength demand to the ield strength oeiient (also knon as response modiiation oeiient in IBC 2000 []). S = Design spetral psedo aeleration at se period (parameter in IBC 2000 []). D S = Design spetral aeleration at short periods (parameter in IBC 2000 []). DS t = Thikness o the bondar o a bar-bell all ross setion. This dimension is parallel to the eb thikness, t. t = Web thikness o a all. T = First mode period o vibration o a all sstem in the design diretion based on rakedsetion stiness, k. T = Period o vibration o an ESDOF model o a all sstem. T s = harateristi period (parameter in IBC 2000 []). T o = 0.2T s (parameter in IBC 2000 []). V = Lateral base shear o a all or all sstem at ield hen sbjeted to a lateral ore distribtion proportional to the prodt o the ndamental mode shape amplitde and loor mass at eah loor (also termed base shear strength). V = Yield strength o the ESDOF model o a all sstem. W = Seismi eight o a all sstem. W = Seismi eight o the ESDOF model o a all sstem. x = Vertial distane o a all ross setion, measred rom the all base. α = First mode eetive mass oeiient. = Lateral roo displaement o a all or a all sstem at ield hen sbjeted to a lateral ore distribtion proportional to the prodt o the ndamental mode shape amplitde and loor mass at eah loor. = Lateral displaement o the ESDOF model o a all sstem at ield. = Maximm lateral roo displaement (also knon as peak drit) o a all sstem at ltimate. = Maximm lateral displaement o the ESDOF model o a all sstem.
15 ε = Conrete strain at the extreme ompression iber hen longitdinal bondar reinorement strain reahes ε. ε ε i κ = Yield strain o longitdinal reinorement. = Strain orresponding to peak stress,, in a niaxial stress-strain rve o onrete. = First mode shape amplitde at the i-th loor o an n-stor bilding. = First-ield rvatre o a all setion at the base. = Eetive ield rvatre o a all setion at the base. = Yield displaement oeiient o a all. κ = Yield rvatre oeiient o a all. Γ = First mode modal partiipation ator. µ = Displaement dtilit ator o a all or all sstem. ρ = Ratio o longitdinal bondar reinorement o a all = A s /( tl). " " ρ = Ratio o longitdinal eb reinorement o a all = A /( t l ). APPENDIX s Table Conversion Fators rom U.S. Cstomar to SI Units To Convert To Mltipl b inh (in.) millimeter (mm) 25.4 oot (t) meter (m) kilopond ore (kip or k) kiloneton (kn) kilopond ore per sqare inh (ksi) megapasal (MPa) pond per sqare oot (ps) megapasal (MPa) 47.88
Horizontal Distribution of Forces to Individual Shear Walls
Horizontal Distribtion of Fores to ndividal Shear Walls nteration of Shear Walls ith Eah Other n the shon figre the slabs at as horizontal diaphragms etending beteen antilever alls and the are epeted to
More informationProbabilistic Models for Seismic Design and Assessment of RC Structural Walls
robabilisti Models for Seismi Design and Assessment of RC Strtral Walls Abstrat Mehrdad Sasani Northeastern Universit Boston, Massahsetts robabilisti models for estimating lateral flexral displaement apait,
More informationSEISMIC EVALUATION AND ITS VERIFICATION OF STREET BUILDINGS IN TAIWAN
13 th World Conerene on Earthqake Engineering Vanover, B.C., Canada Agst 1-6, 2004 Paper No. 2747 SEISMIC EVALUATION AND ITS VERIFICATION OF STREET BUILDINGS IN TAIWAN Maw-Shyong SHEU 1, Tetso, KUBO 2,
More informationCalculation of slab-column middle connection under combined shear and unbalanced moment
Callation o slab-olmn middle onnetion nder ombined shear and nbalaned moment Ha Li 1, a, Nan Go 2,b, Yiing Lin 3, 1,2,3 College o Civil Engineering, Northeast Forestr Universit, Harbin 154 China a liha7515@163.om,
More informationThe Hashemite University Department of Civil Engineering ( ) Dr. Hazim Dwairi 1
Department of Civil Engineering Letre 8 Slender Colmns Definition of Slender Colmn When the eentri loads P are applied, the olmn deflets laterally by amont δ,, however the internal moment at midheight:
More informationPurpose of reinforcement P/2 P/2 P/2 P/2
Department o Civil Engineering Purpose o reinorement Consider a simpl supported beam: P/2 P/2 3 1 2 P/2 P/2 3 2 1 1 Purpose o Reinorement Steel reinorement is primaril use beause o the nature o onrete
More informationSoftware Verification
AISC-360-10 Example 001 COMPOSITE GIRDER DESIGN EXAMPLE DESCRIPTION A typial bay of a omposite floor system is illstrated below. Selet an appropriate ASTM A992 W-shaped beam and determine the reqired nmber
More informationCase Study in Reinforced Concrete adapted from Simplified Design of Concrete Structures, James Ambrose, 7 th ed.
ARCH 631 Note Set 11 F013abn Case Stdy Refored Conrete adapted from Simplified Design of Conrete Strtres, James Ambrose, 7 th ed. Bildg desription The bildg is a three-story offie bildg tended for spelative
More informationINFORMATION CONCERNING MATERIALS TO BE USED IN THE DESIGN
TITLE 5 DESIGN CHAPTER 8 INFORMATION CONCERNING MATERIALS TO BE USED IN THE DESIGN Artile 38. Charateristis o steel or reinorements 38.1 General The harateristis o the steel used or the design desribed
More informationCase Study in Reinforced Concrete adapted from Simplified Design of Concrete Structures, James Ambrose, 7 th ed.
ARCH 631 Note Set 11 F015abn Case Study in Reinfored Conrete adapted from Simplified Design of Conrete Strutures, James Ambrose, 7 th ed. Building desription The building is a three-story offie building
More informationThe Design of Special Truss Moment Frames Against Progressive Collapse
Paper 24 The Design of Speial Trss oment Frames Against Progressie Collapse H.K. Kang, J.Y. Park and J.K. Kim Department of Arhitetral Engineering Sngkynkwan Uniersity, Swon, Korea Ciil-Comp Press, 2012
More informationDesign resistance of steel expansion anchors under shear loading derived using methods of design assisted by testing
Design resistane of steel expansion anhors nder shear loading derived sing methods of design assisted by testing MACELA KAMAZÍNOÁ Falty of Civil Engineering Brno University of Tehnology eveří St. 331/95,
More informationUltimate Strength Evaluation for Wide-Type Box Girders in Cable-Supported Bridges
Ultimate Strength Evalation for Wide-Tpe Box Girders in Cable-Spported Bridges Jong Seo KIM Ph.D. Candidate Seol National Universit Seol,Korea (OK) jskim99@sn.a.kr Jong Seo Kim, born 1980, is a Ph.D andidate
More informationDesign of AAC floor slabs according to EN 12602
Design of AAC floor slabs aording to EN 160 Example 1: Floor slab with uniform load 1.1 Issue Design of a floor slab under a living room Materials Component with a ompressive strength lass AAC 4,5, densit
More informationBEAMS: SHEARING STRESS
LECTURE Third Edition BEAMS: SHEARNG STRESS A. J. Clark Shool of Engineering Department of Civil and Environmental Engineering 14 Chapter 6.1 6.4 b Dr. brahim A. Assakkaf SPRNG 200 ENES 220 Mehanis of
More informationVirtual Work for Frames. Virtual Work for Frames. Virtual Work for Frames. Virtual Work for Frames. Virtual Work for Frames. Virtual Work for Frames
IL 32 /9 ppling the virtual work equations to a frame struture is as simple as separating the frame into a series of beams and summing the virtual work for eah setion. In addition, when evaluating the
More informationf 2 f n where m is the total mass of the object. Expression (6a) is plotted in Figure 8 for several values of damping ( ).
F o F o / k A = = 6 k 1 + 1 + n r n n n RESONANCE It is seen in Figure 7 that displaement and stress levels tend to build up greatly when the oring requeny oinides with the natural requeny, the buildup
More informationCh. 10 Design of Short Columns Subject to Axial Load and Bending
Ch. 10 Design o Short Columns Subjet to Axial Load and Bending Axial Loading and Bending Development o Interation Diagram Column Design Using P-M Interation Diagram Shear in Columns Biaxial Bending Examples
More informationEXPERIMENTAL AND NUMERICAL STUDY OF DEBONDING IN COMPOSITE ADHESIVE JOINTS
6 TH NTERNATONAL CONFERENCE ON COMPOSTE MATERALS EXPERMENTAL AND NUMERCAL STUDY OF DEBONDN N COMPOSTE ADHESVE JONTS Rosen T. Tenhev, Brian. Falzon mperial College, London, UK Keywords: interfae elements,
More informationSlenderness Effects for Concrete Columns in Sway Frame - Moment Magnification Method
Slenderness Effets for Conrete Columns in Sway Frame - Moment Magnifiation Method Slender Conrete Column Design in Sway Frame Buildings Evaluate slenderness effet for olumns in a sway frame multistory
More information1 Differential Equations for Solid Mechanics
1 Differential Eqations for Solid Mechanics Simple problems involving homogeneos stress states have been considered so far, wherein the stress is the same throghot the component nder std. An eception to
More informationSlenderness Effects for Concrete Columns in Sway Frame - Moment Magnification Method
Slenderness Effets for Conrete Columns in Sway Frame - Moment Magnifiation Method Slender Conrete Column Design in Sway Frame Buildings Evaluate slenderness effet for olumns in a sway frame multistory
More informationCEN/TC 250/SC 3 N 2634
CEN/TC 50/SC N 64 CEN/TC 50/SC Euroode - Design o steel strutures E-mail o Seretar: susan.kempa@din.de Seretariat: DIN EN 99--5 First Drat Date o doument 08-05-0 Expeted ation Comment Due Date 08-06-9
More informationSCHOOL OF MECHANICAL, AEROSPACE AND CIVIL ENGINEERING HYDRAULICS 2 LABORATORY EXERCISE. Forces on Two-Dimensional Bodies in a Wind Tunnel
Objet SCHOOL OF MECHANICAL, AEROSPACE AND CIVIL ENGINEERING HYDRAULICS LABORATORY EXERCISE Fores on Two-Dimensional Bodies in a Wind Tnnel To ompare drag oeffiients made by diret measrement on a drag balane
More informationCompatibility of the theory of special relativity with an absolute reference frame with a longitudinal Doppler shift
Compatibility o the theory o speial relatiity with an absolte reerene rame with a longitdinal Doppler shit Masanori ato Honda Eletronis Co., Ltd., Oyamazka, Oiwa-ho, Toyohashi, ihi 44-33, Japan bstrat:
More informationCROSS-CORRELATION OF FLUCTUATING COMPONENTS OF WIND SPEED BASED ON STRONG WIND MEASUREMENT
The Seventh Asia-Paifi Conferene on Wind Engineering, November 8-12, 29, Taipei, Taian COSS-COELATION OF FLUCTUATING COMPONENTS OF WIND SPEED BASED ON STONG WIND MEASUEMENT Maymi Fjimra 1 and Jnji Maeda
More informationReinforced Concrete Design
Reinored Conrete Design Notation: a = depth o the eetive ompression blok in a onrete beam A g = gross area, equal to the total area ignoring any reinorement A s = area o steel reinorement in onrete beam
More informationRC DEEP BEAMS ANALYSIS CONSIDERING LOCALIZATION IN COMPRESSION
RC DEEP BEAMS ANAYSIS CONSIDERING OCAIZATION IN COMPRESSION Manakan ERTSAMATTIYAKU* 1, Torsak ERTSRISAKURAT* 1, Tomohiro MIKI* 1 and Junihiro NIWA* ABSTRACT: It has been found that RC deep beams usually
More informationBrick masonry infills in seismic design of RC frame buildings: Part 2 Behaviour
Brik asonry inills in seisi design o RC rae ildings: Part Behavior Diptesh Das and C.V.R. Mrty on-linear pshover analysis was perored on ive RC rae ildings with rik asonry inills, designed or the sae seisi
More informationAn Analytical Formulation of Stress-Block Parameters for Confined Concrete
The Open Constrution and Building Tehnology Journal, 8,, 37-8 37 Open Aess An Analytial Formulation o Stress-Blok Parameters or Conined Conrete Frano Braga, Rosario Gigliotti, Mihelangelo Laterza* and
More informationOUTLINE. CHAPTER 7: Flexural Members. Types of beams. Types of loads. Concentrated load Distributed load. Moment
OUTLINE CHTER 7: Fleural embers -Tpes of beams, loads and reations -Shear fores and bending moments -Shear fore and bending - -The fleure formula -The elasti urve -Slope and defletion b diret integration
More informationShear-Friction Strength of RC Walls with 550 MPa Bars
Proeedings of the Tenth Paifi Conferene on Earthquake Engineering Building an Earthquake-Resilient Paifi 6-8 November 215, Sydney, Australia Shear-Frition Strength of RC Walls with 55 MPa Bars Jang-woon
More informationUniaxial Concrete Material Behavior
COMPUTERS AND STRUCTURES, INC., JULY 215 TECHNICAL NOTE MODIFIED DARWIN-PECKNOLD 2-D REINFORCED CONCRETE MATERIAL MODEL Overview This tehnial note desribes the Modified Darwin-Peknold reinfored onrete
More informationSoftware Verification
Sotare Veriiation EXAMPLE NZS 3101-06 RC-BM-001 Flexural and Shear Beam Deign PROBLEM DESCRIPTION The purpoe o thi example i to veriy lab lexural deign in. The load level i adjuted or the ae orreponding
More informationDrift Capacity of Lightly Reinforced Concrete Columns
Australian Earthquake Engineering Soiety Conferene, Perth, Western Australia Drift Capaity of ightly Reinfored Conrete Columns A Wibowo, J Wilson, NTK am, EF Gad,, M Fardipour, K Rodsin, P ukkunaprasit
More informationThe degree of slenderness in a column is expressed in terms of "slenderness ratio," defined below:
Chapter 4 Desin of Colmns By rat Saatiol 1 4.1 Introdtion The majority of reinfored onrete olmns in pratie are sbjeted to very little seondary stresses assoiated with olmn deformations. These olmns are
More informationThe Design of Fiber Reinforced Polymers for Structural Strengthening An Overview of ACI 440 Guidelines. Sarah Witt Fyfe Company November 7, 2008
The Design o Fiber Reinored Polymers or Strutural Strengthening An Overview o ACI 440 Guidelines Sarah Witt Fye Company November 7, 2008 1 GUIDE FOR THE DESIGN AND CONSTRUCTION OF EXTERNALLY BONDED FRP
More informationImproved Characterization Model for Granular Bases
128 TRANSPORTATON RESEARCH RECORD 1227 mproved Charateriation Model for Granlar Bases ROBERT P. ELLOTT AND LOURDESNATHAN DAVD Laboratory resilient modls tests ere ondted on granlar materials at stress
More informationPartial versus full wrapping confinement systems for concrete columns
Partial versus ull wrapping oninement systems or onrete olumns J. A. O. Barros Assistant Pro., Dep. o Civil Eng., Shool o Eng., Univ. o Minho, Azurém, 481 58 Guimarães, Portugal D. R. S. M. Ferreira PhD
More informationShear in Beams 2. Reinforced Concrete Design. Shear Design Summary. Shear design summary More detail shear design. Shear span Deep beam WSD SDM
Reinfored Conrete Deign Shear in Beam 2 Shear deign mmary More detail hear deign Shear pan Deep beam Mongkol JIRAACHARADET S U R A N A R E E UNIERSITY OF TECHNOLOGY INSTITUTE OF ENGINEERING SCHOOL OF CIIL
More informationA Comparison of the Greenshields, Pipes, and Van Aerde Car-Following and Traffic Stream Models
A Comparison o the Greenshields, Pipes, and Van Aerde Car-Following and Trai Stream Models by: Hesham Raha and Brent Crowther ABSTRACT The paper ompares three ar-ollowing models. These models inlde the
More informationSimplified Identification Scheme for Structures on a Flexible Base
Simplified Identification Scheme for Strctres on a Flexible Base L.M. Star California State University, Long Beach G. Mylonais University of Patras, Greece J.P. Stewart University of California, Los Angeles
More informationBEHAVIOR OF SQUARE CONCRETE-FILLED TUBULAR COLUMNS UNDER ECCENTRIC COMPRESSION WITH DOUBLE CURVATURE DEFLECTION
Otober 2-7, 28, Beijing, China BEHAVIOR OF SQARE CONCRETE-FILLED TBLAR COLNS NDER ECCENTRIC COPRESSION WITH DOBLE CRVATRE DEFLECTION T. Fujinaga, H. Doi 2 and Y.P. Sun 3 Assoiate Professor, Researh Center
More informationNON-LINEAR BENDING CHARACTERISTICS OF PHC PILES UNDER VARYING AXIAL LOAD
13 th World Conferene on Earthquake Engineering Vanouver, B.C., Canada August 1-6, 24 aper No. 356 NON-LINEAR BENDING CHARACTERISTICS OF HC ILES UNDER VARYING AXIAL LOAD Toshihiko ASO 1 Fusanori MIURA
More informationDr. Hazim Dwairi 10/16/2008
10/16/2008 Department o Civil Engineering Flexural Design o R.C. Beams Tpes (Modes) o Failure Tension Failure (Dutile Failure): Reinorement ields eore onrete ruses. Su a eam is alled under- reinored eam.
More informationThe Effect Of Panel Zone On The Column-To-Beam Strength Ratio Required To Prevent The Soft Story Of Steel Moment Frames
The Effet Of Panel Zone On The Column-To-Beam Strength Ratio Required To Prevent The Soft Stor Of Steel Frames S.W. Choi, Y.S. Kim & H.S. Park Yonsei Universit, Seoul, South Korea SUMMARY: THE EFFECT OF
More informationWRAP-AROUND GUSSET PLATES
WRAP-AROUND GUSSET PLATES Where a horizontal brae is loated at a beam-to-olumn intersetion, the gusset plate must be ut out around the olumn as shown in Figure. These are alled wrap-around gusset plates.
More informationMoment Curvature Characteristics for Structural Elements of RC Building
Moment Curvature Charateristis for Strutural Elements of RC Building Ravi Kumar C M 1,*, Vimal Choudhary 2, K S Babu Narayan 3 and D. Venkat Reddy 3 1 Researh Sholar, 2 PG Student, 3 Professors, Department
More information13 Fitzroy Street London W1T 4BQ Telephone: +44 (0) Facsimile: +44 (0)
Oasys AdSe Theory 13 Fitzroy Street London W1T 4BQ Telephone: +44 (0) 0 7755 330 Fasimile: +44 (0) 0 7755 370 Central Square Forth Street Newastle Upon Tyne NE1 3PL Telephone: +44 (0) 191 38 7559 Fasimile:
More informationA.1. Member capacities A.2. Limit analysis A.2.1. Tributary weight.. 7. A.2.2. Calculations. 7. A.3. Direct design 13
APPENDIX A APPENDIX A Due to its extension, the dissertation ould not inlude all the alulations and graphi explanantions whih, being not essential, are neessary to omplete the researh. This appendix inludes
More informationThe physics of the longitudinal light clock
he physis of the longitdinal light lok Giovanni Zanella Stdioso Senior dello Stdim Patavinm Università di Padova, Italy giovanni.zanella@nipd.it bstrat he standard analysis of the behavior of the longitdinal
More informationThe Simple Solutions of Four Actual Problems. of General Theory of Relativity.
The Simple Soltions of For Atal Problems of General Theory of Relativity. H Changwei Room 81, No.17,Lane 1769, Pdong Wlian Road, 19 Shanghai China,1-8818, hhangwei5@yahoo.om.n Abstrat: It is qite ompliated
More informationShear Strength of Squat Reinforced Concrete Walls with Flanges and Barbells
Transations, SMiRT 19, Toronto, August 2007 Shear Strength of Squat Reinfored Conrete Walls with Flanges and Barbells Cevdet K. Gule 1), Andrew S. Whittaker 1), Bozidar Stojadinovi 2) 1) Dept. of Civil,
More informationTORSION By Prof. Ahmed Amer
ORSION By Prof. Ahmed Amer orque wisting moments or torques are fores ating through distane so as to promote rotation. Example Using a wrenh to tighten a nut in a bolt. If the bolt, wrenh and fore are
More informationBeam Stresses Bending and Shear
Beam Stresses Bending and Shear Notation: A = name or area A web = area o the web o a wide lange setion b = width o a retangle = total width o material at a horizontal setion = largest distane rom the
More informationDerivation of the Bi-axial Bending, Compression and Shear Strengths of Timber Beams
Send Orders of Reprints at reprints@benthasieneorg The Open Mehanis Jornal 0 6 4-4 Open Aess Deriation of the i-axial ending Copression and Shear Strengths of Tiber eas T A C M Van Der Pt * Falt of Ciil
More informationLeif Otto Nielsen. Concrete Plasticity Notes BYG DTU T E K N I S K E UNIVERSITET. Undervisningsnotat BYG DTU U ISSN
BYG DTU Lei Otto Nielsen Conrete Plastiit Notes DANMARKS T E K N I S K E UNIVERSITET Undervisningsnotat BYG DTU U-087 008 ISSN 60-8605 CONCRETE PLASTICITY NOTES Lei Otto Nielsen 6 de 008 CONTENTS. COULOMB
More informationDetails of Check for Boundary Element Requirements
COMUTERS AND STRUCTURES, INC., BERKELEY, CALIFORNIA DECEMBER 2001 SHEAR WALL DESIGN UCB 97 Technical te Wall ier Bondary Elements This Technical te describes how the program considers the bondary element
More informationDesign a reinforced concrete retaining wall for the following conditions. f'c = 3000 psi fy = 60 ksi
CE 4 Fall 005 Retag all Deign Example / 8 Deign a reore onrete retag all or the ollog onition. 000 pi 0 i rharge q 400 p Fill: φ o Unit t 00 p H 8 t toe t tem Natral Soil: φ o alloable bearg prere 5000p
More informationAppendix XI Detailing Requirements of the Prestressed Concrete Girder Bridge
endix XI Detailing Reqirement o the Pretreed Conrete Girder Bridge 1.a. Tranere Reinorement in otential lati hinge zone ing the imliit hear detailing aroah. bh ro etional area o the iral reinorement 0.1
More informationLab Manual for Engrd 202, Virtual Torsion Experiment. Aluminum module
Lab Manal for Engrd 202, Virtal Torsion Experiment Alminm modle Introdction In this modle, o will perform data redction and analsis for circlar cross section alminm samples. B plotting the torqe vs. twist
More informationLecture Note 6. Moment-Curvature (M-φ) Relation - I
7 Letre Note 6 oment-crvatre (-φ) Relation - I -φharateriti oniering IS: 456: The atal moment-rvatre relationhip o R.C. primati etion i obtaine rom tre-train iagram o onrete an teel. Starting rom the bai
More informationMasonry Beams. Ultimate Limit States: Flexure and Shear
Masonry Beams 4:30 PM 6:30 PM Bennett Banting Ultimate Limit States: Flexure and Shear Leture Outline 1. Overview (5) 2. Design for Flexure a) Tension Reinforement (40) b) Compression Reinforement (20)
More informationState variable feedback
State variable feedbak We have previosly disssed systems desribed by the linear state-spae eqations Ax B y Cx n m with xt () R the internal state, t () R the ontrol inpt, and yt () R the measred otpt.
More informationAddition of velocities. Taking differentials of the Lorentz transformation, relative velocities may be calculated:
Addition of veloities Taking differentials of the Lorentz transformation, relative veloities may be allated: So that defining veloities as: x dx/dt, y dy/dt, x dx /dt, et. it is easily shown that: With
More informationConfinement of Reinforced Concrete Columns
This artile was downloaded by: 10.3.98.93 On: 22 Nov 2018 Aess details: subsription number Publisher: CRC Press Inorma Ltd Registered in England and Wales Registered Number: 1072954 Registered oie: 5 Howik
More informationCLEARINGHOUSE FOR FEDERAL SCIgCTIFIJ AND TECHNICAL INFORMATION, CFSTI DOCUMENT KANAGEWEirr BRANCH UO.ll LIMITATIONS IN REPRODUCTION QUALITY
CLEARINGHOUSE FOR FEDERAL SCIgCTIFIJ AND TECHNICAL INFORMATION, CFSTI DOCUMENT KANAGEWEirr BRANCH UO.ll LIMITATIONS IN REPRODUCTION QUALITY Aession # /^."V 1. We regret that legibility of this dov-nent
More informationFlexural Drift Capacity of Reinforced Concrete Wall with Limited Confinement
ACI STRUCTURAL JOURNAL TECHNICAL PAPER Title no. 110-S10 Flexural Drift Capaity of Reinfored Conrete Wall with Limited Confinement by S. Takahashi, K. Yoshida, T. Ihinose, Y. Sanada, K. Matsumoto, H. Fukuyama,
More informationSoftware Verification
Sotware Veriiation EXAMPLE CSA A23.3-04 RC-BM-00 Flexural and Shear Beam Deign PROBLEM DESCRIPTION The purpoe o thi example i to veri lab lexural deign in. The load level i adjuted or the ae orreponding
More informationConcept of Stress at a Point
Washkeic College of Engineering Section : STRONG FORMULATION Concept of Stress at a Point Consider a point ithin an arbitraril loaded deformable bod Define Normal Stress Shear Stress lim A Fn A lim A FS
More informationFORCE DISTRIBUTION OF REINFORCED CONCRETE COUPLING BEAMS WITH DIAGONAL REINFORCEMENT
FORCE DISTRIBUTION OF REINFORCED CONCRETE COULING BEAMS WITH DIAGONAL REINFORCEMENT Yenny Nurhasanah Jurusan Teknik Sipil, Fakultas Teknik, Universitas Muhammadiyah Surakarta Jl. A. Yani Tromol os 1 abelan
More informationChapter 1: Differential Form of Basic Equations
MEG 74 Energ and Variational Methods in Mechanics I Brendan J. O Toole, Ph.D. Associate Professor of Mechanical Engineering Howard R. Hghes College of Engineering Universit of Nevada Las Vegas TBE B- (7)
More informationThree-dimensional Meso-scopic Analyses of Mortar and Concrete Model by Rigid Body Spring Model
Three-dimensional Meso-sopi Analyses of Mortar and Conrete Model by Rigid Body Spring Model K. Nagai, Y. Sato & T. Ueda Hokkaido University, Sapporo, Hokkaido, JAPAN ABSTRACT: Conrete is a heterogeneity
More informationMECHANICS OF MATERIALS
00 The Graw-Hill Copanies, n. All rights reserved. Third E CHAPTER 4 Pure ECHANCS OF ATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Bending Leture Notes: J. Walt Oler Teas Teh Universit
More informationEVALUATION OF EXISTING REINFORCED CONCRETE COLUMNS
13 th World Conferene on Earthquake Engineering Vanouver, B.C., Canada August 1-6, 2004 Paper No. 579 EVALUATION OF EXISTING REINFORCED CONCRETE COLUMNS Kenneth J. ELWOOD 1 and Jak P. MOEHLE 2 SUMMARY
More informationStudent (Ph.D.), 2 Professor, Department of Applied Mechanics, S.V.N.I.T., Surat , Gujarat, India.
Amerian International Journal o Researh in Siene, Tehnology, Engineering & Mathematis Available online at http://www.iasir.net ISSN (Print): 2328-3491, ISSN (Online): 2328-3580, ISSN (CD-ROM): 2328-3629
More informationLinear Strain Triangle and other types of 2D elements. By S. Ziaei Rad
Linear Strain Triangle and other tpes o D elements B S. Ziaei Rad Linear Strain Triangle (LST or T6 This element is also called qadratic trianglar element. Qadratic Trianglar Element Linear Strain Triangle
More informationAcoustic Attenuation Performance of Helicoidal Resonator Due to Distance Change from Different Cross-sectional Elements of Cylindrical Ducts
Exerpt rom the Proeedings o the COMSOL Conerene 1 Paris Aousti Attenuation Perormane o Helioidal Resonator Due to Distane Change rom Dierent Cross-setional Elements o Cylindrial Duts Wojieh ŁAPKA* Division
More information3. Several Random Variables
. Several Random Variables. To Random Variables. Conditional Probabilit--Revisited. Statistical Independence.4 Correlation beteen Random Variables Standardied (or ero mean normalied) random variables.5
More informationNon-linear finite element analysis of reinforced concrete members and punching shear strength of HSC slabs
MATEC Web o Conerenes 49, 56 (8) CMSS-7 https://doi.org/.5/mateon/84956 Non-linear inite element analysis o reinored onrete members and punhing shear strength o HSC slabs Kernou Nassim, Belakhdar Khalil
More informationBeams on Elastic Foundation
Professor Terje Haukaas University of British Columbia, Vanouver www.inrisk.ub.a Beams on Elasti Foundation Beams on elasti foundation, suh as that in Figure 1, appear in building foundations, floating
More informationMODELING OF NONLINEAR BEHAVIOR OF RC SHEAR WALLS UNDER COMBINED AXIAL, SHEAR AND FLEXURAL LOADING
CD02-003 MODELING OF NONLINEAR BEHAVIOR OF RC SHEAR WALLS UNDER COMBINED AXIAL, SHEAR AND FLEXURAL LOADING B. Ghiassi 1, M. Soltani 2, A. A. Tasnimi 3 1 M.Sc. Student, School of Engineering, Tarbiat Modares
More informationAppendix XXII Detailing Requirements of the Prestressed Concrete Girder Bridge
endix XXII Detailing Reqirement o the Pretreed Conrete Girder Bridge Wet Bond Bridge 1.a. Tranere Reinorement in otential lati hinge zone bh ro etional area o the iral reinorement 0.11 in (# rebar enter-to-enter
More informationMODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP OF CONCRETE IN UNIAXIAL COMPRESSION
VIII International Conferene on Frature Mehanis of Conrete and Conrete Strutures FraMCoS-8 J.G.M. Van Mier, G. Ruiz, C. Andrade, R.C. Yu and X.X. Zhang Eds) MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP
More informationDESIGNING FOR LATERAL-TORSIONAL STABILITY IN WOOD MEMBERS
DESIGNING FOR ATERA-TORSIONA STABIITY IN WOOD EBERS American Wood oncil TEHNIA REPORT 4 American Forest & Paper Association The American Wood oncil (AW) is the wood prodcts division of the American Forest
More informationData Extrapolation Method for The Dynamic Increasing Energy Test: SEM-CASE
ata Extrapolation Method for The ynami Inreasing Energy Test: SEM-CASE E.C. Alves, M.M. Sales, P.M.F. iana Abstrat. The dynami inreasing energy test has been widely sed in pile load tests in Brazil in
More informationMECHANICS OF MATERIALS
00 The Graw-Hill Copanies, n. All rights reserved. Third E CHAPTER Pure ECHANCS OF ATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Bending Leture Notes: J. Walt Oler Teas Teh Universit
More informationfib Model Code 2020 Shear and punching provisions, needs for improvements with respect to new and existing structures
fib Model Code 2020 Shear and punhing provisions, needs for improvements with respet to new and existing strutures Aurelio Muttoni Workshop fib Sao Paulo, 29.9.2017 Éole Polytehnique Fédérale de Lausanne,
More informationInternational Journal of Advanced Engineering Research and Studies E-ISSN
Researh Paper FINIE ELEMEN ANALYSIS OF A CRACKED CANILEVER BEAM Mihir Kumar Sutar Address for Correspondene Researh Sholar, Department of Mehanial & Industrial Engineering Indian Institute of ehnology
More informationThe Serviceability Considerations of HSC Heavily Steel Reinforced Members under Bending
Amerian Journal of Applied Sienes 5 (9): 115-114, 8 ISSN 1546-99 8 Siene Publiations The Servieability Considerations of HSC Heavily Steel Reinfored Members under Bending 1 Ali Akbar ghsoudi and Yasser
More informationLecture 11 Buckling of Plates and Sections
Leture Bukling of lates and Setions rolem -: A simpl-supported retangular plate is sujeted to a uniaxial ompressive load N, as shown in the sketh elow. a 6 N N a) Calulate and ompare ukling oeffiients
More informationShooting Method for Ordinary Differential Equations Autar Kaw
Shooting Method or Ordinary Dierential Eqations Atar Kaw Ater reading this chapter, yo shold be able to. learn the shooting method algorithm to solve bondary vale problems, and. apply shooting method to
More informationResidual Bearing Capabilities of Fire-Exposed Reinforced Concrete Beams
International Jornal o Applied Siene and Engineering 2006. 4, 2: 5-63 Reidal Bearing Capabilitie o Fire-Expoed Reinored Conrete Beam J. H. H,2, * and C. S. Lin 2 Department o Civil Engineering, Ching Yn
More informationPunching Shear Retrofit Method Using Shear Bolts for Reinforced Concrete Slabs under Seismic Loading
Punhing Shear Retroit Method Using Shear Bolts or Reinored Conrete Slabs under Seismi Loading by Wensheng Bu A thesis presented to the University o Waterloo in ulillment o the thesis requirement or the
More informationOasys. Concrete Code Reference
Conrete Code Reerene 13 Fitzroy Street London W1T 4BQ Telephone: +44 () 2 7755 332 Fasimile: +44 () 2 7755 372 Central Square Forth Street Newastle Upon Tyne N1 3PL Telephone: +44 () 191 238 7559 Fasimile:
More informationANALYTICAL MODELING ON DEBONDING FAILURE OF FRP-STRENGTHENED RC FLEXURAL STRUCTURES. Abstract. Introduction
ANALYTICAL MODELING ON DEBONDING FAILURE OF FR-STRENGTHENED RC FLEXURAL STRUCTURES Dr. Hedong Niu, Ibaraki University, Hitahi, Japan ro. Zhishen Wu, Ibaraki University, Hitahi, Japan Abstrat Eetive appliation
More informationSimulation of Nonlinear Behavior of Wall-Frame Structure during Earthquakes
Simulation of Nonlinear Behavior of Wall-Frame Structure during Earthquakes b Masaomi Teshigawara 1, Hiroshi Fukuama 2, Hiroto Kato 2, Taiki Saito 2, Koichi Kusunoki 2, Tomohisa Mukai 2 ABSTRACT The reinforced
More information(JPL-2557) DEFORMATION PATH PLANNING FOR BELT OBJET MANIPULATION
Proeedings of 1 ISFA 1 International Symposim on Flexible Atomation Tokyo, Japan Jly 1-14, 1 (JP-557) DEFORMATION PATH PANNING FOR BET OBJET MANIPUATION Yya ASANO, Hidefmi WAKAMATSU, Eiji MORINAGA, Eiji
More informationCity, University of London Institutional Repository
City Researh Online City, University of London Institutional Repository Citation: Labib, M., Moslehy, Y. & Ayoub, A. (07). Softening Coeffiient of Reinfored Conrete Elements Subjeted to Three-Dimensional
More informationFlexural Strength Design of RC Beams with Consideration of Strain Gradient Effect
World Aademy of Siene, Engineering and Tehnology Vol:8, No:6, 04 Flexural Strength Design of RC Beams with Consideration of Strain Gradient Effet Mantai Chen, Johnny Ching Ming Ho International Siene Index,
More information