0% found this document useful (0 votes)
404 views54 pages

1RCD 2-3

Uploaded by

Kechan Shen
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF or read online on Scribd
0% found this document useful (0 votes)
404 views54 pages

1RCD 2-3

Uploaded by

Kechan Shen
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF or read online on Scribd
You are on page 1/ 54
CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE, (STRENGTH DESIGN METHOD) - 2.0 NOTATIONS & SYMBOLS: CHAPTER 2: depth of equivalent stress block, mm area of tension reinforcement, mm? Width of compression face of member, mm distance from extreme compression fiber to neutral axis, mm compressive force of concrete, N balanced c, mm distance from extreme compression fiber to centroid of tension reinforcement, mm distance from extreme compression fiber to centroid of compression — reinforcement > modulus of elasticity of concrete, MPa es modulus of elasticity of steel = 200,000 MPa ive stress of concrete, MPa specified compre calculated stress in reinforcement at service loads, MPa specified yield strength of steel, MPa overall thickness of member, mm nominal moment, Nm nominal balanced moment, Nmm nominal moment for tension-controlled section, Nmm_ nominal maximum moment, Nmm. ultimate moment at section, Nmm_ tensile force of steel reinforcement, N factor depending on the value of fi! strain in steel below yield point = f,/E, strain in concrete, (maximum = 0.003) strain in steel at yield point = f,/E, strength reduction factor ultimate moment capacity, Nmm ultimate maximum moment, Nmm balanced steel ratio ratio of tension reinforcement reinforcement index we eee ae fo CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) 2.1 INTRODUCTION Beams are structural members that are primarily subjected to flexure or bending. There are two philosophies of design that are used to analyze the beam sections ~ (1) Working Stress Method and (2) Strength Design Method. In the Working Stress Method, a structural element is so designed that the stresses resulting from the action of service loads/working loads and computed by the mechanics of elastic members do not exceed some predesignated allowable values. In the Strength Design Method (formerly called Ultimate Strength Design), the service loads are inereased by factors to obtain the load at which failure is considered to be imminent. This load is called the factored load or factored service load. The Strength Design Method requires the conditions of static equilibrium and strain compatibility across the depth of the section to be satisfied. The cross-sectional dimensions of a flexural member and the required amount of flexural reinforcement at critical sections are determined using the strength and serviceability requirements of the Code. For flexure, design strength for at all sections shall satisfy OM, > M, where @My is the design strength of the member at a particular section and My is the moment due to the factored loads, which commonly is referred to as the factored design moment. 2.2 DESIGN ASSUMPTIONS FOR CONCRETE (NSCP 2015 SECTION 4222.2) The following are the assumptions for Strength Design method: = 422.2.2.1 Maximum strain at the extreme concrete compression fiber shall be assumed equal to 0.003 = 4222.22 Tensile strength of concrete shall be neglected in flexural and axial strength calculations. * 422,2,2.3 The relationship between concrete compressive stress and strain shall be represented by a rectangular, trapezoidal, parabolic, or other shape that results in prediction of strength in substantial agreement with results of comprehensive tests, 422.2.2.4.1 Concrete stress of 0.85f¢ shall be assumed uniformly distributed over an equivalent compression zone bounded by edges of the cross section and a line parallel to the neutral axis located a distance @ from the fiber of maximum compressive strain, as calculated by: a=Byc 422.2.24.2 Distance from the fiber of maximum compressive strain to the neutral axis, c, shall bbe measured perpendicular to the neutral axis. 422.2.2.4.3 Values of B, shall be in accordance with Table 422.2.2.4.3 CONCRETE DESIGN MJBCASTRO 4 ee CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) Table 422.2243 Values of f; for Equivalent Rectangular Concrete n 17< fi <28 (a) 0.05(f2 — 28) (b) 7 28 < fi <55 0.85 — fees5 0.65 (©) 2.3 ANALYSIS OF A SINGLY-REINFORCED BEAM fey eae fe — E=}) a 4 a 7 NA| oo | Ti T T=A,fy s ‘Actual Equivalent Stress and Strain Diagram for Singly-Reinforced Rectangular Beam a= Bic > (Eq2.1) Cm ~~ =Ahy a 57 42.2) 0.85f2b oe Multiplying Eq (22) by $; == _—_—sasu—sWXM—a(aCeet”t CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) The term # is called the ratio of steel reinforcement and is denoted as p Phy «~ OaSfe > (Eq 24) Leto = ob — Reinforcement Index Ratio a = (Bq 25) Nominal Moment Capacity From the stress diagram, @ My = C. (a = 3) a M, = 0.85fab (d ~5) 1 wd M,, = 0.85f! sas (4-54) M, = f-wbd*(1 — 0.59w) > (Eq 2.6) Ultimate Moment Capacity (Design Strength): My = OM, My = Of wbd(1 — 0.59w) > (Eq 2.7) Coefficient of Resistance: frw(d — 0.59w) + (Eq 2.8) Then, M, = OR,bd? ~ (Eq 2.9) Solving for «in Eq 2.8 and substitute w =p”; p= o.asfe a- 1-5 1 ag] -ex2. = REINFORCED DESIGN — Pe MJBCASTRO > eS CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) > 23.1 TYPES OF FAILURE AND STRAIN LIMIT Three types of flexural failure of a structural member can be expected depending on the percentage of stec| used in the section. te reaches its maximum strength, in this case, snc failue is due to the yielding of steel reaching a high strain equal #0 oF greater than 0.005 Tie motion contains a relatively emall amount of steel lesser then WHSE’8 required for balanced condition and is called a TENSION-CONTROLLED SECTION. 1. _ Steel may reach its yield strength before the concret ion fiber just reaches the crushing strain 2, The maximum strain at the extreme concrete compress = fy/E, causing them to fail é, = 0.003 at the same time as the tension steel reaches & strain €5 simultaneously, the section is called a BALANCED SECTION. of high percentage of steel in the 3, Concrete may fail before the yield of steel, due to the presence © section more than what is required for balanced condition. In this case, the concrete strength and its maximum strain of 0.003 are reached, but the steel stress 1s ess than the yield strength, that is, f < fy The strain in the steel is equal to or less than (0.002. This section is called 2 COMPRESSION-CONTROLLED SECTION. 0.003 e_ = 0.003 e, = 0.003 £, = 0.003 yr ' ~ «, . Cnas| « a fe > y 1 €, 2 0.005 e, = 0.004 &, 50.002 E=p/z. ‘TENSION MAXIMUM COMPRESSION BALANCED CONTROLLED CONDITION CONTROLLED CONDITION 9=0,75 40,252 1000 where f, = 600 00MPa for maximum condition 000M Pa for tension — controlled fe fe on. \ 0 = 0.6540 ase=fy 8 = 0.90 for Tension-controlled 1000 -f, fel 0 = 0.65 for Compression-controlled a Strength Reduction Factor cowie TR = _—_—_——————“‘_‘—i™S~*~™” CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) > 23.1.1 THE BALANCED CONDITION Considering the ease of balanced section which implies that at ultimate load, the strain in concrete ¢ = 0.003 and that of steel &, = fy/Es &¢ = 0.003 e &s = fy/Es By Ratio & Proportion & _d-a 0.003 f, /e, ole d— ec, 0.003 ~ f,/200000 680d ctated b= Sop f, ~ Balanced c a oa ince a = fic +o = pdf, OBS __pafy Bo (ORSfB pdf, _ 600d . 0.85f/8 — 600+ f, . fe(_ 600 = 0.856 S i Po iB 7, 600+ 7) Balanced Steel Ratio SIMPLIFIED REINFORCED CONCRETE DESIGN MJBCASTRO i { a CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE i (STRENGTH DESIGN METHOD) > 23.1.2 THE MAXIMUM CONDITION For maximum condition, ¢, = 0.004 &¢ = 0.003 By Ratio & Proportion: Cmax _ 4 — Cmax 0.003, 0.004 Cmax = G4 ~ Cmax) max = 54 3 @ = Bicmax = Br 5 For Rectangular Beam: C,=T 0.85 flab = Acmarfy 085f (B: 34)» = pmesbafy 30.85/61 Prax = 5 i OMymax = OC (d - 2) 3 d OMnmax = O(0.85f. By 3 4b) (« bad “r) 1 OM pmax 2 Bifebd? (1 CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) > 2.3.4.3 THE TENSION-CONTROLLED SECTION ‘The beam is tension-controlled when €5 2 0.005 e, = 0.005 Bee mip od a=ho= big For Rectangular Beam: OMpe = OCe (d -9 OMye = 0.9(0.85f¢ab) (d — 3) 3 By 3¢ OMe = 0.9(0.85f¢8, =db) | d-—8— 3 2 _ 459 3 Mae = Teqq Pascoe? ( Sat) ee SIMPLIFIED REINFORCED CONCRETE DESIGN MIBCeane? ey “a >» CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) > 2.3.2 MINIMUM FLEXURAL REINFORCEMENT IN NON-PRESTRESSED BEAMS (NSCP 2015 SECTION 409.6.1) © 409,6.1.1 A minimum area of flexural reinforcement Asymin shall be provided at every section ion reinforcement is required by analysis. where te ), except as provided in Section 409.6.1.3. For + 409.6.1.2 Agymin Shall be the greater of (a) and ( 1w shall be the lesser of by atically determinate beam with a flange in tension, the value of b, a and 2by = 409.6.1.3 If A, provided at every section is at least one-third greater than A, required by analysis, Sections 409.6.1.1 and 409.6.1.2 need not be satisfied. ; > 233 STEPS IN FINDING THE REQUIRED TENSION STEEL AREA A, OF A BEAM WITH 4 KNOWN REQUIRED MOMENT M,, AND OTHER BEAM PROPERTIES. Given: b, d, fé, fy,and My Solve for pynax and OMpmax 3 0.85f2) max = 3 TL fy 51 2 SU ee Mymax = zap Palébe? (1-1) Omgeeios ee & 1000 - f, OMpmae = if Mnmax 2 My design as Singly Reinforced (Step II) if @Mnmax My then tension controlled, 0 = 0,90, il proceed to Ste; if My, 234 STEPS IN FINDING OM, OF A BEAM WITH KNOWN TENSION STEEL AREA 4, AND OTHER BEAM PROPERTIES. Given: b, d, ff, fy, and Ag I. Solve for p: Is °* ba Pmin shall be the greater of (a) or (b): o.25/f @) Pmin = i ) es ) Pmin = Il. Check if steel yields by computing py sp, £000 Pr = 0.8! BF 600+ hy ifp

py steel does not yield, proceed to Step IV NOTE: if p < Pmin, the given A, is not adequate for the beam dimension. — 7 UL. p < py ' 0.85f!ab = Asfy a iff, > 1000 MPa, tension controlled, iff, < 1000 MPa, transition region fe-fy 1000 - = a a OM, = 00.85fab (d — a 9 =0.65+ 0.25 3: ANALYSIS AND DESIGN OF BEAMS FOR FLE LEXURE CHAPTER (STRENGTH DESIGN METHOD) IV. p > Pb compression controlled, @ = 0.65 CC. =T 0.85flab = Asfs a= fie &f, = 6005—= d-c C 0.85f{Bycb = As600—— ce a=fyc = — d fe = 600—— = — Thus, om, or (6-$)=04s (4-5) or OM, = 06. (a 5) = 90.85/eab (a-$) ‘HAPTER 2: ANALYSIS AND DI OF BEAMS FOR FLEXURE mae C (STRENGTH DESIGN METHOD) ILLUSTRATIVE PROBLEMS: Solution: 3 fz (__600 Pn = ose ( ) 600+ f » By = 0.85 for f = 21 MPa 21/600 =08 (= __) = 0.02792 / Pb Te DBALO. 85) 335 (goo rl coe b. : ag Pb ra bd Asp = 0.02792(300)(500) Asp = 4188 mm? Solution: , 600d % S600 = are ili. caine b. a is 600 nae i (eorng) 0.05 B, = 0.85 — | — 28) = 0.85 8 30 — 28) = 0.836 bo CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLE vs (STRENGTH DESIGN METHOD) LEXURE 6) 32 ( 600) Pr = 0.85(0.836) 773 (G99 4 =z) = 0.03047 As, Po =a bd ‘Agy = 0.03047(300)(500) Agy = 4570.5 mm? Solution: a a (se “lag By = 0.85 for f = 21 MPa 2 Pmax = 5(——Se 345 0.01885 b. Asmasx ; Agmax = 0.01885(300)(500) Agmax = 2827.5 mm? c ] 51 3 = O0—A#, fibd? (1-—, OMamax = OF Ps k'ba? (1-= 61) 800-f, 800 - 345 S A ae = BZA Ones = 0165 + 0.25 75555 = 065 + 0.25 7959-545 = ° OM pmax = 08244 (0 2 (1-2 08s) inmax = 0.824 (0,85)(21)(300)(500)? ( 1 - + (0. 0 328.660 kNm CONC AEIED REINFORGED e a CONCRETE DESIGN te MJBCASTRO 1D) DESIGN OF BEAMS FOR FLEXURE | 28 CHAPTER 2: ANALYSIS (STRENGTH DESIGN METHOD) Solution: 7 3 ee 3a = 5 (500) = 214.286 mm b. a ( Bee Pmax = 7\— By = 0.85 for f/ = 28 MPa 85) pn =a es Pmax =a Asmax = 0.02094(300)(500) Asmax = 3141 mm? Solution: Solve for OMpmax: oe SL , 3 Mynax = OF ap Pifibd? (1 -ah) | penance ‘HAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTA DESIGN METHOD) ae 800 ~ 276 max = 0.65 + 0.25 ——__ = 0.65 4.0.25 0 276 _ 1000 = fy 787000 = 276 = 0.831 By = 0.85 for 27.6 MPa Then, 51 4 OMpmax = (0.831) 755 (0.85)(27.6)(300)(490)2 (1 a 740089) OMpmax = 418.371 kNm ~~ a. My =20kNm <@Mymax — Singly Reinforced Determine if the section is tension-controlled or transition: 459, 3 OMae = egg Prlibd? (1- hr) 459 3 OMne = FeG9 (0-85)(27.6)(300)(490)* (1 aa (085)) OMe = 407.508 kNm OMnr > M, — Tension — controlled, 0 = 0.90 Solve for Ry: M, = OR,,bd® 20x 106 = 0.90R,,(300)(490)? Ry, = 0.30851 a. Pt BSF: 08576), |, _ 2(0.30851) 276 rR 0.85(27.6) p= 0.00113 Solve for p: Check min? 4 Pmin =” = 976 = 0.00507 > 0.00113 + Use p= min = 0.00507 Thus, see Az = pbd = 0.00507(300)(490) = 745.29 mm? Fe ee REINFORCED CONCRETE DESIGN MJBCASTRO CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR URI (STRENGTH DESIGN METHOD) b. My = 140 KNm < OMymax > Singly Reinforced Determine if the section is tension-controlled or transition: OMe > My > Tension ~ controlled, @ = 0.90 Solve for R, OR bd® 140 x 10° = 0.90R,,(300)(490)? Ry, = 2.15959 Solve for p: O85 f, 2Rn Pah (.- = oas(a7.6)/,_ |, _2(2:15959) 276 i 0.85(27.6) p= 0.00822 J Check Prin 14 14 === = 0005 00: Pmin = = 776 = 9° 07 < 0.00822 = Use p = 0.00822 Thus, ‘A, = phd = 0.00822(300)(490) = 1208.34 mm? cc. My =410kNm < OMpmax > Singly Reinforced Determine if the section is tension-controlled or transition: My, < My > Transition re Solve for c and As: M,, = 00.85ffab(a-<) a=fe d @ = 0.65 + 0.25: where f, = 600. 1000 jf, 4) (0.85! 8,cb) (a a Ae ee SIMPLIFIED REINFORCED “acm aa ‘CONCRETE DESIGN — § «=—sli(isd ——"“™~S—=——s—s—~S~—i—“i—O—s—sSO CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) iG 49 410x108 = (os +0254 —a59 276 (0.88)(27.6)(0.85)(e)(300) (490 ~ 9255) 276 c= 189.534 mm a = 0,85(189.534) = 161.104 mm 490 — 189.534 189.534 Pieced aeiranz7e Bree (-22" 1000276 = 951.173 MPa > fy, fy = fy a0" f, = 600— = 0.883 Then, ea 0.85fab = Asf, 0.85(27.6)(161.104)(300) = A.(276) A, = 4108.152 mm? @-My=500KNm > OMymax —* Doubly Reinforced ‘Compression reinforcement is necessary (see Chapter 3) Solution: I Solve for p: 2 Ag _ 3525 = 5a = 300500) ~ °° Pmin Shall be the greater of (a) or (b): _ 0.25) fe _ 0.25V3: Pas ee = 0.00353 ©) Pmin = Rae 0.00338 * Pin = 0.00353 if pin (34 — 28) = 0.807 34 Pp = 0.85(0.807) — ( 600 m4 oneal = 0.03333 ifp > pp steel does not yield, f, # f, IIL p > pp ‘compression controlled, 0 = 0.65 C.=T O.85f/ab = Ayf, fs = 600: a=Byec 0.85(34)(,c)(300) = 97 (28? (600 orem SY SAE SIMPLIFIED REINFORCED CONCRETE DESIGN MJBCASTRO- d-c c wy ee eS ‘STRENGTH DESIGN METHOD ETON OF BEAMS FOR FLEXURE ' 9.85(34)(0.807)(c)(300) a 500 — = 97 (28)? (600 “) = 304.673 mm @ = 0.807 (304.673) = 245.871 mm as 500 — 304.673 f, = 600 600?" = 384.662 MP. ‘ 0 s0sG 7am ean Thus, OM, = 00.85 fab (a ~ 5) OM,, = (0.65)(0.85)(34)(245.871) (300) (500 os OM, = 522.463 kNm cae) Z Solution: Wy = 12Wp, + 1.6, Wy = 1.2(20) + 1.6(40) = 88 kN/m For a simply supported beam: wl? _ 88(6)? Noe cae = 396kNm Solve for DMymax? $1 3 = 02g pnd? (1-2, OMnmax = O55 if’ ba? (1-61) 800-f, i000 Dmax = 0.65 + 0.25 fy, = 0.85 for f! = 21MPa a CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLE: (STRENGTH DESIGN METHOD) ao Then, OMymax = (04 927) 5 (0 85)(21)(300)(550)?(1 (: OMpmax = 399-126 kN 40 85) My * 600+ f, 600+ 345 Gp = B,C = 0.85(460.317) = 391.269 mm % = Gy — 150 = 241.269 mm + SIMPLIFIED REINFORCED. a a as CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) 500mm From the figure: C, +20 =T 0.85/cA; + 2(0.85fA2) = Acfy (0.85) (28)(150)(500) + 2(0.85)(28)(125)(241.269) = Aq,(345) Asy = 9334,929 mm? b. Balanced moment capacity of beam Balanced condition, 0 = 0.65 OMyy = 06; (a -) +200,(a- 150-2) = 2 +2(0.65)(0.85)(28)(4125)(241.269) (725 — 150 ~ OM» = 1178.135 kNm OMyy = (0:65)(0.85)(28)(150)(500) (725 — 241.269 2 ) ©. Maximum steel area max = 54 = 5 (725) = 310.714mm Gmax = BiCmax = 0.85(310.714) = 264.107 mm 2max = Omax ~ 150 = 114.107 mm SIMPLIFIED REINFO! CONCRETE DESIGN MIBCASTRO rt . semmmage CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE ~ "(STRENGTH DESIGN METHOD) From the figure: +20, =T 0.85 A, + 2(0.85f' 2) = Ashy (0.85)(28)(150)(500) + 2(0.85)(28)! Agy = 7141845 mm? (125)(114.107) = Asmax (345) d. Maximum moment capacity OMpmax = 06, (d- =) +206, (d - 150-4) 800-fy 800 eA BOOED = 0,65 + 0.25 Omax = 0:65 + 0257599 = 5 To00 150 OMynay = (0:824)(0.85)(28)(150)(500) (725 -+) 114.107 +2(0.824)(0.85)(28)(125)(114.107) (72 —150- =“) OMymax = 1245.808 kNm e. Required tension steel area when M,, = 800 kNm M, = 800 kNm <@Mymax — Singly Reinforced Note: Some formulas derived may not be applicable for a non-rectangular sections Assume a = 150 mm; ee 176471 Oey aa 76.471 = 1864.994 MPa > 1000 MPa, Tension — controlled @ = 0.90 a OM, = 06, (a ~$) = 0.90(0.85)(28)(150)(500) (725 s =) OM, = 1044.25 kNm E Since the required M, = 800 kNm < 1044.225 kNm, a < 150mm eerie ee Be rd, yea CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) Assuming @ = 0.90 o My = 06e(d-$) £800 x 10° = 0.90(0.85)(28)(a)(500) (725 ~ 5) a= 111.623 mm a _ 111.623 BR 085 c= = 131.321 mm Check Assumption: ie 725 - 131.321 me = 2712: f= 600—— = 600 12.494 MPa > 1000 MPa, Tension ~ controlled $ = 0.90 Assumption is ok! Since f, > fy, therefore steel yields, f; = fy co O.85fJab = Acf, 0.85(28)(111.623)(500) = 4,(345) A, = 3850.185 mm? f, Required tension steel area when M,, = 1200 kNm M, = 1200 Nm < OMymax — Singly Reinforced ‘Note: Some formulas derived may not be applicable for a non-rectangular sections Assume a = 150 mm; nao 176.471 OAS aa 71 = 1864.994 MPa > 1000 MPa, 90 Tension — controlled 6 = a OM, = 0C-(a— $= OM, = 1044.225 kNm .90(0.85)(28)(150)(500) (72s = =) Since the required M,, = 1200 kNm > 1044.225 kNm, a > 150 mm ———E—EE sIMPLIFIED CONCRETE DESIGN MIECAEERY: Es ie . | CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) M, = 06, (a- =) + 200, (d - 150 - 3) 6c, = o.ssta, = 0:85(28)(150)(600) = 1798000 Cy = 0.85f2A2 = 0.85(28)(z)(125) = 2975(0.85¢ — 150) z=a—150 = 0.85¢ — 150 a=fc -e fy where f; = 600 fs = 0 = 0.65 + 0.255599 — f (ott) (2) = (oasoas aT id (600: +2 ( 65 + 0.25 oe) [2975(0-85¢ — 150) G —150— 0.85¢ — =n 1000 = fy 725 -¢) 1200 x 10° = | 0.65 + pp es ees [1zaso00 (725 -4)| PE 1000 — 345 2 0.85¢ — 150)) (600 25—*| — 345 42[ 0.65 +0.25- 5355 — [es7scosse ~ 150) (725 - 150-——— 1000 — 345 98.733 mm. a = 0.85(398.733) = 338.923 mm z = 338.923 — 150 = 188.923 mm 725 — 398.733 = 600: = = h = = 600-So5733 490.956 MPa > fy Since f, > fy, therefore steel yields, f; = fy 490.956 — 345 0 = 0.65 + 0.2: ‘ Soop =a45)( sine Thus, G+, =T 0.85f'A; + 2(0.85f/ Az) = Asfs (0.85)(28)(150)(500) + 2(0.85)(28)(188.923)(125) = A,(345) A, = 8432.150 mm? ernest CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE. (STRENGTH DESIGN METHOD) 700mm, Solution: 450mm, d=700-75 =625mm " Asproviaea = 4 (32)? = 3216.991 mm? Note: Some formulas derived may not be applicable for a non-rectangular sections Solve for Asp 600d _ 600(625) ~ 600+f, 600+345 dy = By cy = 0.85(396.825) = 337.301 mm & = 396.825 mm 2p = dy — 150 = 187.301 mm From the figure: GQ+Q=T (0.85/24,) + 0.85/0A2 = Asf, (0.85)(21)(150)(150) + (0.85)(21)(187.301)(450) = A,,(345) Asp = 5524.986 mm? EERE ENS ASR SIMPLIFIED REINFO! CONCRETE DESIGN MJBCASTRO CHAPT d R 2: ANALYSIS AND DESIG ” NALYSIS ESIGN OF BE, f E IGTH DESIGN METHOD) a 150.150 150 150 a : | Since As provided < Asp, Steel will yield, fz = fy G+ (O.85f/A;) + 0.85/42 = Asfs (0.85)(21)(150)(150) + (0.85)(21)(a — 150)(450) = a (32)?(345, a = 238.171 mm = 280.201 mm 8.171 mm $25 — 260201 738.325 MPa < 1000 MP. 280201 fy as - + Transition region 738.325 — 345 Tora = Pe ® = 0.65 + 0.25 M, = OC, (a - 1) +00 (a < re) My = 0(0.85f¢A,) (a -) + 00.85f4, (d ~ 150-5) M,, = (0:800)(0.85)(21)(150)(150) (625 ~ 5°) 93.17! + (0,800) (0.85)(21)(88.171)(450) (625 ~ 150-~ > M, = 420.865 KNm CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH DESIGN METHOD) 125_ 100, 125_ Solution: = 700 ~ 75 = 625 mm = Asproviaea = 43 (32)? = 3216.991 mm? Note: Some formulas derived may not be applicable for a non-rectangular sections Solve for Asp: 600d 600(625) 00+ f 600+ 345 y= Bicy = 0.85(396.825) = 337.301 mm is = 396.825 mm 2p = dy — 125 = 212301 mm 125_ 100.125, oe MJBCASTRO- CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS FOR FLEXUR) (STRENGTH DESIGN METHOD) E From the figure: 24,+G=T 2(0.85 fy) + 0.85f'A2 = Ashy 2(0. 85)(21)(125)(125) + (0. 1 85)(21)(212.301)(350) = Asy(345) Agy = 5461342 mm? Since As provided < Asby Steel will yield, f = fy 20, + =T 2(0.85 FAs) + 0.85f'A2 = Asfs 2(0.85)(21)(125)(125) + (0.85)(21) (a — a = 213.363 mm 125)(350) = 47 (32)"(345) a _ 213.363 =! = 251.015 ag = 251.015 mm 88.363 mm 625 — 251.015 jae eS: Fe 600-5 893.935 MPa < 1000 MPa =: Transition region 893,935 — 345, Beet 025 — pergge = 0860 My = 200, (4-4) + 00, (a = 125-2 My = 20(0.85f24,) (a -*5°) + 00.85//43 (a — 125 - 5) M,, = 2(0.860)(0.85)(21)(125)(125) (62s es =) + (0.860)(0.85)(21)(350)(88.363 ) (62s = 125- ae = 486.247 KNm CHAPTER 2: ANALYSIS AND DESIGN OF BEAMS F1 (STRENGTH DESIGN METHOD) ‘OR FLEXURE SUPPLEMENTARY PROBLEMS: Mos ue = Pa, f, = 345; Oh — _ CHAPTI ANALYSIS AND DESIGN OF BEAMS FOR FLEXURE (STRENGTH D HOD) ==——_— & °° -. °° °&«»}aar i CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS 3.0 NOTATIONS & SYMBOLS: depth of equivalent stress block, mm area of tension reinforcement, mm? As A, area of compression reinforcement, mm? > width of compression face of member, mm c distance from extreme compression fiber to neutral axis, mm. re balanced c, mm Ge compressive force of concrete, N d distance from extreme compression fiber to centroid of tension reinforcement, mm @ distance from extreme compression fiber to centroid of compression reinforcement, mm E. Modulus of Elasticity of concrete, MPa Ey Modulus of Elasticity of steel, = 200,000MPa ft specified compressive stress of concrete, MPa fe calculated stress in reinforcement at service loads, MPa im specified yield strength of steel, MPa h overall thickness of member, mm. My nominal moment, Nmm_ My ultimate moment at section, Nmm_ oD tensile force of steel reinforcement, N A factor depending on the value of f! & strain in steel below yield point = f,/E, e strain in concrete, maximum = 0.003 y strain in steel at yield point =f /E, o strength reduction factor Po balanced steel ratio CONCRETE DESTN See as CHAPTER 3: ) ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS 3.1 T-BEAMS ! otslabs and beams that are placed monolithically, ss have extra widths at their tops, ca ‘of a T-beam below the slab is rete, Reinforced conerete floor systems normally consist a result, the two parts act together to resist loads, In effect, the beam: flanges, and resulting T-shaped beams are called T-beums. The part to as the web ot stem. ; > 3.1.1 T-BEAM GEOMETRY (NSCP 2015 SECTION 40632) + 406.3.2.1 For non-prestressed T-beams supporting monolithic Or composite slabs, the effec flange width by shall include the beam web jvidth By plus an effective overhanging flange wic in accordance with Table 406.3.2.1, where itis the slab thickness and Sw is the clear distance the adjacent web. Table 406.3.2.1 Dimensional Limits for Effective Overhanging Flange Width for T-Beams i 8h Each side of web Least of: Sw/2 1/8 ; 6h One side of web Least of: Sw/2 L,/12 SIMPLIFIED REINFORCE! CONCRETE DESIG CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS j wR > 3.2 MINIMUM FLEXURAL REINFORCEMENT IN NON-PRESTR BEAMS (NSCP 2015 SECTION 409.6.1) except as provided in Section 409.6.1,3. For II be the greater of (a) and (b). the value of by, shall be the lesser of by © 409,6.1.2 Asgnin Sha team with a flange in tension, a statically determinate and 2B o.25Vfe, A ae eae ty ) Note: vn is in tension, the amount of tension nge of a seetior the unreinforced ACI Commentary R9.6.1.2. If the fla reinforcement needed to ntake the strength of the reinforced section equal that of ection is approximately twice that for a rectangular section OF that of a flanged section with the flange in compression. A greater amount ‘of minimum tension reinforcement is particularly necessary in cantilevers and other statically determinate beams where there is no possibility for redistribution of moments Thus, sith their flange in tension, By in the above formula is to be For statically determinate members W of the flange by, whichever is smaller. replaced with either 2by or the width o 3,2 ANALYSIS AND DESIGN OF T-BEAM CASE 1: when a <¢ as those for Rectangular Beam Note: Analysis and Design is the same a SIMPLIFIED REINFORCED CONCRETE DESIGN ee MS AND DOUBI 4 CHAPTER 3: ANALYSIS AND DESIGN OF T-BEA‘ REINFORCED BEAMS CASE 2: whena >¢ Nominal Moment: b-h 1000-f, @ = 0.65 for balanced condition & compression — controlled 0 = 0.90 for tension — controlled 0 = 0.65 + 0.25. for transition region > 32.1 STEPS IN FINDING THE REQUIRED TENSION STEEL AREA A, OF A SINGLY REINFORCED T-BEAMS WITH KNOWN REQUIRED MOMENT M,, AND OTHER BE \\ PROPERTIES. Given: bd, fé, fy and M, 1. Solve for Mamax 3 Cmax = 54 = = BiCmax = —_ z=a-t =Gides z Mynax = Gi (a geclane-) ‘s he ® 0.65 + 0.25 705 Mraz MJBCASTRO SIMPLIFIED REINFORC!Y CONCRETE DI CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS SIMPLIFIED REINFORCED if OMpmax 2 My design as Singly Reinforced if OMpmax < My design as Doubly Reinforced Il. Check moment capacity of flange OMny Assume c By fe = 600 iff, 1000 MPa, tension controlled, 0 = 0.90 iff, < 1000 MPa, transition region es fi-fy 9 = 065 + 0257905 ifM, OMpp, a>¢ analyze as T—beam IML Analysis as T-beam Assume @ = 0.90 M, = 06, (4-5) +00, (a-¢ * iff, = 1000 MPa, tension controlled, @ = 0.90, assumption is ok! G+G=T O.85f/A; + 0.85f!A2 = Asfy As= Cheek Asmin: Asmin Shall be the greater of (a) or (b): nee B (©) Asmin = CONCRETE DESIGN ie 7 BEAMS AND DOUBLY jot ok! CHAPTER 3: ANALYSIS AND DES: Hl 2 SIGN OF T- REINFORCED BEAMS © if f, < 1000 MPa, transition region ,assumption ™ = tora 0 = 065 + 0253559- f G+G=T O.85flAr + 0.85/cA2 = Ashy As Check Asmin: ‘Aemin Shall be the greater of (a) oF (®): @ amin = aE ed by 14 =— bd ©) Asmin =F > 3.2.2 STEPS IN FINDING OM, OF A T-BEAM WITH KNOWN TENSION STEEL AREA 4, AND OTHER BEAM PROPERTIES. Given: b, df, fy,and As 1. Solve for cp; , - hod > = 600+ fy a= Bil» ifae; proceed to step II — Sas og IL. Solve for: CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS C+, =T 0.85/24; + 0.85f!A2 = Aa = — fy + ifA,> As; tension steel does not yield, @ = 0.65 7 2 = by (at) = by (he ~t) f= 6002 GQ+G= 0.85 fA; + O.85f!A2 = Ach, O85 fdby t+ 0.85 fiby (Bye — t) = A, 600 ee c d-c ¢ OM, = OC, iG - "ifs < Asp; tension steel yields c=T 0.85/24, = Asfy Ac = __ ifAc Ay; thena>t analyze asT— beam My =G (4-3) +0 (¢-e-4) My = O85 f'by (a -5) +085 {iby 2(d—e Solve for 0: c iff, = 1000 MPa, tension controlled, = 0.90 iff, <1000MPa, transition region h—fy = 0.65 +0.25—5 o +028 000% >» AND DESIGN OF T-BEAMS AND DOUBLY Rea CH APT 3: ANALY! REINFORCED BEAMS "ORCED BEAMS 3.3 ANALYSIS AND DESIGN OF DOUBLY-R) ce o aesthetic) and other consideration quired to resist the given bend, pression. These by use of architectural (spa compression force re forced with steel to carry com Tesion steel reinforcement, resulting in & dup, If a beam cross section is limited be may happen that the conerete could not develop the e' moment and the compression conerete should be rein sections are designed to have both tension and compr reinforced beam cement is used for reasons other than resistin tions where reversal of moments might occ reinforcement reduces the long-ter However, there are situations in which compression reinfo moments, Doubly reinforced beams are also used in situal specially during earthquakes. In addition, inclusion of compression deflections of beams and increase the ductility of the sections. ed beam is analyzed by dividing the beam into two couples Myx and Myz as shown. ind the part of the tension steel As ff the tension steel area A.. Doubly reinforce jon conerete ai sssion steel A’ and the other part of = Myz is the couple due to compres: = Mya is the couple due to compre L i eee | = Fy/Es =~“ i#2+;« ii. CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS Ultimate Moment Capacity: My = Mus + Mu Mus = Mu — Muz = ©Mnmax a= 0 (t-3) Balanced condition @ = 0.65 600d 600+h, & Maximum Condition 800 - fy 1000 - fy DOUBLY-REINFORCED RECTANGULAR AND OTHER BEAM PROPERTIES. 0 = 0.65 + 0.25 > 33.1 STEPS TO DETERMINE A, AND A; OF A BEAM WITH KNOWN REQUIRED MOMENT M, Given: b,d, fe, fy,and My 1. Solve for @Mpmax OR if @Mpmax 2 My design as Singly Reinforced if Mymax fyi _ tension steel yields f, = fy = iff, fy; compression steel yields ff = fy = iff! fyi__ tension steel yields f; = fy + iff, f,; compression steel yields f = fy = if ff < fy; compression steel does not yield if I. Ifall steel yields iff, = 1000 MPa, tension controlled, @ = 0.90 iff, < 1000 MPa, _ transition region = 0.65 + 0.25 My = Mus + Mug My = Mus + Muz a M, = 07, (d-5) + 072(d - 4) M, = 06. (4 -3) +00,(d-d') or My = OAgify (4-5) + Aczfeld— 2) M, = 0085{fab(d-$) + 04 f4(d - 4) My= My = III. If compression steel does not yield T=Ce+Cy Achy = 0.85 fcab + Asfe Asfy = 0.85 f¢Bycb + As (00! 7 ‘SIMPLIFIED REINFORCED CONCRETE DESIGN D DOUBLY | oR? CHAPTER 3: ANALYSIS AND DESIGN OF T-| AMS AN’ REINFORCED BEAMS : ft tension controlled, = 0.90 if f, = 1000 MPa, nsition region 0 = 0.65 + 0.25 iff, <1000MPa, tra My = Mus + Muz My = Mus + Mug = 07, (a- 5)+ ord - 4’) a‘ My = Ce (4-3) + 6(d-a’) or , i ie =0Anf, (4-5) + OAgf(d - 4) M, = 00.85 fab (d —5) + 94; f1(4 ~ 4 he — ae IV. If tension steel does not yield @ = 0.65 T=Cco+ Asfs = bbe gab+ aiff As (600==*) = = 0.85f/Bicb + Achy c= a= 2 ff = 6005 y d f= 6005 = __ My = Mus + Muz M= Mus + Mua Z " @ = 0% (d-5) + 07(d - a) My = 06,(d-$) + 06,(4 4) or My, = OAgsfy (4-5) + OAsafe(d - 4) M, = 90.85 fab (a — 5) + 0Arfi(d-¢ Me i M= = °° ° & .: CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS ILLUSTRATIVE PROBLEMS: Solution: From NSCP 2015 Table 406.3.2.1 Effective Flange width by is the smallest of a. by + 16h = 250 + 16(120) = 2170 mm be By + (Sws/2) + (Sw2/2) = 250 + (3000/2) + (3000/2) = 3250 mm cc. by + (Ly/4) = 250 + (5000/4) = 1500 mm . Therefore, by = 1500 mm Solution: a, Balanced steel area 600d __ 600(460) _ 57> 199 % = S004 f oo0t414 mm fy = 0.85 for fe! = 20.7 MPa ay = BiCp = 0.85(272,189-) = 231.361 mm nl SIMPLIFIED REINFORCED CONCRETE DESIGN CHAPTER 3: ANALYSIS AND DESIGN OF f LYSIS ESIG! BEAMS AND REINFORCED BEAMS. NOM DOUBL Since ay >t 231.361 — 110 = 121.361mm Thus, Gt on5f (Ay + 0.85f2A2 = Asly 0.85 f: (thy) + 0.85/¢ @nbw) = Ashy 0.85(20.7)(110)(900) + 04 {85(20.7)(121.361) (310) = Asp (414) Agp = 5806.431 mm? b. Nominal and ultimate balanced moment capacity Myy = Gs + Co¥2 Myy = 0.85f¢ (thy) iG -5) +0.85f! @ebw)(d-¢ Myy = 0.85(20.7)(110)(900) (460 — “) +0.85(20.7)(121.361)(310) (460 -110-F Mp = 896.989 KN For Balanced condition, 6 = 0.65 OMyy = 0.65(896.989) OM yy = 583.043 kNm MJBCASTRO SIMPLIFIED REINFORC!? ‘CONCRETE DESIG* o Oe en ee ee ee CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY meee REINFORCED BEAMS c. Maximum steel area ae aha = $460) = 197.143 mm max = BrCmax = 0.85(197.143) = 167.572 mm Since dmax > ti 2max = Amax — ¢ = 167.572 — 110 = 57.572 mm Thus, Q+C,=T O.85f/A; + 0.85f/A, = Asfy 0.85,¢ (thy) + 0.85f¢ Zmaxby) = 0.85(20.7)(110)(900) + a 85(20.' Bn 572)(310) = Ay (414) Asmax = 4966.011 mm? 4. Nominal and ultimate maximum moment capacity Mnmax = CY: + Co¥2 i Mama = 0.85fe(tby) (d ~ §) + 0.854! @nazbw) (a-1-") Mnmax = 0.85(20.7)(110)(900) (460 — *) +0.85(20.7(57.572)(310) (460 ~ 110 ~ 7572) Momax = 806.340 kNm For Maximum condition, 9=065+025 = b - o65 4025 S005 458 000 f, Too0— 414 ~ 9815 OMnmax = 0.815(806.340) OMnmax = 657.167 kNm CONCRETE DESK eeecee MJBCASTRO Solution: IL Solve for OMamax Cmax (470) = 201.429 mm B, = 0.85 for fo = 20.7 MPa max = B1Cmax = 0.85(201.429) = 171.215 mm Since amax >t} 2max = Imax ~ ¢ = 171.215 — 100 = 71.215 mm OMnmax = OC1Y1 + OC2y2 OMymax = 00.85 ¢(tby) (d ~ 3) + 00.85/£ émaxby) (d—¢- Reo 5 tg.95 800-4 tooo f, ~ °° + °?° 7900-414 0 = 0.65 + 0.25. ly a (ek TP ee) | | CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY ‘eos. REINFORCED BEAMS 100) OMmax = 01815(0.85)(20.7)(100)(820) (470 - 400) +0.815(0.85)(20.7)(71.215)(250) (470 ~ 100 -) OMymax = 579.239 kNm Il. Check moment capacity of flange @Mny 00 =f =< 2 = 117647 aes on 470 - 1174 ee ee 797 0 600 797.001 MPa f,>1000MPa, tension controlled, = 0.90 a 100. Olay = 86, (d ~ 3) = 0.90(0.85)(207)(100)(820) (470 - 02) OMyy = 545.375 kNm Mp = 150kNm & M, = 120kNm My = 1.2Mp + 1.6M, = 1.2(150) + 1.6(120) = 372 kNm > OMnmax >My design as Singly Reinforced >My 1000 MPa, tension controlled, @ = 0.90 Assumption is correct! SIMPLIFIED REINFORCED CONCRETE DESIGN MJBCASTRO et F CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS A) REINFORCED BEAMS we goueLy G=T O.85flaby = Ash, (0.85) (20.7)(65.521)(820) = As(414) Ag = 2283.407 mm? Flange is in compression, shall be the greater of (a) or (b): Asmin § (a) Asmin = a d= 925V207 (250)(470) = 322.822 mm? (b) Asmin = ite d= 24 (2501470) = = 397.343 mm? Therefore, Ay = 2283.407 mm? Mp = 175kNm & M, = 190kNm b. = 1.2Mp + 1.6M; = 1.2(175) + 1.6(190) = 514 kNm 5 OMpmax > My design as Singly Reinforced My, 1000 MPa, tension controlled, 0 = 0.90 Assumption is cor fe > fy therefore f, = aT 0.85faby = Asfe (0.85)(20.7)(93: 526)(820) = 4,(414) Ag = 3259.381 mm? Coo ee CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS ora Flange is in compression, Asin Shall be the greater of (a) ot (b): o2s/ fe, , _ 0.25V207 (a) Asmin = Ee = Fig (250)(470) = 322.822 mm? 14 14 ae (0) Asmin = yet = Gia (250)(470) = 397.343 mm Therefore, Ay = 3259. 381 mm? Mp = 195kNm &M, = 210kNm My, = 1.2Mp + 1.6M, = 1.2(195) + 1.6(210) = 570 kNm + OMpma > My design as Singly Reinforced >My > OMye, a>t analyze as T— beam Assume @ = 0.90 t z M, =0¢,(¢-5) +06, (a-«-3) 570x 108 = 0,90(0.85)(20.7)(100(820) (470 — Ss) + 0.90(0.85)(20.7)(z)(250) (470 - 100 - 3) 17.212 mm t+z=100+17.212= 117.212 mm a _ 117212 _ 147996 Ani 085 Vignes d-c__ 470-137.896 acne Tagewasrase 1445.019 MPa Je > 1000 MPa, tension controlled, © = 0.90 Assumption is correct! fe > fy therefore f, = fy ,+G= O.85f'A1 + 0.85/A2 = Acf, 0.85 fi tby + 0.85f/zby = Acfy (0.85)(20.7)(100)(820) + (0.85)(20.7)(17.212)(250) = As(414) As = 3667.878 mm? EERE EARN A SIMPLIFIED REINFORCED CONCRETE DESIGN er CHAPTER 3: ANALYSIS AND DESIGN OF T-BEAMS AND DOUBLY REINFORCED BEAMS Flange is in compression, Asmin Shall be the greater of (a) or (b): (0) Agmin = ooVEE pg = 225N207 (950)(470) = 322.822 mm? fy 414 14 14 2 eS pais = 397.343 mm Cb) Apia he byd Fig (25000470) Therefore, A, = 3667.878 mm? Solution: L Solve for cp; 600d 600(600) = =———_ = 1.952 > = Coors mao aa uaa dy = Bycy = 0.85(380.952) = 323.809 mm > t IL. Solve for: 323.809 — 100 = 223.809 mm 2p = ay G+G=T O.B5f'A; + O.85f'Az = Acfy O.B5fthy + 0.85f!2pby = Asp fy (0.85) (20.7)(100)(1500) + (0.85)(20.7)(223.809)(250) = Asy(345) Asp = 10503.564 mm? " Ay = 63 (28)? = 3694.513 mm? As A, 1000 MPa fs > 1000 MPa, tension controlled, @ = 0.90 fe > fy therefore f, = fy Thus, a OM, = 6C.(d-5) OM, = 00.85f’aby (4-5) 48. OM,, = 0.90(0.85)(20.7)(48.294)(1500) (600 ne, OM, = 660.584 kKNm

You might also like