concret o
TRANSCRIPT
1
CHAPTER 3 FLEXURAL ANALYSIS OF REINFORCED CONCRETE BEAMS
Problem 3.1 a ( ρmax = 0.01806, ρ min = 0.00333 ) for all problems. Given: b = 14 in, d = 22.5 in, As = 5.08 in2, fc’ = 4 ksi, fy = 60 ksi Solution: φ = 0.9
a =A ff bs y
c085. ' = 5 08 60
0 85 4 14.
.×
× × = 6.4 in.
φMn = φAsfy (d - a/2) = 0.9 × 5.08 × 60 × (22.5 - 6.4/2) = 5294 k.in. = 441.2 k.ft
ρ = As / bd = 5 0814 22 5
..×
= 0.016
ρ < ρmax = 0.01806, ρ > ρmin = 0.00333 Ok General Equations:
a =A ff bs y
c085. ' ,
ρ = As / bd,φMn = φAsfy (d - a/2) Problem 3.1
DIM. Prob. No.a
Prob. No.b
Prob. No.c
Prob. No.d
Prob. No.e
Prob. No.f
Prob. No.g
Prob. No.h
b (in.) 14 18 12 12 16 14 10 20 d (in.) 22.5 28.5 23.5 18.5 24.5 26.5 17.5 31.5
As (in.2) 4#10 5.08
6#10 7.62
4#9 4.00
4#8 3.16
5#10 6.35
5#9 5.00
3#9 3.00
4#9 4.00
a(in.) 6.4 7.47 5.88 4.65 7.00 6.3 5.29 3.53
φMn(k.ft) 441.2 849.1 370.1 230.0 600.0 525.3 200.5 535.2
ρ 0.0161 0.0149 0.0142 0.0142 0.0162 0.0135 0.0171 0.0063
ρmax<ρ<ρmin Yes Yes Yes Yes Yes Yes Yes Yes
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Problem 3.2a ( ρmax = 0.01806, ρ min = 0.00333 ) for all problems. Typical Solution, comp. steel yields Given: b = 15 in, d = 22.5 in, As = 8 in2, As’ = 2 in2 , fc’ = 4 ksi, fy = 60 ksi Solution: φ = 0.9
ρ = As/bd = 815 22.5×
= 0.0237
ρ’ = As’/bd = 215 22.5×
= 0.0059
ρ - ρ’ = 0.0237 - 0.0059 = 0.0178
k = 085 8787
2.' '× × ×
−ff
dd f
c
y y
= 085 460
2 522 5
8787 60
2. ..
× × ×−
= 0.0172
ρ - ρ’ = 0.0178 > k = 0.0172, Compression steel yields.
a =bffAA
c
yss
'85.0)'( −
=(8 2) 600.85 4 15− ×
× ×= 7.06 in.
φMn = φ[(As - As’) fy (d - a/2)+ As’fy(d-d’)]
= 0.9[( 8 - 2)×60×(22.5 - 7.06/2) + 2×60(22.5-2.5)]= 8306.5 k.in. = 692.2 k.ft
ρmax < ( ρ - ρ’ )< ρ min , OK General Equations:ρ = As/bd, ρ’ = As’/bd,
a =bffAA
c
yss
'85.0)'( −
,
k = 085 8787
2.' '× × ×
−ff
dd f
c
y y
A = 0.85 fc’β1b, B = As’ (87 - 0.85 fc’) - As fy, C = -87As’d’ c = [-B ± ACB 42 − ] / 2A fs’= 87( c - d’ )/c ≤ fy, C1 = 0.85 fc’ab, C2 = As’ (fs’- 0.85 fc ’) Comp. steel yields:
a =bffAA
c
yss
'85.0)'( −
,
φMn = φ[(As - As’)fy (d - a/2)+ As’fy(d-d’)]
3
4
3.2 e: Typical solution, Comp. steel does not yield. Given: b = 14 in., d = 20.5 in., As = 7.62 in.2, As’ = 2.54 in.2 , fc’ = 4 ksi, fy = 60 ksi Solution: φ = 0.9
ρ = As/bd = 5.2014
62.7×
= 0.0266
ρ’ = As’/bd = 2 5414 20 5
..×
= 0.0089
ρ - ρ’ = 0.0266 - 0.0089 = 0.0177
k = 085 8787
2.' '× × ×
−ff
dd f
c
y y
= 085 460
2 520 5
8787 60
2. ..
× × ×−
= 0.0189
ρ - ρ’ = 0.0177 < k = 0.0189, Compression steel doesn’t yield. A = 0.85 fc’β1b = 0.85 × 4 × 0.85 × 14 = 40.46 B = As’ (87 - 0.85 fc’) - As fy = 2.54(87 - 0.85 ×4) - 7.62 ×60 = - 244.9 C = -87As’d’ = - 87 ×2.54 ×2.5 = - 552.45 c = [-B ± ACB 42 − ] / 2A = 7.8 in. a = β1c = 0.85 ×7.8 = 6.63 in. fs’= 87( c - d’ )/c = 87( 7.8 - 2.5 )/7.8 = 59.1 ksi ≤ fy
Cc = 0.85 fc’ab = 0.85 × 4 × 6.63 × 14 = 315.7 k Cs = As’ (fs’- 0.85 fc ’) = 2.54(59.1 - 0.85 ×4) = 141.48 k As1 = Cc / fy = 315.7/60 = 5.26 in.2
ρ1 = As1 / bd = 5.26/(14 × 20.5) = 0.0183 < ρmax
φMn = φ[ Cc (d - a/2)+ Cs(d-d’)] = 0.9[315.7×(20.5 - 6.63/2) + 141.48×(20.5-2.5)]= 7173.2 k.in. = 597.9 k.ft
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Problem 3.2
DIM. Prob. No.a
Prob. No.b
Prob. No.c
Prob. No.d
Prob. No.e
Prob. No.f
Prob. No.g
Prob. No.h
b (in.) 15 17 13 10 14 16 20 18
d (in.) 22.5 24.5 22 21.5 20.5 20.5 18 20.5
As (in.2) 8#9 8.00
8#10 10.08
7#9 7.00
4#10 5.08
6#10 7.62
9#9 9.00
12#9 12.00
8#10 10.12
As’(in.2) 2#9 2.0
2#10 2.54
3#7 1.8
2#7 1.2
2#10 2.54
4#9 4.0
6#9 6.0
4#10 5.08
ρ 0.0237 0.0242 0.0245 0.0236 0.0266 0.0274 0.0333 0.0275
ρ’ 0.0059 0.0061 0.0063 0.0056 0.0089 0.0122 0.0167 0.0138
ρ- ρ’ 0.0178 0.0181 0.0182 0.0180 0.0177 0.0152 0.0167 0.0137
k 0.0172 0.0158 0.0176 0.0180 0.0189 0.0189 0.0216 0.0189
a ( in.) 7.06 7.83 7.06 6.85
φ Mn 692.2 950 590.2 418.2
A 40.46 46.24 57.8 52.6
B -244.9 -205.6 -218.4 -184.9
C -552.45 -870 -1305 -1100.49
c 7.8 7.097 7.0 6.7
a 6.63 6.033 5.95 5.71
fs’ 59.1 56.36 55.94 54.62
C1 315.7 328.2 504.8 349.4
C2 141.5 211.8 315.2 260.2
As1 5.26 5.47 6.75 5.82
ρ1 0.0183 0.0167 0.0187 0.0158
ρ1≤ρmax Yes Yes Yes Yes
φ Mn 597.9 716.3 822.5 813.7
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Problem 3.3 a: Typical solution of T-sections, Rect. Section analysis. Given: bw = 14 in., b = 54 in., t = 3 in., d = 17.5 in., As = 5.08 in.2,
fc’ = 3 ksi, fy = 60 ksi Solution: φ = 0.9
a =A ff bs y
c085. ' =
54385.06008.5××
× = 2.213 in. < t
c = 2.6 in. dt = 17.5 in. εt = 0.003(dt – c)/c = 0.0172 > 0.005 Rectangular section analysis φMn = φAsfy ( d - a/2 ) = 0.9 × 5.08 × 60 × (17.5 – 2.21/2) = 4497 k.in. = 374.7 k.ft Asmax = 0.0425 [t (be-bw) + 0.319bwd] = 0.0425 [3(54-14) + 0.319×54×17.5]) = 8.42 in.2
Asmin = ρminbwd = 0.00333 ×14×17.5 = 0.81 in.2
Asmin < As< Asmax Ok Problem 3.3 d: Typical solution of T-sections analysis. Given: bw = 16 in., b = 32 in., t = 3 in., d = 15.5 in., As = 6 in.2, fc’ = 3 ksi, fy = 60 ksi Solution:
a =A ff bs y
c085. ' =
32385.0606
××× = 4.41 in. > t
T-section Asmax = 0.0425 [t (be-bw) + 0.319bwd] = 0.0425 [3(32-16) + 0.319×16×15.5]
= 5.40 in.2
As = 6 in2 > Asmax N.G. Section doesn’t meet ACI Code. If ρmax is used: Asf = 0.85 fc’t(b-bw)/fy = 0.85×3×3× (32-16) /60 =2.04 in.2
Mflange = φAsffy (d - t/2) = 0.9 × 2.04 × 60 (15.5 – 3/2) = 1542.24 k.in. = 128.52 k.ft As1 (web) = 5.40 – 2.04 = 3.36 in.2
a = 3.36 600.85 3 16
×× ×
= 4.94 in.; c = 5.81 in.
dt = 15.5 + 1 = 16.5 in. εt = 0.003(dt – c)/c = 0.0055 > 0.005 φMn (web)= φAs1fy ( d - a/2 ) = 0.9 × 3.36× 60 × (15.5 – 4.94/2)/12 = 197.01 k.ft Total φMn = 128.52 + 197.01 = 325.53 k.ft
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Problem 3.3 e: Typical solution of T-sections analysis. Given: bw = 12 in., b = 44 in., t = 4 in., d = 20.5 in., As = 8 in.2, fc’ = 3 ksi, fy = 60 ksi Solution: φ = 0.9
a =bf
fA
c
ys
'85.0=
44385.0608
××× = 4.27 in. > t
T-section Asf = 0.85 fc’t(b-bw)/fy
= 0.85×3×4× (44-12) /60 = 5.44 in.2
a =wc
ysfs
bffAA
'85.0)( −
=12385.060)44.58(
×××− = 5.02 in.
c = 5.906 in. dt = 21.5 in. εt = 0.003(dt – c)/c = 0.0079 > 0.005 φMn = φ[(As - Asf ) fy ( d - a/2 ) + Asf fy ( d - t/2 ) = 0.9[(8 – 5.44)×60(20.5 – 5.02/2) + 5.44 × 60(20.5 – 4/2) = 7921 k.in. = 660.1 k.ft Asmax = 0.0425 [t (be-bw) + 0.319bwd] = 0.0425 [4(44-12) + 0.319×12×20.5]
= 8.77 in.2
Asmin = ρminbwd = 0.00333 ×12×20.5 = 0.82 in.2
Asmin < As< Asmax Ok Problem 3.3
DIM. Prob. No.a
Prob.No.b
Prob.No.c
Prob.No.d
Prob.No.e
Prob.No.f
Prob.No.g
Prob.No.h
b ( in.) 54 48 72 32 44 50 40 42 bw ( in.) 14 14 16 16 12 14 16 12 t ( in. ) 3 4 4 3 4 3 3 3 d ( in. ) 17.5 16.5 18.5 15.5 20.5 16.5 16.5 17.5
As (in.2) 4#10 5.08
4#9 4.00
8#10 10.16
6#9 6.00
8#9 8.00
7#9 7.00
5#10 6.35
6#9 6.00
a ( in. ) 2.213 1.961 3.32 4.41 4.27 3.29 3.74 3.36 Rect. or T R R R T T T T T φMn (k.ft) 374.7 279.4 769.9
Asmin< As < Asmax Yes Yes Yes Asf (in.2) 2.04 5.44 4.59 3.06 3.83a ( in. ) 4.94 5.02 4.05 4.84 4.25
φMn (k.ft) 293.41 660.1 466.8 415 425.9
Asmin< As < Asmax No Yes Yes Yes Yes
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9
3.4 a: Typical Solution: Given: b = 12 in., d = 20 in., As = 3.14 in.2, fc’ = 3 ksi, fy = 40 ksi Solution: ρb = 0.85β1(fc’/fy)[87/( 87+ fy)] = 0.85 ×0.85( 3/40 ) × [87/(87+40)] = 0.0371 ρmax = 0.5474ρb = 0.5474 × 0.0371 = 0.0203
Ru(max) = φρmax fy ( )'7.1
1 max
c
y
ffρ
−
= 0.9 ×0.0203×40 ( )0.0203 4011.7 3
×−
×= 0.615 ksi
ρ = As / bd = 3.14/ (12×20) = 0.01308
Ru = φρ fy ( )'7.1
1c
y
ffρ
−
= 0.9 ×0.01308×40 ( )37.1
4001308.01×
×− = 0.4226 ksi
a / d ratio = '85.0 c
y
ffρ
=385.0
4001308.0×× = 0.2052
(a / d) max = '85.0
max
c
y
ffρ
= 0.0203 400.85 3
××
= 0.319
Problem 3.4 e: Typical Solution:
Given: b = 300 mm, d = 500mm, As = 3× ( )430 2π = 2121mm2, fc’ = 30Mpa, fy = 400Mpa
Solution: ρb = 0.85β1(fc’/fy)[600/( 600+ fy)] = 0.85 ×0.85(30/400) × [600/ (600+400)] = 0.0325 ρmax = 0.625ρb = 0.625× 0.0325 = 0.0203
Ru(max) = φρmax fy ( )'7.1
1 max
c
y
ffρ
−
= 0.9 ×0.0203×400 ( )0.0203 40011.7 30
×−
×= 6.14 Mpa
ρ = As / bd = 2121/(300×500) = 0.01414
Ru = φρ fy ( )'7.1
1c
y
ffρ
− = 0.9 ×0.01414×400 ( )307.1
40001414.01×
×− = 4.53 Mpa
a / d ratio = '85.0 c
y
ffρ
=3085.0
40001414.0×× = 0.2218
(a/ d) max = '85.0
max
c
y
ffρ
= 0.0203 4000.85 30
××
= 0.3184
10
Problem 3.4
DIM. Prob. No.a
Prob. No.b
Prob. No.c
Prob. No.d
Prob. No.e
Prob. No.f
Prob. No.g
Prob. No.h
fc’ 3 ksi 4 ksi 4 ksi 5 ksi 30 Mpa 20 Mpa 30 Mpa 25 Mpa
fy 40 ksi 60 ksi 75 ksi 60 ksi 400 Mpa 300 Mpa 500 Mpa 300 Mpa
b 12 in. 12 in. 12 in. 12 in. 300 mm 300 mm 300 mm 300 mm
d 20 in. 20 in. 20 in. 20 in. 500 mm 500 mm 500 mm 500 mm
As(in.2)(mm2)
4#8
3.14
4#7
2.41
4#9
4.00
4#9
4.00
3*30 mm
2121mm2
3*25 mm
1473
4*25 mm
1963
4*20 mm
1257
β1 0.85 0.85 0.85 0.8 0.85 0.85 0.85 0.85
ρb 0.0371 0.0285 0.0207 0.0335 0.0325 0.0321 0.0236 0.04
ρmax 0.0203 0.0181 0.0145 0.0212 0.0203 0.01805 0.0162 0.0225
Rumax 0.614
ksi 0.821
ksi 0.822
ksi 0.973
ksi 6.14 Mpa
4.11 Mpa
6.13 Mpa
5.11 Mpa
ρ 0.0131 0.01004 0.01667 0.01667 0.01414 0.00982 0.01309 0.0084
Ru0.4227
ksi 0.4942
ksi 0.9182
ksi 0.7941
ksi 4.52 Mpa
2.42 Mpa
5.13 Mpa
2.13 Mpa
a/d ratio 0.2052 0.1772 0.3676 0.2353 0.2218 0.1732 0.2567 0.118
(a/d) max 0.3184 0.3194 0.3199 0.2993 0.3184 0.3194 0.3176 0.3176
ρmin<ρ<ρmax Yes Yes No Yes Yes Yes Yes Yes
3.5 a: Given: b = 250 mm, d = 550mm, As = 4×20mm, fc’ = 20 Mpa, fy = 420 Mpa Solution:
As = 4× ( )420 2π = 1256.6mm2
ρ = As / bd = 1256.6/(250×550) = 0.00914
Ru = φρ fy ( )'7.1
1c
y
ffρ
−
= 0.9 ×0.00914×420 ( )207.1
42000914.01×
×− = 3.6 Mpa
φMn = Ru bd2 =3.6×106×0.25×0.552 = 272.3 KN.m ρb = 0.85β1(fc’/fy)[600/( 600+ fy)] = 0.85 ×0.85(20/420) × [600/ (600+420)] = 0.02024 ρmax = 0.6375ρb = 0.6375× 0.02024 = 0.0129 Ok
11
3.5 b: Given: b = 250 mm, d = 550mm, As = 3×25mm, fc’ = 20 Mpa, fy = 420 Mpa Solution:
As = 3× ( )425 2π = 1472 mm2
ρ = As / bd = 1472 / (250×550) = 0.0107 ρb = 0.85β1(fc’/fy)[600/( 600+ fy)] = 0.02024 ρmax = 0.6375ρb = 0.0129 ρ < ρmax Ok
Ru = φρ fy ( )'7.1
1c
y
ffρ
−
= 0.9 ×0.0107×420 ( )0.0107 42011.7 20
×−
×= 3.51 Mpa
φMn = Ru bd2 =3.51×0.25×0.552
= 265.4 KN.m 3.5 c: Given: b = 250 mm, d = 550mm, As = 4×30 mm, fc’ = 20 Mpa, fy = 420 Mpa Solution:
As = 4× ( )430 2π = 2827 mm2
ρ = As / bd = 2827/ (250×550 ) = 0.02056 ρmax = 0.0129 ρ> ρmax N.G. , Section does not meet ACI code, reduce steel.
Ru(max) = φρmax fy ( )'7.1
1 max
c
y
ffρ
−
= 0.9 ×0.0129×420 ( )0.0129 42011.7 20
×−
×= 4.1 Mpa
φMn = Ru (max) bd2 = 4.1×0.25×0.552
= 310 KN.m
12
3.5 d: Given: b = 10 in., d = 22 in., As = 2.0 in.2, fc’ = 3 ksi, fy = 60 ksi Solution: ρ = As / bd = 2/(10×22) = 0.0091 ρb = 0.85β1(fc’/fy)[87/( 87+ fy)] = 0.85 ×0.85(3/60) × [87/ (87+60)] = 0.0214 ρmax = 0.01356 ρmin < ρ < ρmax Ok
Ru = φρ fy ( )'7.1
1c
y
ffρ
−
= 0.9 ×0.0091×60 ( )0.0091 6011.7 3
×−
×= 0.439 ksi
φMn = Ru bd2 = 0.439×10×222 = 2124 k.in. = 177 k.ft
3.5 e: Given: b = 10 in., d = 22 in., As = 6.0 in.2, fc’ = 3 ksi, fy = 60 ksi Solution: ρ = As / bd = 6/(10×22) = 0.02727 ρmax = 0.01356 < ρ N.G. , Section does not meet ACI code, reduce steel.
Ru(max) = φρmax fy ( )'7.1
1 max
c
y
ffρ
−
= 0.9 ×0.01356×60 ( )0.01356 6011.7 3
×−
×= 0.615 Ksi
φMn = Ru(max) bd2 =0.615×10×222 = 2976.6 k.in. = 248.1 k.ft
13
3.6: Given: b = 8 in., d = 18 in., fc’ = 3 ksi, fy = 50 ksi Solution:
(a) εy =Ef y =
2900050 = 0.00172, εc = 0.003
εy > εs = 0.0015 This section is over- reinforced.
(b) dcb =
00172.0003.0003.0
+
cb =00172.0003.0
003.0+
× 18 = 11.44 in.
ab = β1cb = 0.85×11.44 = 9.725 in. 0.85fc’ab b = Asbfy
Asb =y
bc
fbaf '85.0
=50
8725.9385.0 ××× = 3.97 in.2
(c) dc =
0015.0003.0003.0+
c =0015.0003.0
003.0+
× 18 = 12 in.
a = β1c = 0.85×12 = 10.2 in. fs = Esεs = 29000×0.0015 = 43.5 ksi 0.85fc’a b = Asfs
As = 0.85 'cs
f a bf
=5.43
82.10385.0 ××× = 4.783 in.2
φMn = φAsfs (d - a/2) = 0.9×4.783×43.5(18 – 10.2/2) = 2416 k.in. = 201.3 k.ft From tables: ρmax = 0.01628 As max = ρmax bd = 0.01628×8×18 = 2.34 in.2
a = max
0.85 's y
c
A ff b
= 2.34 500.85 3 8
×× ×
= 5.74 in.
(max) φMn = φAsmaxfy (d - a/2 ) = 0.9×2.34×50(18 – 5.74/2) = 1593.2 k.in. = 132.8 k.ft (max) φMn allowed by ACI code is less than φMn of the section = 201.3 k.ft (d) ρ = 0.014 < ρmax As = ρbd = 0.014×8×18 = 2.016
a =bf
fA
c
ys
'85.0=
8385.050016.2××
× = 4.941 in.
φMn = φAsfy (d - a/2) = 0.9×2.016×50(18 – 4.941/2) = 1408.8 k.in. = 117.4 k.ft
14
15
Problem 3.7: Given: b = 12 in., d = 24 in., L = 10 ft, As = 3.93 in.2, fc’ = 3 ksi, fy = 60 ksi Solution:
a =bf
fA
c
ys
'85.0=
12385.06093.3××
× = 7.706 in.
φMn = φAsfy (d - a/2) = 0.9×3.93×60(24 – 7.706/2) = 4275.6 k.in. = 356.3 k.ft
Mu = 1.2(2
2lWD ) + 1.6(2
2lWL ) = φMn
1.2(2
10685.0 2× ) + 1.6(2102×lW ) = 356.3
Wl = 3.94 k/ft
Problem 3.8: Given: b = 10 in. h = 28 in., d = 24.5 in., L = 17 ft, As = 3.53 in.2, fc’ = 3 ksi, fy = 40 ksi Solution:
a =bf
fA
c
ys
'85.0=
10385.04053.3××
× = 5.537 in
φMn = φAsfy (d - a/2) = 0.9×3.53×40(24.5 – 5.537/2) = 2761.6 k.in = 230.1 k.ft
Mu = 1.2(8
2lWD ) + 1.6(4lpL ) = φMn
1.2(8
1755.2 2× ) + 1.6(417×Lp ) = 230.1
Pl = 17.6 k
Problem 3.9 a: Given: b = 12 in., d = 20 in., As = 3.14 in.2, fc’ = 4 ksi, fy = 60 ksi Solution: (1) At balanced condition
dcb =
00207.0003.0003.0
+cb = 11.834 in.
ab = β1cb = 0.85×11.834 = 10.059 in. C = 2×0.85fc’×3×4 + 0.85 fc’×12(10.059 – 4) = 328.8 k Asb = C/fy = 328.8/60 = 5.48 in.2
Asmax = 0.63375Asb = 0.63375×5.48 = 3.473 in.2
As < Asmax
16
(2) T = Asfy = 3.14×60 = 188.4 k T = C = 2×0.85 fc’×3×4 + 0.85 fc’×12(a – 4) 188.4 = 2×0.85×4×3×4 + 0.85×4×12(a – 4) a = 6.618 in C1= 2×0.85fc’×3×4 = 81.6 kC2= 0.85 fc’×12(a – 4) = 0.85×4×12(6.618 – 4) = 106.8 k
φMn = φ[C1( d - 4/2 )+ C2( d – 4 -2
4−a )]
= 0.9[81.6( 20 - 4/2 )+ 106.8( 20 – 4 - 2
4618.6 − )]
= 2734 k.in = 227.83 k.ft
Problem 3.9 b: Given: b = 12 in., d = 16 in., As = 3.93 in.2, fc’ = 4 ksi, fy = 60 ksi Solution: (1) At balanced condition
dcb =
00207.0003.0003.0
+cb = 9.467 in.
ab = β1cb = 0.85×9.467 = 8.047 in. C = 0.85 fc’×5×4 + 0.85 fc’×12(ab – 4 ) = 233.1 kAsb = C/fy = 233.1/60 = 3.89 in.2
Asmax = 0.63375Asb = 0.63375×3.89 = 2.465 in.2
As = 3.93> Asmax , N.G. Section does not meet ACI code, reduce steel. (2) Use As = As max = 2.465 in.2
T = Asfy = 2.465×60 = 147.9 kT = C = 0.85 fc’×5×4 + 0.85 fc’×12(a – 4) 174.85 = 0.85×4×5×4 + 0.85×4×12(a – 4) a = 5.96 in. C1= 0.85fc’×5×4 = 68 kC2= 0.85 fc’×12(a – 4) = 0.85×4×12(5.96 – 4) = 79.97 k
φMn = φ[C1( d – 4/2 )+ C2( d – 4 –2
4−a )]
= 137.5 K.ft
17
Problem 3.10 a: Given: b = 12 in., d = 18in., d’ = 2.5in., As = 2.41 in.2, As’ = 1.2 in.2, fc’ = 3ksi, fy = 40ksi Solution:
ρ = As/bd = 1812
41.2×
= 0.011157
ρ’ = As’/bd = 1812
2.1×
= 0.00556
ρ - ρ’ = 0.005597 < ρmax = 0.0203
k = 085 8787
2.' '× × ×
−ff
dd f
c
y y
=4087
8718
5.240385.0 2
−××× = 0.0139
ρ - ρ’ < k = 0.0139, Compression steel doesn’t yield. A = 0.85 fc’β1b = 0.85 × 3 × 0.85 × 12 = 26.01 B = As’ ( 87 - 0.85 fc’) - As fy = 1.2( 87 - 0.85 ×3) – 2.41 ×40 = 4.94 C = -87 As’d’ = - 87 ×1.2 ×2.5 = - 261 c = [-B ± ]B AC2 4− / 2A = 3.07 in. a = β1c = 0.85 ×3.07 = 6.61 in. fs’= 87( c - d’ )/c = 87( 3.07 - 2.5 )/3.07 = 16.15 ksi ≤ fyC1 = 0.85 fc’ab = 0.85 × 3 × 2.61 × 12 = 79.85 k C2 = As’ ( fs’- 0.85 fc ’) = 1.2( 16.15 - 0.85 ×3 ) = 16.32 k As1 = C1 / fy = 79.85/40 = 1.996 in.2
ρ1 = As1 / bd = 1.996/(12 × 18) = 0.009242 < ρmax φMn = φ[ C1(d - a/2 )+ C2(d-d’)]
= 0.9[79.85×(18 – 2.61/2) + 16.32×(18-2.5)] = 1428 k.in. = 119 k.ft Problem 3.10 b: Given: b = 12 in., d = 18 in., As = 4.82 in.2, As’ = 1.2 in.2, fc’ = 3 ksi, fy = 40 ksi Solution:
ρ = As/bd = 4.8212 18×
= 0.0223
ρ’ = As’/bd = 1812
2.1×
= 0.00556
ρ - ρ’ = 0.0167
k = 085 8787
2.' '× × ×
−ff
dd f
c
y y
=4087
8718
5.240385.0 2
−××× = 0.0139
ρ - ρ’ > k = 0.0139, Compression steel yields. ρ - ρ’< ρmax = 0.0203 Ok
a =bffAA
c
yss
'85.0)'( −
= (4.82 1.2) 400.85 3 12
− ×× ×
= 4.73 in.
φMn = φ[(As-As’)fy ( d - a/2 ) + As’fy ( d – d’ ) = 0.9[(4.82-1.2)×40(18 – 4.73/2) +1.2×40(18 – 2.5)] = 2707 k.in. = 225.6 K.ft
18
Problem 3.11: Given: b = 12 in., d = 22 in., d’ = 2.5 in., As’= 1.32 in.2, fc’ = 4 ksi, fy = 60 ksi, l = 16 ft Solution: (1) At balanced condition:
dcb = 0.003
0.003 0.00207+cb = 13.02 in.
ab = β1cb = 0.85×13.02 = 11.07 in.
fs’ = )5.2
(87b
b
cc −
= 13.02 2.587( )13.02
− = 70.3 > 60
Compression steel yields, fs’ = 60 ksi C1 = 0.85 fc’abb = 0.85×4×12×11.07 = 451.66 k C2 = As’ fy = 1.32×60 = 79.2 k T = C1 + C2 = 530.86 k As1b = C1/fy =451.66/60 = 7.53 in.2
As max = 0.63375As1b + As’= 0.63375×7.53+1.32 = 6.09 in.2
(2) ρ = As / bd = 6.0912 22×
= 0.02307
ρ’ = As’/bd = 1.3212 22×
= 0.005
ρ - ρ’ = 0.01807
k = 085 8787
2.' '× × ×
−ff
dd f
c
y y
= 2 4 2.5 870.8560 22 87 60
× × ×−
= 0.0176
ρ - ρ’ > k, Compression steel yields. ρ - ρ’= ρmax Ok
a =bffAA
c
yss
'85.0)'( −
= (6.09 1.32) 600.85 4 12
− ×× ×
= 7.01 in.
φMn = φ[(As-As’)fy ( d - a/2 ) + As’fy ( d – d’ ) = 0.9[(6.09-1.32)×60(22 – 7.01/2) + 1.32×60(22 – 2.5)] = 6153.9 k.in. = 512.8 k.ft Mu = 1.2 MD + 1.6ML = φMn
1.2(8162 2× )+1.6(
2168
LW × )= 512.8
Wl = 8.516 k/ft
19
Problem 3.12 Given: b = 10 in., d = 20 in., d’ = 2.5 in., As = 3.61 in.2, As’ = 0.62 in.2, fc’ = 4 ksi, fy = 60 ksi, l = 10 ft, Wl = 1.25 k/ft, WD = 2 k/ft (excluding self weight) Solution:
ρ = As/bd = 2010
61.3×
= 0.01805
ρ’ = As’/bd = 0.6210 20×
= 0.0031
ρ - ρ’ = 0.015 < ρmax = 0.01806
k = 085 8787
2.' '× × ×
−ff
dd f
c
y y
=6087
8720
5.260485.0 2
−××× = 0.0194
ρ - ρ’ < k , Compression steel doesn’t yield. A = 0.85 fc’β1b = 0.85 × 4 × 0.85 × 10 = 28.9 B = As’ (87 - 0.85 fc’) - As fy = 0.62(87 - 0.85 ×4) – 3.61 × 60 = -165 C = -87 As’d’ = - 87 ×0.62 ×2.5 = - 134.85 c = [-B ± ]B AC2 4− / 2A = 6.44 in. a = β1c = 0.85 ×6.44 = 5.47 in. fs’= 87( c - d’ )/c = 87( 6.44 - 2.5 )/6.44 = 53.23 ksi < fyC1 = 0.85 fc’ab = 0.85 × 4 × 5.47 × 10 = 186 k C2 = As’ ( fs’- 0.85 fc ’) = 0.62( 53.23 - 0.85 ×4 ) = 30.4 k As1 = C1 / fy = 186/60 = 3.1 in.2
ρ1 = As1 / bd = 3.1/(10 × 20) = 0.0155 < ρmax
φMn = φ[ C1 (d - a/2)+ C2(d-d’)] = 0.9[186×(20 – 5.47/2) + 30.4×(20-2.5)]= 3369 k.in. = 280.7 k.ft
WD = 2 + 15.0144
2010 ×× = 2.208 k/ft
WL = 1.25 k /ft
Mu = 1.2 MD + 1.6ML = 1.2(2
2lWD ) + 1.6(2
2lWL ) = φMn
1.2(2
10208.2 2× ) + 1.6(2
1025.1 2× ) = 232.5 k.ft
The internal design moment of 280.7 k.ft is great than the external ultimate moment of 232.5 k.ft, the section is adequate.
20
Problem 3.13: Given: bw= 10 in., t = 4 in., d =18 in., As = 3 in.2, l = 18 ft, b = 9 ft, fc’ = 4 ksi, fy = 60 ksi Solution: (1) Effective width, be= b = 108 in. be= l/4 = 18×12/4 = 54 in. be= 16t+bw = 16×4 +10 = 74 in, use be = 54 in.
(2) a =bf
fA
c
ys
'85.0=
54485.0603
××× = 0.98 in. < t
Rectangular Section (3) φMn = φAsfy (d - a/2) = 0.9×3×60(18 – 0.98/2) = 2836.6 k.in. = 236.4 k.ft Asmin = ρminbwd = 0.00333×10×18 = 0.6 in2
Asmax = 0.0567 [t (be-bw) + 0.319bwd] = 0.0567 [4(54-10) + 0.319×10×18]
= 13.23 in.2
Asmin < As< Asmax Ok Problem 3.14: Given: bw= 10 in., t = 3 in., d =18 in., As = 4.71 in.2, b = 30 in., fc’ = 3 ksi, fy = 60 ksi Solution:
(1) a =bf
fA
c
ys
'85.0=
30385.06071.4××
× = 3.69 in. > t
T section Asmax = 0.0425 [t (be-bw) + 0.319bwd] = 0.0425 [3(30-10) + 0.319×10×18]
= 4.99 in.2 > As Ok (2) Asf = 0.85 fc’t(b-bw)/fy = 0.85×3×3( 30 – 10)/60 = 2.55 in.2
a =( ')
0.85 's s f y
c
A A ff b
−=
10385.060)55.271.4(
×××− = 5.08 in.
φMn = φ[(As-As’) fy ( d - a/2 ) + Asf fy ( d – d’ )] = 0.9[(4.71-2.55)×60(18 – 5.08/2)+2.55×60(18 – 3/2)] = 4075.3 k.in. = 339.6 k.ft
Problem 3.15: a′ = 3.69 in. > t, T-section, Asf = 2.55 in.2, Asw = 2.16 in.2, As(max) = 5.80 in.2,
a = 5.08 in., Mu = 466.78 k-ft. Problem 3.16: Same analysis and answer as 3.14