Uploaded by Umar Adil

Chapter # 7 (Part-B)(1)

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Chapter # 7
Design of Two-Way Slabs
(Part-B)
Problem # 4
Compute the positive and negative moments in the column and
middle strips of the exterior panel of the Flat Plate Slab between
columns B and E in figure. The slab is 8 in. thick and supports a
superimposed service dead load of 25 psf and service live load of
60 psf. The edge beam is 12 in wide by 16 in. in overall depth and
is cast monolithically with the slab.
Problem # 4
Column and middle strips
Problem # 4 - Solution
Solution:
1) Compute the factored loads
8
π‘žπ‘’ = 1.2
× 150 + 25 + 1.6 60 = 246 𝑝𝑠𝑓
12
Note: Live load reduction must be carried out if local building
code allows it
2) Compute moments in span BE of the slab
a) Compute 𝑙𝑛 and 𝑙2 (average) and divide the slab into
column and middle strips
Problem # 4 - Solution
1 14
1 16
𝑙𝑛 = 21.0 𝑓𝑑 −
−
= 19.75 𝑓𝑑
2 12
2 12
20
18
𝑙2 =
𝑓𝑑 + 𝑓𝑑 = 19 𝑓𝑑
2
2
The column strip extends the smaller of 𝑙2 Τ4 or
𝑙1 Τ4 on each side of the column centerline.
Because 𝑙1 is greater than either value of 𝑙2 , base this on 𝑙2
The column strip extends 20Τ4 = 5𝑓𝑑 toward AD and
18Τ4 = 4.5𝑓𝑑 toward CF from line BC as shown in figure.
The total width of column strip is 9.5 ft.
The half-middle strip between BE and CF has a width of
4.5 ft, and the other one is 5 ft, as shown
Problem # 4 - Solution
b) Compute 𝑀𝑂
π‘žπ‘’ 𝑙2 𝑙𝑛2
𝑀𝑂 =
8
0.246 × 19 × 19.752
→ 𝑀𝑂 =
= 228 π‘˜π‘–π‘ − 𝑓𝑑
8
c) Divide MO into negative and positive moments
The distribution of the moment to the negative and positive regions is as given by Table 13-2
(refer next slide). In the terminology of Table 13-2, this is a “slab without beams between interior
supports and with edge beam.” From Table 13-2, the total moment is divided as follows:
πΌπ‘›π‘‘π‘’π‘Ÿπ‘–π‘œπ‘Ÿ π‘›π‘’π‘”π‘Žπ‘‘π‘–π‘£π‘’ π‘šπ‘œπ‘šπ‘’π‘›π‘‘ 𝑀𝑒 = −0.70𝑀𝑂 = −0.70 × 228 = −160 π‘˜π‘–π‘ − 𝑓𝑑
π‘ƒπ‘œπ‘ π‘–π‘‘π‘–π‘£π‘’ 𝑀𝑒 = 0.50𝑀𝑂 = 0.50 × 228 = +114 π‘˜π‘–π‘ − 𝑓𝑑
𝐸π‘₯π‘‘π‘’π‘Ÿπ‘–π‘œπ‘Ÿ π‘›π‘’π‘”π‘Žπ‘‘π‘–π‘£π‘’ π‘šπ‘œπ‘šπ‘’π‘›π‘‘ 𝑀𝑒 = −0.30𝑀𝑂 = −0.30 × 228 = −68.4 π‘˜π‘–π‘ − 𝑓𝑑
Problem # 4 - Solution
Problem # 4 - Solution
d) Divide the moments between the column and middle strips
(i) Interior Negative Moments
This division is a function of 𝛼𝑓1 𝑙2 Τ𝑙1 , which equals zero, because there are no beams parallel to BE.
Using Table 13-3,
Interior Column − strip negative moment = 0.75 × −160 = −120 π‘˜π‘–π‘ − 𝑓𝑑
−120
=
= −12.6 π‘˜π‘–π‘ − 𝑓𝑑/𝑓𝑑 width of column strip
9.5 (π‘€π‘–π‘‘π‘‘β„Ž π‘œπ‘“ π‘π‘œπ‘™π‘’π‘šπ‘› π‘ π‘‘π‘Ÿπ‘–π‘)
Interior Middle − strip negative moment = 0.25 × −160 = −40 π‘˜π‘–π‘ − 𝑓𝑑
Half of this goes to each half-middle strips beside column strip BE
Problem # 4 - Solution
Problem # 4 - Solution
(ii) Positive Moments
This division shall be carried out as per Table 13-4, shown below
Problem # 4 - Solution
Column − strip positive moment = 0.60 × 114 = 68.4 π‘˜π‘–π‘ − 𝑓𝑑
Middle − strip positive moment = 0.40 × 114 = 45.6 π‘˜π‘–π‘ − 𝑓𝑑
Half of this goes to each half-middle strip
(iii) Exterior Negative Moments
As per Table 13-5, the division of exterior
negative moment is a function of
𝛼𝑓1 𝑙2 Τ𝑙1 , which is again equal to zero,
because there are no beams parallel to 𝑙1 . Also:
𝐸𝑐𝑏 𝐢
𝛽𝑑 =
𝐸𝑐𝑠 𝐼𝑠
and
𝐢=෍
π‘₯
1 − 0.63
𝑦
π‘₯ 3𝑦
3
The 𝐸𝑐𝑏 and C refer to the attached torsional member
shown in figures on slide # 13
Problem # 4 - Solution
Computation of value of “C”
To compute C, divide the edge beam into
rectangles. The two possibilities are shown
in figures opposite. Considering figure-a:
𝐢=෍
π‘₯
1 − 0.63
𝑦
π‘₯ 3𝑦
3
(a) Attached torsion member
(b) Attached torsion member
1 − 0.63 × 12Τ16 123 × 16
1 − 0.63 × 8Τ8 83 × 8
𝐢 𝑓𝑖𝑔. −π‘Ž =
+
= 5367 𝑖𝑛.4
3
3
1 − 0.63 × 20Τ8 203 × 8
1 − 0.63 × 12Τ8 123 × 8
𝐢 𝑓𝑖𝑔. −𝑏 =
+
= 3741 𝑖𝑛.4
3
3
Problem # 4 - Solution
Larger of the two governs
→ 𝐢 = 5367 𝑖𝑛.4
Is is the moment of inertia of the strip of slab section perpendicular to the
edge, which has b = 8 in., then
12 × 19 × 83
𝐼𝑠 =
= 9728 𝑖𝑛.4
12
Because 𝑓𝑐′ is the same in slab and beam, 𝐸𝑐𝑏 = 𝐸𝑐𝑠 and
𝐸𝑐𝑏 𝐢
𝛽𝑑 =
𝐸𝑐𝑠 𝐼𝑠
5367
→ 𝛽𝑑 =
= 0.276
2 9728
Problem # 4 - Solution
Interpolating from Table 13-5, we
get:
𝛽𝑑 = 0:
100 π‘π‘’π‘Ÿπ‘π‘’π‘›π‘‘ π‘œπ‘“ π‘π‘œπ‘™π‘’π‘šπ‘› π‘ π‘‘π‘Ÿπ‘–π‘
𝛽𝑑 = 2.5: 75 π‘π‘’π‘Ÿπ‘π‘’π‘›π‘‘ π‘œπ‘“ π‘π‘œπ‘™π‘’π‘šπ‘› π‘ π‘‘π‘Ÿπ‘–π‘
⇒ π‘“π‘œπ‘Ÿ 𝛽𝑑 = 0.276,
97.2 π‘π‘’π‘Ÿπ‘π‘’π‘›π‘‘ π‘œπ‘“ π‘π‘œπ‘™π‘’π‘šπ‘› π‘ π‘‘π‘Ÿπ‘–π‘
Exterior Column − strip negative moment = 0.972 × (−68.4) = −66.5 π‘˜π‘–π‘ − 𝑓𝑑
= −7 π‘˜π‘–π‘ − 𝑓𝑑 /𝑓𝑑
Exterior Middle − strip negative moment = 0.028 × (−68.4) = −1.92 π‘˜π‘–π‘ − 𝑓𝑑
Problem # 4 - Solution
Flow diagram of the calculation of moments in an
exterior span of a two-way flat-plate slab
Class Work Problem
Compute the column strip and middle moments in the direction
perpendicular to the edge of the exterior bay of the flat plate slab
shown in figure on next slide. The slab is 7.5 in. thick and supports
a superimposed service dead load of 25 psf and service live load of
50 psf. There is NO edge beam and columns are all 18 in. square.
Class Work Problem
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