Evaluation of punching shear strength of voided...

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Magazine of Concrete Research http://dx.doi.org/10.1680/macr.14.00080 Paper 1400080 Received 14/03/2014; revised 14/07/2014; accepted 04/06/2014 ICE Publishing: All rights reserved Magazine of Concrete Research Evaluation of punching shear strength of voided transfer slabs Han and Lee Evaluation of punching shear strength of voided transfer slabs Sang Whan Han Professor of Architectural Engineering, Department of Architectural Engineering, Hanyang University, Seoul, Korea Chang Seok Lee Graduate Student, Department of Architectural Engineering, Hanyang University, Seoul, Korea To satisfy the various space demands of occupants in high-rise buildings, such buildings are often constructed with different structural systems along the height of the building, which causes vertical irregularity in the structural system. In buildings with a vertically irregular structural system, transfer slabs are often used to transfer loads from the upper part to the lower part of the building. The transfer slab can perform more efficiently by placing voids in slab regions that do not resist a high level of slab loads. This study evaluated the punching shear strength of voided transfer slabs by conducting experimental tests on five transfer slab specimens. Based on the test results, methods were developed for accurately calculating the punching shear strength of voided transfer slabs. Notation a width (or diameter) of void b closest distance between two voids (see Table 1 for details) b 0 perimeter of critical section c 1 dimension of square column section d depth of slab d c diameter of circular section d e distance from column face to an assumed critical section d r distance from centre of column to critical section located d/2 from column face d v width of void overlapping the critical section f 9 c average compressive strength of concrete f y yield strength of reinforcement h height of slab h v height of void overlapping the critical section L distance between two supports in experimental set-up l span of slab l/d span-to-depth ratio of transfer slab l r length to be deduced from critical section located d/2 from column face t cover thickness of voided area (see Table 1 for details) V c computed punching shear strength V test measured punching shear strength V test-S measured punching shear strength of reference specimen S Æ s constant used to compute V c in slabs: 40 for interior columns; 30 for edge columns; 20 for corner columns â ratio of long side to short side of column ª ratio of reduced net area to area of original critical section ˜ test displacement at maximum load ˜ test-S displacement at maximum load of reference specimen S º modification factor for lightweight concrete Introduction Occupants of high-rise buildings have various demands on space usage. To satisfy these differing demands, high-rise buildings are often constructed with different structural systems along the height of the building, which causes vertical irregularity in the structural systems. In Korea, residential areas are located in the upper parts of the building while commercial and parking areas are often in the lower parts. For residential areas, bearing wall systems are commonly used, whereas moment frame systems are used in commercial and parking areas to provide open and flexible spaces. Figure 1 shows some examples of buildings with vertically irregular structural systems. To transfer loads between the two different systems along the height of the building, transfer girders and transfer slabs can be used. A transfer slab distributes the load more efficiently than a one-way transfer girder because the transfer slab behaves in two- way action. The depth of a transfer slab is much shallower than that of a transfer girder, which leads to a decrease in building height. The concrete formwork for transfer slabs is also much simpler than that of transfer girders since the transfer slab has a flat surface. Furthermore, because the arrangement of bearing walls is commonly irregular in plan, it is very difficult to construct transfer girders below bearing walls. The amount of concrete required to construct a transfer slab may, however, be greater than that for a transfer girder since the slab thickness is constant throughout the whole floor. The typical thickness of a transfer slab is 1000–3000 mm, which results in a span-to-depth ratio (l/d ) of 2 . 5–5 . 0. The typical range of l/d for 1

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Page 1: Evaluation of punching shear strength of voided …earthquake.hanyang.ac.kr/journal/2014/macr1400080h.pdfEvaluation of punching shear strength of voided transfer slabs Han and Lee

Magazine of Concrete Research

http://dx.doi.org/10.1680/macr.14.00080

Paper 1400080

Received 14/03/2014; revised 14/07/2014; accepted 04/06/2014

ICE Publishing: All rights reserved

Magazine of Concrete Research

Evaluation of punching shear strength ofvoided transfer slabsHan and Lee

Evaluation of punching shearstrength of voided transfer slabsSang Whan HanProfessor of Architectural Engineering, Department of ArchitecturalEngineering, Hanyang University, Seoul, Korea

Chang Seok LeeGraduate Student, Department of Architectural Engineering, HanyangUniversity, Seoul, Korea

To satisfy the various space demands of occupants in high-rise buildings, such buildings are often constructed with

different structural systems along the height of the building, which causes vertical irregularity in the structural

system. In buildings with a vertically irregular structural system, transfer slabs are often used to transfer loads from

the upper part to the lower part of the building. The transfer slab can perform more efficiently by placing voids in

slab regions that do not resist a high level of slab loads. This study evaluated the punching shear strength of voided

transfer slabs by conducting experimental tests on five transfer slab specimens. Based on the test results, methods

were developed for accurately calculating the punching shear strength of voided transfer slabs.

Notationa width (or diameter) of void

b closest distance between two voids (see Table 1 for

details)

b0 perimeter of critical section

c1 dimension of square column section

d depth of slab

dc diameter of circular section

de distance from column face to an assumed critical

section

dr distance from centre of column to critical section

located d/2 from column face

dv width of void overlapping the critical section

f 9c average compressive strength of concrete

f y yield strength of reinforcement

h height of slab

hv height of void overlapping the critical section

L distance between two supports in experimental set-up

l span of slab

l/d span-to-depth ratio of transfer slab

lr length to be deduced from critical section located d/2

from column face

t cover thickness of voided area (see Table 1 for

details)

V c computed punching shear strength

V test measured punching shear strength

V test-S measured punching shear strength of reference

specimen S

Æs constant used to compute V c in slabs: 40 for interior

columns; 30 for edge columns; 20 for corner

columns

� ratio of long side to short side of column

ª ratio of reduced net area to area of original critical

section

˜test displacement at maximum load

˜test-S displacement at maximum load of reference

specimen S

º modification factor for lightweight concrete

IntroductionOccupants of high-rise buildings have various demands on space

usage. To satisfy these differing demands, high-rise buildings are

often constructed with different structural systems along the height

of the building, which causes vertical irregularity in the structural

systems. In Korea, residential areas are located in the upper parts

of the building while commercial and parking areas are often in

the lower parts. For residential areas, bearing wall systems are

commonly used, whereas moment frame systems are used in

commercial and parking areas to provide open and flexible spaces.

Figure 1 shows some examples of buildings with vertically

irregular structural systems.

To transfer loads between the two different systems along the

height of the building, transfer girders and transfer slabs can be

used. A transfer slab distributes the load more efficiently than a

one-way transfer girder because the transfer slab behaves in two-

way action. The depth of a transfer slab is much shallower than

that of a transfer girder, which leads to a decrease in building

height. The concrete formwork for transfer slabs is also much

simpler than that of transfer girders since the transfer slab has a

flat surface. Furthermore, because the arrangement of bearing

walls is commonly irregular in plan, it is very difficult to

construct transfer girders below bearing walls.

The amount of concrete required to construct a transfer slab may,

however, be greater than that for a transfer girder since the slab

thickness is constant throughout the whole floor. The typical

thickness of a transfer slab is 1000–3000 mm, which results in a

span-to-depth ratio (l/d ) of 2.5–5.0. The typical range of l/d for

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normal flat slabs is 20–30. For a floor area of 1000 m2, the weight

of the transfer slab is almost 30 000 kN.

In order to reduce the amount of concrete required for construc-

tion of a transfer slab, voids can be formed in the transfer slab

where the internal shear force is not significant. For proper

distribution of voids in a transfer slab, it is important to estimate

the punching shear strength near a column. Punching shear failure

of flat slabs occurs in a brittle manner without warning, causing

catastrophic slab failure (Gardner et al., 2002). The consequences

of failure of a transfer slab are more catastrophic than failure of

normal individual flat slabs because failure of a transfer slab

results in collapse of the whole structure (Cook, 2012). Further-

more, voided transfer slabs are more susceptible to punching

shear failure than solid slabs.

Numerous research studies have been conducted to evaluate the

punching shear strength of solid flat slabs (Elstner and Hognestad,

1956; Han et al., 2006, 2012; Hawkins et al., 1974; Hueste and

Wight, 1999; Islam and Park, 1976; Kang and Wallace, 2005;

Kinnunen and Nylander, 1960; Pan and Moehle, 1992; Rodrigues,

2012; Sagaseta et al., 2011), but research on evaluating the

punching shear strength of voided flat slabs is limited (Aldejo-

hann and Schnellenbach-Held, 2003; Schnellenbach-Held and

Pfeffer, 2002). So far, research regarding the punching shear

strength of voided transfer slabs with small l/d has not been

reported. Since accurate and systematic methods have not yet

been developed for calculating the punching shear strength of

voided transfer slabs, structural engineers can encounter difficul-

ties when designing such slabs.

In order to fill this knowledge gap, experimental tests were

conducted on four voided transfer slab specimens and one solid

transfer slab considered as the reference specimen. Based on

the test results, an accurate and simplified method for calculat-

ing the punching shear strength of voided transfer slabs was

developed.

Experimental details

Model building and test specimens

Figure 2 illustrates the floor plan and elevation of the ten-storey

model building. The building was designed using the bearing wall

system in the upper nine storeys and the moment frame system in

the first storey. The thickness of the slab was assumed to be

1200 mm and the span length was 5500 mm, resulting in a span-

to-depth ratio (l/d ) of 4.6. Gravity loads on the slab transferred

from the bearing walls were assumed to be a uniform load of

50 kN/m2 on the transfer slab. The wall thickness was taken as

300 mm, with the wall arrangement as shown in Figure 2. The

columns were of 800 mm square section; the column height was

3500 mm. Slab moments and shear forces due to gravity loads

were obtained from finite-element analysis using the commercial

software Midas/gen version 6.3.2 (Midas IT, 2004). Figure 3

shows the moment and shear diagrams used for slab design.

To construct the test specimens, this study considered interior

transfer slabs in the model building as shown in Figure 2(a). Five

one-third scale specimens were made. Four were voided transfer

slab specimens (V1, V2, V3 and V4) and one was a solid transfer

slab (S) used as the reference specimen. Specimen V1 had the

smallest number of voids and V4 had the largest number of

voids. The width and length of the slabs were both 800 mm and

the slab thickness was 400 mm. Both ends of the slab were

extended by a distance of 200 mm to provide a space for

supports. Columns in the specimen were of square section with a

dimension of 267 mm.

To make voids in the slab, circular column type Styrofoam of

diameter 200 mm and height 250 mm was placed in the slab

before casting the concrete. This study considered four different

arrangements of slab voids, as shown in Figure 4. Table 1 gives

detailed information on the specimens. As the specimens were

made in order to evaluate the punching shear strength of transfer

slabs, all had sufficient flexural reinforcement to avoid flexural

failure prior to punching shear failure. The same amount of

(a) (b) (c)

Figure 1. Buildings with vertical irregularities: (a) Seosan Techno

Valley apartments constructed by Daewoo Development Company

Ltd, Kyunggi-do, Korea; (b) Starpark apartments constructed by

POSCO, Bundang-gu, Kyunggi-do, Korea; (c) City Avenue

apartments constructed by POSCO, Pusan, Korea

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flexural reinforcement was placed in all the specimens. Rebars

(D13) of diameter 13 mm and a specified yield strength of

400 MPa were used as flexural reinforcement.

In this study, the main test variables were the existence of voids

in the transfer slabs, the arrangement of the voids and the

location of the voids. Figure 4(a) shows the flexural reinforce-

ment arrangement in the transfer slab specimens. Solid specimen

S is shown in Figure 4(b). Specimens V1 and V2 (Figures 4(c)

and 4(d)) had voids overlapping the critical section. The critical

section specified in ACI 318-11 (ACI, 2011) is located at a

distance of d/2 from the column face (d being the effective slab

depth), as shown in Figure 4. Specimens V1 and V2 had 8 and

12 voids respectively. Specimen V3 (Figure 3(e)) had voids

outside the ACI critical section. Specimen V4 (Figure 3(f)) had

two rows of voids. In the first row, 12 voids overlapped the ACI

critical section. In the second row, 20 voids were placed at d

(¼ 480 mm) from the column face and did not overlap the ACI

critical section.

Figure 5(a) shows the stress–strain curve for concrete obtained

from material tests. The average compressive strength was

33 MPa, which was obtained from strength tests using three

100 3 200 mm cylindrical specimens at the time of testing. The

maximum aggregate size for the concrete was 19 mm and the

slump of the concrete was 100–150 mm. The stress–strain curve of

the D13 reinforcement is shown in Figure 5(b). The specified yield

strength was 400 MPa, but the actual yield and tensile strengths

were determined to be 523 MPa and 604 MPa respectively.

Test set-up and instrumentation

Figure 6(a) shows the test set-up. For convenient application of a

concentrated load to cause punching shear failure, a specimen

was placed upside down and vertical loading was applied in the

downward direction to the top of the column using a hydraulic

jack with a capacity of 3000 kN. A load cell was mounted on the

hydraulic jack at the top of the column. A simple support

condition was maintained by placing rollers along the support

line as shown in Figure 6. In order to measure vertical displace-

ments of the specimen, seven linear variable displacement

transducers (LVDTs) were installed at the positions shown in

Figure 6(b).

Test results

Crack patterns

Figure 7 shows the cracks on the bottom surface of the transfer

slab specimens observed after completing the tests. All specimens

experienced punching shear failure. Most of the cracks in the

voided transfer slab specimens were distributed within a narrow

band at a distance slightly greater than d from the column face

(Figure 7(b)–7(f)). The solid specimen showed more cracks over

a wider area, as shown in Figure 7(a).

Comparing the crack patterns of specimens V1 and V2 with voids

overlapping the ACI critical section at d/2 from the column face

(Figures 7(b) and 7(c)), the number of cracks increased with a

decrease in the number of voids. In specimen V3, with voids

located at d from the column face and not overlapping the ACI

critical section (Figure 7(d)), cracks were observed at a greater

12

4 4 4

5·6

A A�

44

4

12

0·8Shear wall

(a)

12

0·8

3·5

3·5

3·5

3·5

1·2

0·3 0·3

(b)

Transfer slab

Figure 2. Model building: (a) floor plan; (b) elevation (dimensions

in m)

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distance from the column face compared with the other voided

specimens. In specimen V4 with two rows of voids (Figure 7(e)),

sparse cracks were distributed more widely than the other voided

specimens.

Punching shear strength and displacement at maximum

load

Figure 8 shows the force–displacement curves using the force

and displacement values taken from the load cell and the LVDT

at the column centre (Figure 6(b)). Table 2 summarises the

punching shear strengths (V test) and displacements at maximum

load (˜test) of the specimens measured at failure.

The punching shear strength of the voided transfer slab specimens

was as low as 50–70% of that of the reference specimen S

(V test-S). Specimen V4, which had the largest number of voids,

had the least punching shear strength (¼ 51% of V test-S). It was

found that the punching shear strength did not vary with a

constant rate according to an increase in the number of voids.

The net area of the ACI critical section at d/2 from the column

face was calculated by deducting the area of voids overlapping

the critical section from the original critical section. The ratio of

the reduced net area to the area of the original critical section is

represented by ª: As shown in Table 2, the punching shear

strength of the voided transfer slabs did not vary consistently

according to ª, indicating that the punching shear strength

estimated by only considering the ACI critical section located at

d/2 from the column face may not guarantee an accurate

punching shear strength of voided transfer slabs.

Comparing ˜test of the specimens at punching shear failure, solid

specimen S had the largest value of ˜test: Among the voided slab

specimens, specimen V1 had the largest ˜test (88% of that of

specimen S) and specimen V4 had the smallest value of ˜test

(54% of ˜test-S): specimens V1 and V4 respectively had the least

and greatest numbers of voids. Voided specimens V2 and V3

showed ˜test values of 72% and 81% of that of the solid specimen

respectively.

�200

�100

0

100

200

0 2 4 6 8 10 12

Mom

ent:

kN

m/m

Column Column Column

(a)

�300

�200

�100

0

100

200

300

0 2 4 6 8 10 12

Shea

r: k

N/m

Distance: m

Column ColumnColumn

(b)

Figure 3. Moment (a) and shear force (b) diagrams along section

A–A9 shown in Figure 2(a)

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200 200

200

1800 1800

1800

200 200

200

160 13 D13 43 D13 160

Top reinforcement Bottom reinforcement

8 D253 D13

Column section

(a)

Critical section ( /2)d

267

300

400

(b)

200 200540 540360 240360 240 240540 540200 200

200 300 240 240 240 240 240 300 200200 240 240 240 240 420420 200

Void

Void

(c)

100

250

50

(d)

(e) (f)

Figure 4. Transfer slab specimens: (a) arrangement of flexural

reinforcement; (b) specimen S; (c) specimen V1; (d) specimen V2;

(e) specimen V3; (f) specimen V4 (dimensions in mm)

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Prediction of punching shear strength ofvoided transfer slabsAccording to section 11.11.2.1 of ACI 318-11 (ACI, 2011), the

punching shear strength (V c) of two-way slabs without shear

reinforcement is determined as the smallest of the values obtained

from Equations 1–3

V c ¼ 0.33º( f 9c)1=2b0d1:

V c ¼ 0.17 1þ 2

� �º( f 9c)1=2b0d

2:

V c ¼ 0.083Æsd

b0

þ 2

� �º( f 9c)1=2b0d

3:

in which f 9c is the mean compressive strength of concrete (note

that f 9c is defined as the specified compressive strength in ACI

318-11), b0 is the perimeter of the ACI critical section (assumed

to be at d/2 from the column face), � is the ratio of the long side

to the short side of the column, Æs is 40, 30 and 20 for interior,

exterior and corner columns respectively and º is a modification

factor for lightweight concrete. Since normal-weight concrete was

used in this study, º is unity. For the transfer slab specimens tested

in this study, Equation 1 produced the smallest punching shear

strength. Equations 1–3 do not account for the effect of flexural

reinforcement. Although it has been reported that slab flexural

reinforcement strongly affects the punching shear strength and the

failure mechanism (Han et al., 2012; Sagaseta et al., 2011), this

study only considered the equations specified in ACI 318-11.

For slabs with discontinuities, two possible methods can be used

Specimen L: mm h: mm a: mm b: mm hv: mm t: mm f 9c: MPa f y: MPa

S 1800 400 — — — — 33 523

V1 1800 400 200 40 250 50 33 523

V2 1800 400 200 160 250 50 33 523

V3 1800 400 200 40 250 50 33 523

V4 1800 400 200 40 250 50 33 523

L

h

th v

ab

Table 1. Dimensions and reinforcement details of specimens

0

5

10

15

20

25

30

35

0 0·001 0·002 0·003 0·004

Stre

ss: M

Pa

Strain(a)

Strain(b)

0

100

200

300

400

500

600

700

0 0·05 0·10 0·15

Stre

ss: M

Pa

Figure 5. Material test results for (a) concrete and (b) steel

reinforcement (D13)

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for determining the critical section according to ACI 318-11

(ACI, 2011). First, when openings are located in a two-way slab,

the perimeter of the critical section should be reduced according

to section 11.6.1 of ACI 318-11. The second method is to

determine the critical section governing the punching shear

strength of the slab with a discontinuity in slab section. For

example, in two-way slabs with drop panels, two critical sections

should be considered, located at d/2 from the column face and

from the drop panel face (Wight and MacGregor, 2009).

However, a method for calculating the punching shear strength of

voided transfer slabs has not yet been proposed. Schnellenbach-

Held and Pfeffer (2002) reported that the punching shear strength

of voided flat slabs may be calculated using the method used for

solid flat slabs if voids are not located within the critical section.

This observation was made solely based on normal flat plates,

and may not be valid for transfer slabs with very low span-to-

depth ratios. In this study, the punching shear strength of transfer

slabs was calculated using the area of the critical section

determined by three different methods – based on rectangular and

circular critical sections and considering void sections as slab

openings – as described in the following sections.

Punching shear strength based on a rectangular critical

section

First, it was assumed that the critical section is located at a

distance d/2 from the column surface, as shown in Figure 4. In

this method, only voids overlapping the critical section were

deducted from the critical section. As mentioned earlier, of

Equations 1–3, Equation 1 produced the smallest value of Vc. To

consider a reduced critical section due to voids in the slab,

Equation 1 was modified as

V c ¼ 0.33( f 9c)1=2 b0d �X

dvhv

� �4:

where dv and hv are the width and height of voids overlapping

the critical section (Figure 9(a)).

Table 3 summarises errors in the punching shear strength (V c)

predicted by Equation 4 with respect to the actual punching shear

strengths (V test) obtained from the tests. The punching shear

strength predicted by Equation 4 matches the actual punching

shear strengths within less than 50% error apart from specimen

V3. Equation 4 overestimated the punching shear strength of V3

by 70%. Specimen V3 had voids completely outside the ACI

critical section at d/2 from the column surface (Figure 4(e)).

Since voids not overlapping the ACI critical section cannot be

considered in this method, the predicted punching shear strength

of voided specimen V3 was the same as that of solid specimen S.

Punching shear strength based on a circular critical

section

Figure 7 shows that crack patterns obtained were neither perfectly

rectangular nor perfectly circular. ACI 318-11 (ACI, 2011) adopts

a rectangular critical section and this work thus attempted to use

a circular critical section to calculate the punching shear strength.

Accordingly, the square column in the transfer slab specimen was

Hydraulic jack

Load cell

Roller Roller Roller

(a)

200 1800

1800

200

360

360

360

360

180

180

180

180

720

720

200

200

400

300

267

(b)

d

d/2

LVDT

Figure 6. (a) Test set-up of transfer slabs. (b) LVDT locations

(dimensions in mm)

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d d

d d

d

20 cm

20 cm

d d

Load

Crack failure line

45°

d/2 d/2

d/2 d/2

d/2

(a) (b)

(c) (d)

(e) (f)

Figure 7. Crack patterns on transfer slab specimens at failure:

(a) specimen S; (b) specimen V1; (c) specimen V2; (d) specimen

V3; (e) specimen V4; (f) section view

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substituted with an equivalent circular column having the same

cross-sectional area. The diameter of the circular column section

(dc) was calculated from

dc ¼ 2c1(1=�)1=25:

where c1 is the dimension of the square column section.

Again, the critical section was assumed to be located at a distance

d/2 from the column face, as shown in Figure 9(b). To calculate

the area of the critical section, the area of voids overlapping the

critical section was excluded. The punching shear strength was

then calculated using

V c ¼ 0.33( f 9c)1=2 2�drd �X

2�dr

Ł

360hv

� �6:

where dr is the distance from the centre of the column to the

perimeter of the critical section and Ł is the angle (in degrees)

measured at the centre of the column between the two points

along the perimeter of the void overlapping the critical section as

shown in Figure 9(b).

Table 3 summarises the punching shear strength predicted using

Equation 6. With an assumed circular critical section located at d/

2 from the face of the equivalent circular column, Equation 6

predicted the punching shear strength of solid specimen S with

0

400

800

1200

1600

2000

0 2 4 6 8 10

Forc

e: k

N

Drift: mm

Specimen S

V1V3V2

V4

Figure 8. Force–displacement curves

Specimen ª: % V test:

kN

V test=V test-S:

%

˜test:

mm

˜test=˜test-S:

%

S 100 1848 100 7.2 100

V1 69 1297 70 6.3 88

V2 51 1071 58 5.2 72

V3 100 1111 60 5.8 81

V4 51 944 51 3.9 54

Table 2. Punching shear strength V test and drift capacity ˜test at

failure

Void

Overlapping section

Overlapping section

Overlapping section

θ

dv

h v

d v

Cross-section

dr d/2

d/2

d/2

Critical section

Critical section

(a)

(b) (c)

l r

Figure 9. Assumed critical sections in voided transfer slabs:

(a) rectangular critical section; (b) circular critical section;

(c) considering void sections as slab openings

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good accuracy (2% overestimation). For the voided specimens,

Equation 6 underestimated the punching shear strengths of V1, V2

and V4 by 12%, 16% and 5% respectively, and overestimated the

punching shear strength of specimen V3 by 70%. Methods con-

sidering only voids overlapping the critical section may thus not

guarantee an accurate prediction of the punching shear strength of

voided transfer slabs. This observation is somewhat different from

that for normal flat slabs (Schnellenbach-Held and Pfeffer, 2002).

Prediction of punching shear strength considering void

sections as slab openings

To estimate the punching shear strength of voided transfer slabs,

this study also considered voids in transfer slabs as slab openings.

According to ACI 318-11 (ACI, 2011), when openings are

located at a distance less than ten times the slab thickness from a

column, the effect of openings should be considered in the

calculation of punching shear strength.

ACI 318-11 specifies that for slabs without shear studs, the part

of the perimeter of the critical section that is enclosed by straight

lines projecting from the centroid of the column and tangential to

the boundaries of the openings should be considered ineffective

(Figure 9(c)). Here, since the voids did not pass throughout the

slab thickness (Figure 9(a)), the concrete area above and below

the void was not excluded from the critical section. Considering

voids as slab openings, the punching shear strength was calcu-

lated using

V c ¼ 0.33( f 9c)1=2 b0d �X

lrhv

� �7:

in which lr is the length to be deducted from the critical section

located at a distance d/2 from the column face (Figure 9(c)).

Table 3 shows that Equation 7 underestimated the punching shear

strengths of voided transfer slab specimens V1, V2, V3 and V4

by 14%, 33%, 34% and 24%, respectively.

Prediction of punching shear strength with a modified

critical section

The punching shear strength of voided transfer slabs was

calculated using three different methods. As shown in Table 3,

none of the methods predicted the punching shear strength

accurately for all specimens. They were particularly erroneous for

predicting the punching shear strength of specimen V3, which

had voids outside the ACI critical section at d/2 from the column

face (Figure 4(e)). As shown in Figure 7(d), cracks in specimen

V3 formed at a distance greater than in the other voided transfer

slab specimens. This indicates that the location of the critical

section could vary according to the location of voids.

An accurate method for calculating the punching shear strength

of voided transfer slabs was developed based on the experimental

results. An iterative procedure was adopted for determining the

critical section that produced the smallest punching shear

strength. In this method, the punching shear strength of the slab

is first calculated at the ACI critical section at d/2 from the

column face. The area of voids overlapping the critical section is

then removed from the critical section and the punching shear

strength calculated using the reduced critical section. The critical

section is then relocated to a distance greater than d/2 from the

column face and the punching shear strength is recalculated with

the changed critical section using Equation 4. This process is

repeated until detection of the critical section producing the

smallest of the calculated punching shear strengths. Figure 10

shows the punching shear strength (V c) calculated at different

locations of critical sections normalised by the actual strength

(V test).

As shown Figure 10(a), the punching shear strength of specimen

V3 increases with an increase in de until void sections were

encountered, de being the distance from the column face to the

assumed critical section. (Recall that the voids in specimen V3

were located outside the initial ACI critical section (at d/2 from

the column face), with no overlap of the critical section.) Then,

Specimen V test:

kN

Rectangular critical

section

(Equation 4)

Circular critical

section

(Equation 6)

Slab openings

(Equation 7)

Accurate method Simplified method

V c: kN V c=V test Vc: kN V c=V test

V c: kN V c=V test

V c: kN V c=V test V c: kN V c=V test

S 1848 1883 1.01 1557 0.84 1883 1.02 1883 1.02 1883 1.02

V1 1297 1012 0.78 1144 0.88 1113 0.86 1304 1.01 1310 1.01

V2 1071 470 0.44 895 0.84 721 0.67 930 0.87 947 0.89

V3 1111 1883 1.70 1883 1.70 732 0.66 1249 1.13 1262 1.14

V4 944 470 0.50 895 0.95 721 0.76 929 0.99 947 1.00

Table 3. Summary of actual and predicted punching shear

strengths

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the punching shear strength decreased with an increase in de

(from location ‘2’ to the minimum shear strength (MSS)) prior to

reaching the MSS indicated by a cross in Figure 10(a)). Beyond

the MSS, the strength increased again with a further increase in

de. The punching shear strength, which was the smallest of the

values in Figure 10(a), matched the actual strength of specimen

V3 (13% overestimation) obtained from the experiment, whereas

Equations 4 and 6 overestimated the punching shear strength of

V3 by 70%. Unexpectedly, it was observed that the punching

shear strength measured with the critical section at the centre of

the voids (location ‘3’ in Figure 10(a)) was almost the same as

that obtained with the critical section using the iterative proce-

dure.

Specimens V1 and V2 had voids overlapping the ACI critical

section at d/2 from the column face. The critical section

producing the smallest punching shear strength was located

between the initial ACI critical section and the centre of the voids

(locations 1–2 in Figure 10(b)). The punching shear strengths

calculated with the ACI critical sections at d/2 and at the centre

of the voids were very close to the MSS (marked with crosses in

Figure 10(b)). The proposed method using the iterative procedure

predicted the punching shear strengths of specimens V1 and V2

with good accuracy – an overestimation of 1% for V1 and 13%

underestimation for V2. When the critical section was assumed to

be at the centre of the voids instead of the location determined

from the iterative procedure, the punching shear strengths of V1

and V2 were almost same as those obtained from the method

using the iterative procedure. As shown in Figure 10(b), the

punching shear strengths of specimens V1 and V2 could be also

calculated using the ACI critical section at d/2 from the column

face with relatively good accuracy.

Unlike the other voided specimens, V4 had two rows of voids

(Figure 4(f)). As shown in Figure 10(b), the punching shear

strength calculated from the method using the iterative procedure

matched the actual strength, with negligible error. The critical

section producing the smallest punching shear strength was

located between the centres of the first row of voids (1–2 in

Figure 10(b)). Similarly to the punching shear strengths of

specimens V1 and V2, the punching shear strength of V4 could

also be calculated with good accuracy using critical sections

located at the centre of the voids in the first row and at d/2 from

the column face of two rows of voids.

Summary of proposed methods forcalculating punching shear strength of voidedtransfer slabsThe punching shear strength of voided transfer slabs can be

calculated using the proposed accurate method using the iterative

procedure or the simplified method avoiding the iterative proce-

dure.

In the accurate method, the critical section that produces the

smallest punching shear strength is determined from an iterative

procedure. In the simplified method, critical sections are assumed

to be located at either d/2 from the column face or at the centre

of the voids. If there is more than one row of voids, the centre of

the voids in each row should be considered as the possible

location of the critical section. Then, punching shear strengths

are calculated for all possible critical sections (d/2 and the centre

of each row of voids). Among the calculated values, the smallest

gives the punching shear strength to be determined. Figure 11

illustrates the assumed critical sections for the simplified method.

ConclusionsAccurate and simplified methods for calculating the punching

shear strength of voided transfer slabs have been proposed. To

evaluate the punching shear strength of voided transfer slabs,

1

1

1

1

2

2

2

2

3

3

3

3 4

4

0·8

1·3

120 170 220 270 320de (distance from column to critical perimeter): mm

Minimum shear strength (MSS)

V1

V4

V2

d/2

d/2

(b)

1·0

1·0

1·5

2·0

150 225 300 375

VV

cte

st/

VV

cte

st/

de (distance from column to critical perimeter): mm

Minimum shear strength (MSS)

d/2

d de ( /2)�

d de ( /2)�

V3

(a)

Figure 10. Punching shear strength using the accurate method

with iterative procedure: (a) specimen V3; (b) specimens V1, V2

and V4

11

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experimental tests were conducted using five specimens. The

following conclusions can be drawn from this study.

j The punching shear strengths of voided transfer slabs were

lower than that of the solid slab. The punching shear

strengths of voided transfer slabs varied according to the

arrangement and location of voids.

j Punching shear strength was poorly predicted by the method

only considering the ACI critical section located at d/2 from

the column face, particularly for transfer slab specimen V3

with voids located outside and not overlapping the ACI

critical section at d/2 from the column face. The error in the

calculated punching shear strength obtained from this method

was as high as 70%.

j An accurate method was developed that determined the

critical section producing the smallest shear strength using an

iterative procedure. This method accurately predicted the

punching shear strength of all the specimens. The largest

error, for specimen V3, was only 13%.

j A simplified method that does not require an iterative

procedure to determine the critical section was also proposed.

In this method, critical sections were assumed to be located at

either d/2 or the centre of each row of voids. The punching

shear strengths were calculated with assumed critical sections

and the smallest value was taken to be the punching shear

strength to be determined. The errors associated with this

method were almost the same as that of the accurate method

using the iterative procedure.

AcknowledgementThe authors would like to acknowledge financial support provided

by the National Research Foundation of Korea (2012R1A2A2A

06045129).

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A A�

3

3

2

2

1

1

d/2

h v

First critical section at /2d

Second critical section at centre of voids in the first row

Third critical section at centre of voids in the second row

1

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3

d

dv

Section view A–A�

Figure 11. Possible critical sections considered by the simple

method

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Magazine of Concrete Research Evaluation of punching shear strength ofvoided transfer slabsHan and Lee

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Magazine of Concrete Research Evaluation of punching shear strength ofvoided transfer slabsHan and Lee