# Experimental Study on Sandwich Bridge Decks with GFRP Face Sheets and a Foam-Web Core Loaded under Two-Way Bending

Authors: Ruili Huo; Weiqing Liu; Li Wan; Yuan Fang; Lu Wang
Journal: Advances in Materials Science and Engineering
 (2015)

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## Abstract

In recent years, the sandwich bridge decks with GFRP face sheets and light weight material core have been widely used in the world due to their advantages of low cost, high strength to weight ratios, and corrosion resisting. However, as the bridge decks, most of them are used in foot bridges rather than highway bridges because the ultimate bending strength and initial bending stiffness are relatively low. To address this issue and expand the scope of use, a simple and innovative sandwich bridge deck with GFRP face sheets and a foam-web core, manufactured by vacuum assisted resin infusion process, is developed. An experimental study was carried out to validate the effectiveness of this panel for increasing the ultimate bending strength and initial bending stiffness under two-way bending. The effects of face sheet thickness, foam density, web thickness, and web spacing on displacement ductility and energy dissipation were also investigated. Test results showed that, compared to the normal foam-core sandwich decks, an average approximately 657.1% increase in the ultimate bending strength can be achieved. Furthermore, the bending stiffness, displacement ductility, and energy dissipation can be enhanced by increasing web thickness, web height, and face sheet thickness or decreasing web spacing.


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## Body

## 1. Introduction

In recent years, composite sandwich decks have been used increasingly in the bridge engineering due to their advantages of low cost, high strength to weight ratios, and corrosion resisting. In sandwich decks, low density materials, such as polyurethane foam, paulownia wood, and honeycombs, have been usually employed to be the cores, which are combined with high stiffness face sheets to resist applied loads. The composite face sheets provide major contribution to the bending stiffness while the core provides the major shear stiffness of sandwich decks.A great number of experimental and analytical studies of sandwich bridge decks with composite face sheets and a foam core under bending have been conducted in the past twenty years. Sharaf et al. [1] tested sandwich wall panels with GFRP face sheets and a foam core under four-point bending. The test results indicated that a higher foam density can generate a larger ultimate bending strength and stiffness. Meanwhile, the horizontal slip was affected by foam core toughness. However, the horizontal slip between face sheet and foam core can accelerate the occurrence of interfacial delamination. Romanoff and Varsta [2, 3] proposed an analytical model based on the plane frame analysis to predict the bending strength of a web-core sandwich beams and panels. The Clebsch’s method was adopted to calculate the deformation of face sheets. Compared to the existing homogenized beam analysis method, the proposed model can achieved more accuracy results. Russo and Zuccarello [4] carried out three-point bending, four-point bending, shear, and flatwise compressive and tensile tests of sandwich decks with PVC foam and polyester mat cores. The test results showed that the ultimate bending strength of decks depended on the failure mode. A numerical model was also established to study the influences of transverse stress on failure modes. In other words, the local buckling failure and delamination failure restrict the practical application of the proposed sandwich decks. Steeves and Fleck [5, 6] conducted the experimental and analytical investigations on the collapse mechanisms for simply supported sandwich beams with GFRP face sheets and a PVC foam core loaded in three-point bending. The test results demonstrated that failure mode was determined by the beam geometry and the density of the foam core. But the ultimate bending strength and initial stiffness of sandwich panels are small because there are no lattice web or fiber insertions to improve the stiffness of core. Tagarielli et al. [7] investigated the collapse modes of sandwich beams with clamped and simple supports under three-point bending. The results demonstrated that the simply supported beams exhibit a softening postyield response, while the clamped beams perform a hardening behavior due to membrane stretching of the face sheets. Reis [8] and Reis and Rizkalla [9] developed a new type of panels that consisted of GFRP face sheets, foam cores, and through-thickness GFRP insertions. The delamination between GFRP face sheets and core did not occur due to the use of the fiber insertions. Meanwhile, the flatwise compressive strength of proposed panels can be improved sharply. The strength was mainly affected by fiber insertion density, face sheets thickness, and panel height. However, this kind of sandwich decks is used as the foot bridge deck since the ultimate bending strength and initial bending stiffness of sandwich decks are relatively small, which did not satisfy the design requirements of highway bridges. Zi et al. [10] carried out a bending test to study the performance of a polyurethane foam-filled GFRP bridge deck. The GFRP bridge decks with rectangular holes were manufactured by pultrusion process. The results showed that the bending strength and stiffness were improved significantly compared to the control decks, in which the holes were not filled with foams. In order to avoid the web-flange joint failure, Zi et al. [11] developed the construction of the web-flange joints during the pultrusion process, in which the fibers of the lattice web were extended to half width of the flanges. Thus, the failure mode was determined by the adhesive strength of interface. Nevertheless, the size of this kind of bridge deck can be restricted due to the use of the pultrusion process. In the meantime, the pultrusion process is not allowed to arrange the GFRP webs in the two directions.Furthermore, besides the shortcomings summarized in the above literature review, almost all of existing studies focused on investigating the behavior of sandwich panels loaded under one-way bending rather than two-way bending; hence the effects of concentrated loading on the mechanical performance were ignored.Dawood et al. [12] studied the performance of 3D GFRP sandwich decks with fiber insertions loaded in two-way bending. The results demonstrated that the performance of the decks was governed by the deck height and the shear stiffness of the core. The main failure mode of the decks was local buckling of the deck at the support positions. The influences of face sheet thickness, fiber insertion density, deck height, and aspect ratio on the bending performance of the decks were also investigated. However, the bottom face sheet of deck cannot bring into full play the tensile resistant to the applied loads because of the presence of local buckling effects.In order to address the mentioned issues, a kind of sandwich bridge deck with GFRP face sheets and foam-web core (GFFW deck), manufactured through vacuum assisted resin infusion process, was developed, as shown in Figure1. The detailed manufacture procedure, axial compression tests, and one-way bending tests were introduced in our companion papers [13–15]. The test results indicated that, compared to normal sandwich decks, the ultimate bending strength and initial bending stiffness of GFFW decks loaded in four-point bending were enhanced significantly due to the presence of GFRP web. Moreover, this kind of sandwich bridge decks has been applied in some projects, as shown in Figure 2. Figure 2(a) shows a truss bridge with GFFW bridge decks in Shanghai harbor, which allowed the fork lift trucks on the bridge; and Figure 2(b) shows that the GFFW bridge decks were paved on the muddy road as the backing board. In order to thoroughly understand the mechanical behavior of GFFW decks, there is a need to investigate the bending behavior of GFFW decks through experimental evaluation, which is the motivation of this investigation. In this paper, to simulate the two-way bending effects on a deck by a single vehicle tie, the two-way bending test was conducted to study the ultimate bending strength, initial bending stiffness, displacement ductility, and failure modes of the GFFW decks.Figure 1
The sandwich bridge deck with GFRP face sheets and a foam-web core.Figure 2
Practical applications of GFFW decks: (a) a truss bridge with GFFW decks and (b) GFFW bridge decks used as the backing board.
(a)
(b)


## 2. Experimental Program

### 2.1. Description of Test Specimens and Parameters

In this study, all decks were manufactured by means of vacuum assisted resin infusion process in the Advanced Composite Structures Research Center at Nanjing Tech University. Table1 shows a summary of the test matrix and designed dimension of decks. Fourteen specimens, involving two control decks (CON60 and CON100) and twelve GFFW decks, were subjected to concentrated load. All decks have identical length (l) and width (w), which were equal to 1000 mm. The other specimens were strengthened by GFRP webs with varying face sheet thickness (ts), foam density (ρ), web thickness (tw), and web spacing (s):(1)
Foam density with either 40 kg/m3, 60 kg/m3, or 100 kg/m3, designated as P4, P6, and P1, respectively.(2)
Decks with either 75 mm or 125 mm web spacing, designated as S7 and S1, respectively.(3)
Webs with either 1.6 mm or 3.2 mm thickness, designated as W1 and W3, respectively.(4)
Face sheets with either 1.6 mm or 3.2 mm thickness, designated as T1 and T3, respectively.Table 1
Details of specimens.
Specimen
l
d
ρ
s
t
w
t
s
(mm)
(mm)
(kg/m3)
(mm)
(mm)
(mm)
CON60
1000
1000
60
—
—
3.2
CON100
1000
1000
60
—
—
3.2
P4S7W1T3
1000
1000
40
75
1.6
3.2
P6S7W1T3
1000
1000
60
75
1.6
3.2
P1S7W1T3
1000
1000
100
75
1.6
3.2
P6S7W1T1
1000
1000
60
75
1.6
1.6
P6S7W1T4
1000
1000
60
75
1.6
4.8
P6S7W3T3
1000
1000
60
75
3.2
3.2
P4S1W1T3
1000
1000
40
125
1.6
3.2
P6S1W1T3
1000
1000
60
125
1.6
3.2
P1S1W1T3
1000
1000
100
125
1.6
3.2
P1S1W1T1
1000
1000
100
125
1.6
1.6
P1S1W1T4
1000
1000
100
125
1.6
4.8
P6S1W4T3
1000
1000
60
125
4.8
3.2


### 2.2. Material Properties

The composite face sheets were fabricated using E-glass mat and HS-2101-G100 unsaturated polyester resin. The tensile and compressive tests were conducted by the authors in accordance with ASTM D3039/D 3039 M-08 [16] and ASTM D695-10 [17], respectively. The average tensile strength and tensile modulus were 52.7 MPa and 4.9 GPa, respectively. The average compressive strength and compressive modulus were 313.7 MPa and 21.7 GPa, respectively. Table 2 lists the material properties of the GFRP face sheets.Table 2
Material properties of GFRP face sheet.
Face sheets
Compressive strength    (MPa)
52.7
Compressive modulus  (GPa)
4.9
Tensile strength   (MPa)
313.7
Tensile modulus  (GPa)
21.1The PU foams with three different densities (40 kg/m3, 60 kg/m3, and 100 kg/m3) were employed in this study. For each of PU foams, total twelve cubic foam core coupons of 50 mm thick were tested by the authors in compression based on ASTM C365-03 [18] and in shear based on ASTM C273/273M-07 [19], using six cubic foam core coupons for each case. Table 3 summarized the measured material properties of foams.Table 3
Material properties of foam.
Foam
40 kg/m3
60 kg/m3
100 kg/m3
Compressive strength    (MPa)
0.4
0.7
1.3
Compressive modulus  (MPa)
5.5
9.2
14.5
Shear strength   (MPa)
0.4
0.6
0.9
Shear modulus  (GPa)
51.2
66.2
81.9


### 2.3. Test Setup and Instrumentation

The tests were conducted in the Structural Engineering Laboratory at Nanjing Tech University. The decks were supported around all four edges by a stiff steel support which was welded by four steel channels, as shown in Figure3. A concentrated load was applied using a 500 kN hydraulic actuator acting on a 100 mm × 100 mm square area at the center of the decks. A 3 mm thick steel shim and a 2 mm thick neoprene pad with 100 mm length and 100 mm width were placed between actuator and loading area. The load was applied in displacement control at a rate of 2 mm/min.Figure 3
Test setup.To measure the bending deflections of the tested deck, five linear variable displacement transducers (LVDTs) with a stroke of 100 mm were installed. The arrangement of LVDTs was shown in Figure4(a). In the meantime, for each deck, five electric resistance strain gauges were pasted on the bottom face sheet to analysis the strain distribution, as shown in Figure 4(b). Moreover, the readings of strain gauges were also used to identify the failure mode of decks.Figure 4
Instrumentation of Specimen P6S7W1T3: (a) LVDT and (b) strain gauge arrangements.
(a)
(b)


## 2.1. Description of Test Specimens and Parameters

In this study, all decks were manufactured by means of vacuum assisted resin infusion process in the Advanced Composite Structures Research Center at Nanjing Tech University. Table1 shows a summary of the test matrix and designed dimension of decks. Fourteen specimens, involving two control decks (CON60 and CON100) and twelve GFFW decks, were subjected to concentrated load. All decks have identical length (l) and width (w), which were equal to 1000 mm. The other specimens were strengthened by GFRP webs with varying face sheet thickness (ts), foam density (ρ), web thickness (tw), and web spacing (s):(1)
Foam density with either 40 kg/m3, 60 kg/m3, or 100 kg/m3, designated as P4, P6, and P1, respectively.(2)
Decks with either 75 mm or 125 mm web spacing, designated as S7 and S1, respectively.(3)
Webs with either 1.6 mm or 3.2 mm thickness, designated as W1 and W3, respectively.(4)
Face sheets with either 1.6 mm or 3.2 mm thickness, designated as T1 and T3, respectively.Table 1
Details of specimens.
Specimen
l
d
ρ
s
t
w
t
s
(mm)
(mm)
(kg/m3)
(mm)
(mm)
(mm)
CON60
1000
1000
60
—
—
3.2
CON100
1000
1000
60
—
—
3.2
P4S7W1T3
1000
1000
40
75
1.6
3.2
P6S7W1T3
1000
1000
60
75
1.6
3.2
P1S7W1T3
1000
1000
100
75
1.6
3.2
P6S7W1T1
1000
1000
60
75
1.6
1.6
P6S7W1T4
1000
1000
60
75
1.6
4.8
P6S7W3T3
1000
1000
60
75
3.2
3.2
P4S1W1T3
1000
1000
40
125
1.6
3.2
P6S1W1T3
1000
1000
60
125
1.6
3.2
P1S1W1T3
1000
1000
100
125
1.6
3.2
P1S1W1T1
1000
1000
100
125
1.6
1.6
P1S1W1T4
1000
1000
100
125
1.6
4.8
P6S1W4T3
1000
1000
60
125
4.8
3.2


## 2.2. Material Properties

The composite face sheets were fabricated using E-glass mat and HS-2101-G100 unsaturated polyester resin. The tensile and compressive tests were conducted by the authors in accordance with ASTM D3039/D 3039 M-08 [16] and ASTM D695-10 [17], respectively. The average tensile strength and tensile modulus were 52.7 MPa and 4.9 GPa, respectively. The average compressive strength and compressive modulus were 313.7 MPa and 21.7 GPa, respectively. Table 2 lists the material properties of the GFRP face sheets.Table 2
Material properties of GFRP face sheet.
Face sheets
Compressive strength    (MPa)
52.7
Compressive modulus  (GPa)
4.9
Tensile strength   (MPa)
313.7
Tensile modulus  (GPa)
21.1The PU foams with three different densities (40 kg/m3, 60 kg/m3, and 100 kg/m3) were employed in this study. For each of PU foams, total twelve cubic foam core coupons of 50 mm thick were tested by the authors in compression based on ASTM C365-03 [18] and in shear based on ASTM C273/273M-07 [19], using six cubic foam core coupons for each case. Table 3 summarized the measured material properties of foams.Table 3
Material properties of foam.
Foam
40 kg/m3
60 kg/m3
100 kg/m3
Compressive strength    (MPa)
0.4
0.7
1.3
Compressive modulus  (MPa)
5.5
9.2
14.5
Shear strength   (MPa)
0.4
0.6
0.9
Shear modulus  (GPa)
51.2
66.2
81.9


## 2.3. Test Setup and Instrumentation

The tests were conducted in the Structural Engineering Laboratory at Nanjing Tech University. The decks were supported around all four edges by a stiff steel support which was welded by four steel channels, as shown in Figure3. A concentrated load was applied using a 500 kN hydraulic actuator acting on a 100 mm × 100 mm square area at the center of the decks. A 3 mm thick steel shim and a 2 mm thick neoprene pad with 100 mm length and 100 mm width were placed between actuator and loading area. The load was applied in displacement control at a rate of 2 mm/min.Figure 3
Test setup.To measure the bending deflections of the tested deck, five linear variable displacement transducers (LVDTs) with a stroke of 100 mm were installed. The arrangement of LVDTs was shown in Figure4(a). In the meantime, for each deck, five electric resistance strain gauges were pasted on the bottom face sheet to analysis the strain distribution, as shown in Figure 4(b). Moreover, the readings of strain gauges were also used to identify the failure mode of decks.Figure 4
Instrumentation of Specimen P6S7W1T3: (a) LVDT and (b) strain gauge arrangements.
(a)
(b)


## 3. Experimental Results and Discussion

The test results, involving the observed failure modes, yield bending strength (Py), ultimate bending strength (Pu), yield midspan deflection (Δy), ultimate midspan deflection (Δu), initial bending stiffness (Ke), displacement ductility factor (η), and energy dissipation factor (μ), are presented in Table 4.Table 4
Two-way bending test results.
Specimen
P
y
P
u
Δ
y
Δ
u
K
e
η
E
y
E
u
μ
Failure mode
(kN)
(kN)
(mm)
(mm)
(kN/mm)
(kN∗mm)
(kN∗mm)
CON60
18.2
18.2
16.49
16.49
1.10
1.00
150.1
150.1
1.00
D
CON100
32.1
32.1
20.43
20.43
1.57
1.00
327.9
327.9
1.00
D
P4S7W1T3
34.6
53.2
14.2
40.9
2.44
2.88
245.7
1417.8
5.77
C
P6S7W1T3
79.6
82.1
17.5
32.5
4.55
1.86
696.5
1909.3
2.74
C
P1S7W1T3
88.5
108.4
12.3
21.4
7.20
1.74
544.3
1440.2
2.65
C
P6S7W1T1
31.8
38.9
14.5
32.1
2.19
2.21
230.6
852.7
3.70
C
P6S7W1T4
111.2
144.2
18.9
28.2
5.88
1.49
1050.8
2238.5
2.13
C
P6S7W3T3
130.1
137.8
10.2
15.7
12.75
1.54
663.5
1400.2
2.11
C
P4S1W1T3
37.2
48.5
16.7
33.2
2.23
1.99
310.6
1017.7
3.28
C
P6S1W1T3
58.2
63.6
15.9
28.1
3.66
1.77
462.7
1205.7
2.61
C
P1S1W1T3
71.4
86.7
13.9
23.1
5.14
1.66
496.2
1223.5
2.47
C
P1S1W1T1
32.3
40.9
17.5
31.9
1.85
1.82
282.6
809.7
2.86
C
P1S1W1T4
102.3
130.9
9.78
14.3
10.46
1.46
500.3
1027.3
2.05
C
P6S1W4T3
105.7
126.9
11.2
16.5
9.44
1.47
591.9
1208.3
2.04
C
Note: “D” is delamination failure and “C” is top face sheet compressive failure.


### 3.1. Failure Mode

According to the readings of the strain gauges attached to the face sheets, the failure modes of all specimens can be categorised as two types:(1) delamination failure, which occurred in control decks, as shown in Figure 5(a); (2) top face sheet compressive failure, which occurred in GFFW decks, as shown in Figure 5(b). For the first failure mode, when the shear stress in the interface between face sheet and foam core was larger than adhesive shear stress, the delamination phenomenon can be observed. While for the GFFW decks, the delamination failure did not occur because the webs can improve adhesive strength between face sheets and foam cores. For the second failure mode, because the GFRP webs can provide the displacement and rotation restricts for the face sheets, based on the classic elastic stability theory, the calculated critical buckling stress of face sheet is larger than yield stress. Hence, the local buckling failure did not occur. For all GFFW decks, the foam core shear failure and indentation failure did not occur, because the webs can provide resistance to the shear force and meanwhile improve the bending stiffness of GFFW decks.Figure 5
Failure modes (a) delamination of Specimen CON60 and (b) face sheet rupture of Specimen P6S7W1T1.
(a)
(b)


### 3.2. Ultimate Bending Strength

Compared with the control decks, the GFFW decks show various degrees of strengthening, which are summarized in Table4. Compared to Specimens CON60 (ρ = 60 kg/m3), the ultimate bending strength of Specimens P6S7W1T3 and P6S7W3T3 increased by 351.1% and 657.1%, respectively. Compared to Specimen CON100 (ρ = 100 kg/m3), the ultimate bending strength of Specimens P1S7W1T3 and P1S1W1T3 increased by 237.7% and 170.1%, respectively. Hence, it is evident that the improvement in ultimate bending strength of GFFW decks is significantly due to the presence of GFRP webs.Figures6(a) and 6(b) show the influence of face sheet thickness (ts) on the ultimate bending strength of GFFW decks. As shown in Figure 6(a), under the same foam density (ρ = 60 kg/m3), web spacing (s = 75 mm), and web thickness (tw = 1.6 mm), when the face sheet thickness was 1.6 mm, the ultimate bending strength of Specimen P6S7W1T1 was the smallest, which was equal to 38.9 kN. While the face sheet thickness increased to 4.8 mm, the ultimate bending strength of Specimen P6S7W1T4 was the largest, which increased by 270.7% compared to that of Specimen P6S7W1T1. As shown in Figure 6(b), under the same foam density (ρ = 100 kg/m3), web spacing (s = 125 mm), and web thickness (tw = 1.6 mm), when the face sheet thickness was 1.6 mm, the ultimate bending strength of Specimen P1S1W1T1 was the smallest, which was equal to 40.9 kN. While the face sheet thickness increased to 4.8 mm, the ultimate bending strength of Specimen P1S1W1T4 was the largest, which increased by 220.0% compared to that of Specimen P1S1W1T1.Figure 6
The influence of face sheet thickness: (a)tw = 1.6 mm, s = 75 mm, and ρ = 60 kg/m3 and (b) tw = 1.6 mm, s = 125 mm, and ρ = 100 kg/m3.
(a)
(b)Figures7(a) and 7(b) show the influence of foam density (ρ) on the ultimate bending strength of GFFW decks. Compared to specimens P4S7W1T3 (ts = 3.2 mm, s = 75 mm, and tw = 1.6 mm) and P4S1W1T3 (ts = 3.2 mm, s = 125 mm, and tw = 1.6 mm) with 40 kg/m3 foam density, the ultimate bending strength of specimens P6S7W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) and P6S1W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) with 60 kg/m3 foam density increased by 54.3% and 103.8%, respectively, and the ultimate bending strength of specimens P1S7W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) and P1S1W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) with 100 kg/m3 foam density increased by 31.1% and 78.8%, respectively.Figure 7
The influence of foam density: (a)ts = 3.2 mm, s = 75 mm, and tw = 1.6 mm and (b) ts = 3.2 mm, s = 125 mm, and tw = 1.6 mm.
(a)
(b)Figures8(a) and 8(b) show the influence of web thickness (tw) on the ultimate bending strength of GFFW decks. Compared to Specimen P6S7W1T3 (ts = 3.2 mm, s = 75 mm, and ρ = 60 kg/m3) with 1.6 mm thick web thickness, the ultimate bending strength of Specimen P6S7W3T3 with 3.2 mm web thickness increased by 67.8%. Compared to Specimen P6S1W1T3 (ts = 3.2 mm, s = 125 mm, and ρ = 60 kg/m3) with 1.6 mm thick web thickness, the ultimate bending strength of Specimen P6S1W4T3 with 4.8 mm web thickness increased by 99.5%.Figure 8
The influence of web thickness: (a)ts = 3.2 mm, s = 75 mm, and ρ = 60 kg/m3 and (b) ts = 3.2 mm, s = 125 mm, and ρ = 60 kg/m3.
(a)
(b)Figures9(a) and 9(b) show the influence of web spacing (s) on the ultimate bending strength of GFFW decks. Under the conditions of ts = 3.2 mm, tw = 1.6 mm, and ρ = 60 kg/m3, the ultimate bending strength of Specimen P6S7W1T3 (s = 75 mm) was 83.3 kN, which was 29.1% larger than that of Specimen P6S1W1T3 (s = 125 mm). Under the conditions of ts = 3.2 mm, tw = 1.6 mm, and ρ = 100 kg/m3, the ultimate bending strength of Specimen P1S7W1T3 (s = 75 mm) was 83.3 kN, which was 25.0% larger than that of Specimen P1S1W1T3 (s = 125 mm).Figure 9
The influence of web spacing: (a)ts = 3.2 mm, ρ = 60 kg/m3, and tw = 1.6 mm and (b) ts = 3.2 mm, ρ = 100 kg/m3, and tw = 1.6 mm.
(a)
(b)Hence, a larger face sheet thickness, foam density, and web thickness can lead to a higher ultimate bending strength of the GFFW decks, while a larger web spacing can lead to a lower ultimate bending strength of the GFFW decks.


### 3.3. Initial Bending Stiffness

The initial bending stiffness of a deck (Ke) is determined by(1)Ke=PyΔy,where Py and Δy are the yield strength of a deck and corresponding yield deflection, respectively (see Figure 10).Figure 10
The idealised load-midspan deflection curve.Figure11(a) shows the influences of GFRP face sheet thickness on the initial bending stiffness of GFFW decks. Compared to Specimen P6S7W1T1 (Ke = 2.19 kN/mm) with 1.6 mm face sheet thickness, Ke of Specimens P6S7W1T3 (ts = 3.2 mm) and P6S7W1T4 (ts = 4.8 mm) increased by 107.7% and 168.7%, respectively. Compared to Specimen P1S1W1T1 (Ke = 1.85 kN/mm) with 1.6 mm face sheet thickness, Ke of Specimens P1S1W1T3 (ts = 3.2 mm) and P1S1W1T4 (ts = 4.8 mm) increased by 97.9% and 465.4%, respectively. Thus, using thicker GFRP face sheet can improve the initial bending stiffness of decks significantly.Figure 11
Initial bending stiffness: (a) the influence of face sheet thickness, (b) the influence of foam density, (c) the influence of web thickness, and (d) the influence of web thickness.
(a)
(b)
(c)
(d)Figure11(b) shows the influences of foam density on the initial bending stiffness of GFFW decks. Compared to Specimen P4S7W1T3 (Ke = 2.44 kN/mm) with 40 kg/m3 foam density, Ke of Specimens P6S7W1T3 (ρ = 60 kg/m3) and P1S7W1T3 (ρ = 100 kg/m3) were 4.55 kN/mm and 7.20 kN/mm, respectively, which were 86.4% and 194.9% greater than that of Specimen P4S7W1T3. Compared to Specimen P4S1W1T3 (Ke = 2.23 kN/mm) with 40 kg/m3 foam density, Ke of Specimens P6S1W1T3 (ρ = 60 kg/m3) and P1S1W1T3 (ρ = 100 kg/m3) were 3.66 kN/mm and 5.14 kN/mm, respectively, which were 64.1% and 130.3% greater than that of Specimen P4S7W1T3. The foam with larger density also behaves stiffer. Therefore, a larger foam density can generate a larger bending stiffness.Figure11(c) shows the influences of web thickness on the initial bending stiffness of GFFW decks. Compared to specimens P6S7W1T3 (ts = 3.2 mm, s = 75 mm, and ρ = 60 kg/m3) and P6S1W1T3 (ts = 3.2 mm, s = 125 mm, and ρ = 60 kg/m3) with 1.6 mm web thickness, Ke of specimens P6S7W3T3 with 3.2 mm web thickness and P6S1W4T3 with 4.8 mm web thickness increased by 180.4% and 157.8%, respectively, which were equal to 12.75 kN/mm and 9.44 kN/mm. Because increasing the web thickness can result in a larger ratio of the volume of web to foam, which can increase the equivalent Young’s modulus according to (3), a larger ultimate bending strength of GFFW deck can be achieved.Figure11(d) shows the influences of web spacing on the initial bending stiffness of GFFW decks. For Specimens P6S7W1T3 and P1S7W1T3 with 75 mm web spacing, 1.6 mm web thickness, 3.2 mm face sheet thickness, and 60 kg/m3 foam density, Ke of them were 4.55 kN/mm and 7.20 kN/mm, respectively, which were 24.3% and 40.1% greater than those of Specimens P6S1W1T3 and P1S1W1T3 with 125 mm web spacing, 1.6 mm web thickness, 3.2 mm face sheet thickness, and 60 kg/m3 foam density. Decreasing web spacing can increase the ratio of the volume of web to foam, which was the same as the thicker webs. Hence, the equivalent Young’s modulus can be improved. Furthermore, the larger ratio of the volume of web to foam can enhance the shear capacity and face sheet/core adhesive strength of panels. Therefore, smaller web spacing leads to a higher ultimate bending strength.


### 3.4. Improvements in Displacement Ductility

The displacement ductility factor (η) is adopted to evaluate the ductility performance of the specimens, which is given by(2)η=ΔuΔy,where Δu is the ultimate deflection corresponding to the ultimate bending strength (see Figure 12).Figure 12
Displacement ductility factor: (a) the influence of face sheet thickness, (b) the influence of foam density, (c) the influence of web thickness, and (d) the influence of web thickness.
(a)
(b)
(c)
(d)As summarized in Table4, the displacement ductility factors range from 1.0 (for control specimens) to 2.88 (for Specimen P4S7W1T3). As shown in Figure 12(a), compared to Specimens P6S7W1T1 (η = 2.21) and P1S1W1T1 (η = 1.82) with 1.6 mm face sheet thickness, η of Specimens P6S7W1T3 (η = 1.86) and P1S1W1T3 (η = 1.66) with 3.2 mm face sheet thickness decreased by 18.8% and 9.6%, respectively; η of Specimens P6S7W1T4 (η = 1.49) and P1S1W1T4 (η = 1.46) with 4.8 mm face sheet thickness decreased by 48.3% and 24.7%, respectively. Hence, using thinner GFRP face sheet can effectively improve the displacement ductility of GFFW decks.In terms of the influence of foam density on the displacement ductility (see Figure12(b)), compared to Specimen P1S7W1T3 (η = 1.46) with 100 kg/m3 foam density, η of Specimens P4S7W1T3 with 40 kg/m3 foam density and P6S7W1T3 with 60 kg/m3 foam density increased by 65.5% and 6.7%, respectively, which were equal to 2.88 and 1.86. Compared to Specimen P1S1W1T3 (η = 1.66) with 100 kg/m3 foam density, η of Specimens P4S1W1T3 with 40 kg/m3 foam density and P6S1W1T3 with 60 kg/m3 foam density increased by 19.8% and 6.5%, respectively, which were equal to 1.99 and 1.77. Therefore, the displacement ductility factor can become smaller with the increase in the foam density.As shown in Figure12(c), using thicker web tw = 3.2 mm for strengthening Specimen P6S7W3T3 and tw = 4.8 mm for strengthening Specimen P6S1W4T3 instead of thinner web (tw = 1.6 mm) for Specimens P6S7W1T3 and P6S7W1T3, η of P6S7W3T3 and P6S1W4T3 were almost 85% when compared with their counterpart. Hence, the thinner web can result in better ductility of decks. For the influence of web spacing on the displacement ductility (see Figure 12(d)), compared to Specimens P6S7W1T3 and P1S7W1T3 (s = 75 mm), η of Specimens P6S1W1T3 and P1S1W1T3 with 125 mm web spacing decreased by 4.8% and 4.5%, respectively. Thus, the displacement ductility of GFFW decks can be affected by web spacing slightly.


### 3.5. Energy Dissipation

The energy ductility coefficient (μ) was much more reasonable to evaluate the postyield deformation of the decks [14], which can be expressed as(3)μ=EuEy,where the yield energy Ey is the triangular area under the load-midspan deflection curve and the ultimate energy Eu is the total area under the load-midspan deflection curve (see Figure 10).As summarized in Table4, the energy ductility coefficients of control specimens are the smallest, which were nearly equal to 1.0. Figure 13(a) shows the influence of face sheet thickness on the energy ductility coefficient of decks. Comparison of the values of μ of Specimens P6S7W1T1, P6S7W1T3, and P6S7W1T4 indicates that increasing the skin thickness from 1.6 mm to 4.8 mm decreased the energy ductility coefficient of the deck by 25.9% and 42.4% relative to μ of Specimen P6S7W1T1. Similarly, comparison of the values of μ of Specimens P1S1W1T1, P1S1W1T3, and P1S1W1T4 shows that increasing the skin thickness from 1.6 mm to 4.8 mm decreased the energy ductility coefficient of the deck by 13.8% and 28.2% relative to μ of Specimen P1S1W1T1. Figure 13(b) shows the influence of foam density on the energy ductility coefficient of decks. Compared to Specimen P1S7W1T3 (μ = 2.65) with 100 kg/m3 foam density, μ of Specimens P4S7W1T3 with 40 kg/m3 foam density and P6S7W1T3 with 60 kg/m3 foam density were equal to 5.77 and 2.74, which increased by 117.8% and 3.4%, respectively. Compared to Specimen P1S1W1T3 (μ = 2.47) with 100 kg/m3 foam density, μ of Specimens P4S1W1T3 with 40 kg/m3 foam density and P6S1W1T3 with 60 kg/m3 foam density were equal to 3.28 and 2.61, which increased by 32.6% and 5.5%, respectively. Turning to the influence of web thickness on the energy ductility coefficients, as shown in Figure 13(c), compared to Specimens P6S7W1T3 (μ = 2.74) and P6S1W1T3 (μ = 2.61) with 1.6 mm web thickness, μ of Specimens P6S7W3T3 with 3.2 mm web thickness and P6S1W4T3 with 4.8 mm web thickness were equal to 2.11 and 2.04, which slightly decreased by 23.0% and 21.8%, respectively. As shown in Figure 13(d), Although the web spacing of Specimens P6S1W1T3 and P1S1W1T3 was nearly 1.7 times of that of Specimens P6S7W1T3 and P1S7W1T3 (s = 75 mm), the energy ductility coefficients were 4.9% and 6.8% smaller than that of Specimens P6S7W1T3 and P1S7W1T3, which were equal to 2.74 and 2.65, respectively. Therefore, the test results indicate that the energy ductility coefficients of GFFW decks were mainly affected by face sheet thickness, foam density, and the web thickness. The thinner face sheet, smaller foam density, and thinner web can provide better energy dissipation.Figure 13
Energy ductility coefficient: (a) the influence of face sheet thickness, (b) the influence of foam density, (c) the influence of web thickness, and (d) the influence of web thickness.
(a)
(b)
(c)
(d)


## 3.1. Failure Mode

According to the readings of the strain gauges attached to the face sheets, the failure modes of all specimens can be categorised as two types:(1) delamination failure, which occurred in control decks, as shown in Figure 5(a); (2) top face sheet compressive failure, which occurred in GFFW decks, as shown in Figure 5(b). For the first failure mode, when the shear stress in the interface between face sheet and foam core was larger than adhesive shear stress, the delamination phenomenon can be observed. While for the GFFW decks, the delamination failure did not occur because the webs can improve adhesive strength between face sheets and foam cores. For the second failure mode, because the GFRP webs can provide the displacement and rotation restricts for the face sheets, based on the classic elastic stability theory, the calculated critical buckling stress of face sheet is larger than yield stress. Hence, the local buckling failure did not occur. For all GFFW decks, the foam core shear failure and indentation failure did not occur, because the webs can provide resistance to the shear force and meanwhile improve the bending stiffness of GFFW decks.Figure 5
Failure modes (a) delamination of Specimen CON60 and (b) face sheet rupture of Specimen P6S7W1T1.
(a)
(b)


## 3.2. Ultimate Bending Strength

Compared with the control decks, the GFFW decks show various degrees of strengthening, which are summarized in Table4. Compared to Specimens CON60 (ρ = 60 kg/m3), the ultimate bending strength of Specimens P6S7W1T3 and P6S7W3T3 increased by 351.1% and 657.1%, respectively. Compared to Specimen CON100 (ρ = 100 kg/m3), the ultimate bending strength of Specimens P1S7W1T3 and P1S1W1T3 increased by 237.7% and 170.1%, respectively. Hence, it is evident that the improvement in ultimate bending strength of GFFW decks is significantly due to the presence of GFRP webs.Figures6(a) and 6(b) show the influence of face sheet thickness (ts) on the ultimate bending strength of GFFW decks. As shown in Figure 6(a), under the same foam density (ρ = 60 kg/m3), web spacing (s = 75 mm), and web thickness (tw = 1.6 mm), when the face sheet thickness was 1.6 mm, the ultimate bending strength of Specimen P6S7W1T1 was the smallest, which was equal to 38.9 kN. While the face sheet thickness increased to 4.8 mm, the ultimate bending strength of Specimen P6S7W1T4 was the largest, which increased by 270.7% compared to that of Specimen P6S7W1T1. As shown in Figure 6(b), under the same foam density (ρ = 100 kg/m3), web spacing (s = 125 mm), and web thickness (tw = 1.6 mm), when the face sheet thickness was 1.6 mm, the ultimate bending strength of Specimen P1S1W1T1 was the smallest, which was equal to 40.9 kN. While the face sheet thickness increased to 4.8 mm, the ultimate bending strength of Specimen P1S1W1T4 was the largest, which increased by 220.0% compared to that of Specimen P1S1W1T1.Figure 6
The influence of face sheet thickness: (a)tw = 1.6 mm, s = 75 mm, and ρ = 60 kg/m3 and (b) tw = 1.6 mm, s = 125 mm, and ρ = 100 kg/m3.
(a)
(b)Figures7(a) and 7(b) show the influence of foam density (ρ) on the ultimate bending strength of GFFW decks. Compared to specimens P4S7W1T3 (ts = 3.2 mm, s = 75 mm, and tw = 1.6 mm) and P4S1W1T3 (ts = 3.2 mm, s = 125 mm, and tw = 1.6 mm) with 40 kg/m3 foam density, the ultimate bending strength of specimens P6S7W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) and P6S1W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) with 60 kg/m3 foam density increased by 54.3% and 103.8%, respectively, and the ultimate bending strength of specimens P1S7W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) and P1S1W1T3 (ts = 1.6 mm, s = 75 mm, and tw = 1.6 mm) with 100 kg/m3 foam density increased by 31.1% and 78.8%, respectively.Figure 7
The influence of foam density: (a)ts = 3.2 mm, s = 75 mm, and tw = 1.6 mm and (b) ts = 3.2 mm, s = 125 mm, and tw = 1.6 mm.
(a)
(b)Figures8(a) and 8(b) show the influence of web thickness (tw) on the ultimate bending strength of GFFW decks. Compared to Specimen P6S7W1T3 (ts = 3.2 mm, s = 75 mm, and ρ = 60 kg/m3) with 1.6 mm thick web thickness, the ultimate bending strength of Specimen P6S7W3T3 with 3.2 mm web thickness increased by 67.8%. Compared to Specimen P6S1W1T3 (ts = 3.2 mm, s = 125 mm, and ρ = 60 kg/m3) with 1.6 mm thick web thickness, the ultimate bending strength of Specimen P6S1W4T3 with 4.8 mm web thickness increased by 99.5%.Figure 8
The influence of web thickness: (a)ts = 3.2 mm, s = 75 mm, and ρ = 60 kg/m3 and (b) ts = 3.2 mm, s = 125 mm, and ρ = 60 kg/m3.
(a)
(b)Figures9(a) and 9(b) show the influence of web spacing (s) on the ultimate bending strength of GFFW decks. Under the conditions of ts = 3.2 mm, tw = 1.6 mm, and ρ = 60 kg/m3, the ultimate bending strength of Specimen P6S7W1T3 (s = 75 mm) was 83.3 kN, which was 29.1% larger than that of Specimen P6S1W1T3 (s = 125 mm). Under the conditions of ts = 3.2 mm, tw = 1.6 mm, and ρ = 100 kg/m3, the ultimate bending strength of Specimen P1S7W1T3 (s = 75 mm) was 83.3 kN, which was 25.0% larger than that of Specimen P1S1W1T3 (s = 125 mm).Figure 9
The influence of web spacing: (a)ts = 3.2 mm, ρ = 60 kg/m3, and tw = 1.6 mm and (b) ts = 3.2 mm, ρ = 100 kg/m3, and tw = 1.6 mm.
(a)
(b)Hence, a larger face sheet thickness, foam density, and web thickness can lead to a higher ultimate bending strength of the GFFW decks, while a larger web spacing can lead to a lower ultimate bending strength of the GFFW decks.


## 3.3. Initial Bending Stiffness

The initial bending stiffness of a deck (Ke) is determined by(1)Ke=PyΔy,where Py and Δy are the yield strength of a deck and corresponding yield deflection, respectively (see Figure 10).Figure 10
The idealised load-midspan deflection curve.Figure11(a) shows the influences of GFRP face sheet thickness on the initial bending stiffness of GFFW decks. Compared to Specimen P6S7W1T1 (Ke = 2.19 kN/mm) with 1.6 mm face sheet thickness, Ke of Specimens P6S7W1T3 (ts = 3.2 mm) and P6S7W1T4 (ts = 4.8 mm) increased by 107.7% and 168.7%, respectively. Compared to Specimen P1S1W1T1 (Ke = 1.85 kN/mm) with 1.6 mm face sheet thickness, Ke of Specimens P1S1W1T3 (ts = 3.2 mm) and P1S1W1T4 (ts = 4.8 mm) increased by 97.9% and 465.4%, respectively. Thus, using thicker GFRP face sheet can improve the initial bending stiffness of decks significantly.Figure 11
Initial bending stiffness: (a) the influence of face sheet thickness, (b) the influence of foam density, (c) the influence of web thickness, and (d) the influence of web thickness.
(a)
(b)
(c)
(d)Figure11(b) shows the influences of foam density on the initial bending stiffness of GFFW decks. Compared to Specimen P4S7W1T3 (Ke = 2.44 kN/mm) with 40 kg/m3 foam density, Ke of Specimens P6S7W1T3 (ρ = 60 kg/m3) and P1S7W1T3 (ρ = 100 kg/m3) were 4.55 kN/mm and 7.20 kN/mm, respectively, which were 86.4% and 194.9% greater than that of Specimen P4S7W1T3. Compared to Specimen P4S1W1T3 (Ke = 2.23 kN/mm) with 40 kg/m3 foam density, Ke of Specimens P6S1W1T3 (ρ = 60 kg/m3) and P1S1W1T3 (ρ = 100 kg/m3) were 3.66 kN/mm and 5.14 kN/mm, respectively, which were 64.1% and 130.3% greater than that of Specimen P4S7W1T3. The foam with larger density also behaves stiffer. Therefore, a larger foam density can generate a larger bending stiffness.Figure11(c) shows the influences of web thickness on the initial bending stiffness of GFFW decks. Compared to specimens P6S7W1T3 (ts = 3.2 mm, s = 75 mm, and ρ = 60 kg/m3) and P6S1W1T3 (ts = 3.2 mm, s = 125 mm, and ρ = 60 kg/m3) with 1.6 mm web thickness, Ke of specimens P6S7W3T3 with 3.2 mm web thickness and P6S1W4T3 with 4.8 mm web thickness increased by 180.4% and 157.8%, respectively, which were equal to 12.75 kN/mm and 9.44 kN/mm. Because increasing the web thickness can result in a larger ratio of the volume of web to foam, which can increase the equivalent Young’s modulus according to (3), a larger ultimate bending strength of GFFW deck can be achieved.Figure11(d) shows the influences of web spacing on the initial bending stiffness of GFFW decks. For Specimens P6S7W1T3 and P1S7W1T3 with 75 mm web spacing, 1.6 mm web thickness, 3.2 mm face sheet thickness, and 60 kg/m3 foam density, Ke of them were 4.55 kN/mm and 7.20 kN/mm, respectively, which were 24.3% and 40.1% greater than those of Specimens P6S1W1T3 and P1S1W1T3 with 125 mm web spacing, 1.6 mm web thickness, 3.2 mm face sheet thickness, and 60 kg/m3 foam density. Decreasing web spacing can increase the ratio of the volume of web to foam, which was the same as the thicker webs. Hence, the equivalent Young’s modulus can be improved. Furthermore, the larger ratio of the volume of web to foam can enhance the shear capacity and face sheet/core adhesive strength of panels. Therefore, smaller web spacing leads to a higher ultimate bending strength.


## 3.4. Improvements in Displacement Ductility

The displacement ductility factor (η) is adopted to evaluate the ductility performance of the specimens, which is given by(2)η=ΔuΔy,where Δu is the ultimate deflection corresponding to the ultimate bending strength (see Figure 12).Figure 12
Displacement ductility factor: (a) the influence of face sheet thickness, (b) the influence of foam density, (c) the influence of web thickness, and (d) the influence of web thickness.
(a)
(b)
(c)
(d)As summarized in Table4, the displacement ductility factors range from 1.0 (for control specimens) to 2.88 (for Specimen P4S7W1T3). As shown in Figure 12(a), compared to Specimens P6S7W1T1 (η = 2.21) and P1S1W1T1 (η = 1.82) with 1.6 mm face sheet thickness, η of Specimens P6S7W1T3 (η = 1.86) and P1S1W1T3 (η = 1.66) with 3.2 mm face sheet thickness decreased by 18.8% and 9.6%, respectively; η of Specimens P6S7W1T4 (η = 1.49) and P1S1W1T4 (η = 1.46) with 4.8 mm face sheet thickness decreased by 48.3% and 24.7%, respectively. Hence, using thinner GFRP face sheet can effectively improve the displacement ductility of GFFW decks.In terms of the influence of foam density on the displacement ductility (see Figure12(b)), compared to Specimen P1S7W1T3 (η = 1.46) with 100 kg/m3 foam density, η of Specimens P4S7W1T3 with 40 kg/m3 foam density and P6S7W1T3 with 60 kg/m3 foam density increased by 65.5% and 6.7%, respectively, which were equal to 2.88 and 1.86. Compared to Specimen P1S1W1T3 (η = 1.66) with 100 kg/m3 foam density, η of Specimens P4S1W1T3 with 40 kg/m3 foam density and P6S1W1T3 with 60 kg/m3 foam density increased by 19.8% and 6.5%, respectively, which were equal to 1.99 and 1.77. Therefore, the displacement ductility factor can become smaller with the increase in the foam density.As shown in Figure12(c), using thicker web tw = 3.2 mm for strengthening Specimen P6S7W3T3 and tw = 4.8 mm for strengthening Specimen P6S1W4T3 instead of thinner web (tw = 1.6 mm) for Specimens P6S7W1T3 and P6S7W1T3, η of P6S7W3T3 and P6S1W4T3 were almost 85% when compared with their counterpart. Hence, the thinner web can result in better ductility of decks. For the influence of web spacing on the displacement ductility (see Figure 12(d)), compared to Specimens P6S7W1T3 and P1S7W1T3 (s = 75 mm), η of Specimens P6S1W1T3 and P1S1W1T3 with 125 mm web spacing decreased by 4.8% and 4.5%, respectively. Thus, the displacement ductility of GFFW decks can be affected by web spacing slightly.


## 3.5. Energy Dissipation

The energy ductility coefficient (μ) was much more reasonable to evaluate the postyield deformation of the decks [14], which can be expressed as(3)μ=EuEy,where the yield energy Ey is the triangular area under the load-midspan deflection curve and the ultimate energy Eu is the total area under the load-midspan deflection curve (see Figure 10).As summarized in Table4, the energy ductility coefficients of control specimens are the smallest, which were nearly equal to 1.0. Figure 13(a) shows the influence of face sheet thickness on the energy ductility coefficient of decks. Comparison of the values of μ of Specimens P6S7W1T1, P6S7W1T3, and P6S7W1T4 indicates that increasing the skin thickness from 1.6 mm to 4.8 mm decreased the energy ductility coefficient of the deck by 25.9% and 42.4% relative to μ of Specimen P6S7W1T1. Similarly, comparison of the values of μ of Specimens P1S1W1T1, P1S1W1T3, and P1S1W1T4 shows that increasing the skin thickness from 1.6 mm to 4.8 mm decreased the energy ductility coefficient of the deck by 13.8% and 28.2% relative to μ of Specimen P1S1W1T1. Figure 13(b) shows the influence of foam density on the energy ductility coefficient of decks. Compared to Specimen P1S7W1T3 (μ = 2.65) with 100 kg/m3 foam density, μ of Specimens P4S7W1T3 with 40 kg/m3 foam density and P6S7W1T3 with 60 kg/m3 foam density were equal to 5.77 and 2.74, which increased by 117.8% and 3.4%, respectively. Compared to Specimen P1S1W1T3 (μ = 2.47) with 100 kg/m3 foam density, μ of Specimens P4S1W1T3 with 40 kg/m3 foam density and P6S1W1T3 with 60 kg/m3 foam density were equal to 3.28 and 2.61, which increased by 32.6% and 5.5%, respectively. Turning to the influence of web thickness on the energy ductility coefficients, as shown in Figure 13(c), compared to Specimens P6S7W1T3 (μ = 2.74) and P6S1W1T3 (μ = 2.61) with 1.6 mm web thickness, μ of Specimens P6S7W3T3 with 3.2 mm web thickness and P6S1W4T3 with 4.8 mm web thickness were equal to 2.11 and 2.04, which slightly decreased by 23.0% and 21.8%, respectively. As shown in Figure 13(d), Although the web spacing of Specimens P6S1W1T3 and P1S1W1T3 was nearly 1.7 times of that of Specimens P6S7W1T3 and P1S7W1T3 (s = 75 mm), the energy ductility coefficients were 4.9% and 6.8% smaller than that of Specimens P6S7W1T3 and P1S7W1T3, which were equal to 2.74 and 2.65, respectively. Therefore, the test results indicate that the energy ductility coefficients of GFFW decks were mainly affected by face sheet thickness, foam density, and the web thickness. The thinner face sheet, smaller foam density, and thinner web can provide better energy dissipation.Figure 13
Energy ductility coefficient: (a) the influence of face sheet thickness, (b) the influence of foam density, (c) the influence of web thickness, and (d) the influence of web thickness.
(a)
(b)
(c)
(d)


## 4. Conclusions

This paper presents the experimental study on the sandwich bridge decks with GFRP face sheets and a foam-web core loaded under two-way bending. The main findings of this study are summarized as follows:(1)
A new type of sandwich bridge decks with GFRP face sheets and a foam-web core was developed by means of vacuum assisted resin infusion process. These decks had the characteristics of high ultimate bending strength and initial bending stiffness.(2)
The experimental results show that, compared to the normal foam-core sandwich decks, a maximum of an approximately 657.1% increase in the ultimate bending strength of GFFW decks can be achieved due to the use of GFRP webs.(3)
The thicker GFRP face sheets, the smaller web spacing, the larger foam density, and the thicker GFRP webs can significantly enhance the ultimate bending strength and initial bending stiffness of GFFW decks. But the displacement ductility of GFFW decks can be affected by face sheet thickness slightly.(4)
The test results indicated that the displacement ductility of GFFW decks was mainly affected by the face sheet thickness, foam density, and web thickness, while the displacement ductility of GFFW decks decreased with the increase in web spacing slightly.(5)
The test results demonstrated that the energy ductility coefficient of GFFW decks decreased with the increase in face sheet thickness, foam density, and web thickness, while the energy ductility coefficient was not mainly affected by the web spacing.(6)
This new type of sandwich bridge decks with GFRP face sheets and a foam-web core is still under development; the corresponding numerical and analytical model will be developed to calculate the ultimate bending strength and deflection, and the minimum weight design procedure will also be proposed after carrying out more tests and simulation of GFFW decks.



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*Source: 434721-2015-10-04.xml*