Introduction

Due to acute housing shortage there is a need for the development of an appropriate cheap construction technology. Thus any effort in the direction of cost reduction of housing elements will be a valuable contribution and service to the society. Ferrocement is a composite material in which filler material called matrix, is reinforced with fibers dispersed throughout composite. The distribution of the reinforcement is made uniform by spreading out the wire meshes throughout the thickness of the member. This dispersion of the wire meshes in the brittle matrix offers not only convenience and practical means of achieving improvements in many structural engineering properties of the material such as fracture, tensile and flexural strength, toughness, fatigue and impact resistance and at the same time provide ease of construction. The uniform distribution and larger surface area of reinforcing material provides better crack prevention properties. Thus, ferrocement can be considered as a promising material system to address the low cost housing issue.

Numerous investigations have been carried out in past to establish the mechanical behavior of ferrocement under both static and dynamic loads. The researches have been carried out to determine the behavior of ferrocement in flexure and concluded that strength bears direct relation with number of layers and fineness of mesh [1]. The influence of skeletal steel on flexural behavior of ferrocement and concluded that skeletal steel does not contribute significantly towards the cracking strength [2]. The cracking behaviour of ferrocement have been discussed by different researchers [3]. Some researches have investigated crack arrest performance of ferrocement [4]. The experimental studies were carried out to determine the flexural behavior of polymer mixed ferrocement and concluded that first cracking load and ultimate load increases with the increase of polymer cement ratio [5]. The effect of partial replacement of cement with fly ash in the ferrocement panels, was investigated by various scientists [6]. No significant drop in the flexural strength of panels using fly ash was observed up to 20 % partial replacement of cement.

The main objective of the present investigation is to assess the strength and structural performance of ferrocement roofing system comprising of pre-cast ferrocement panels resting on two RC pre-cast beams and brick masonry walls on all four sides of an enclosure of size 2,400 × 2,250 mm. A similar test was also undertaken on roofing system using RC pre-cast beam and red sand stone panels for comparison of strength and cost.

Experimental Procedure

Two sets of ferrocement panels with 0 and 20 % partial replacement of cement with fly ash in three replications each were prepared. The roof slab system comprised of these pre-cast panels resting on two pre-cast RC beams and brick masonry walls on all four sides of an enclosure as shown in Fig. 1. Thus for each set of roofing system, 12 pre-cast ferrocement panels were used. The load was transferred through a load tree at a total of 48 points on slab surface (Fig. 2). The load was applied on incremental basis. For each increment of load, the deflection was measured up to failure for all the six sets (three replications each for 0 and 20 % replacement of cement by fly ash). The first crack load, ultimate load and failure pattern was studied. In a similar manner tests were also conducted on roofing system assembly using sand stone panels in place of ferrocement panels.

Fig. 1
figure 1

Placement of the panels (marked 1–12) resting on RC Beams and Brick Masonry Walls

Fig. 2
figure 2

A schematic view of loading arrangement at 48 points on the slab panel

Materials Used

Ordinary Portland cement (43 grade) conforming to IS:8112-1989 [7] was used. The physical properties of cement were determined in the laboratory and presented in Table 1. The electro-statically precipitated fly ash was procured from NTPC Dadari (U.P.). The fly ash had a fineness of 3,800 cm2/g. The constituents of the fly ash were SiO2 (45–60 %) Al2O3 (10–30 %) and Fe2O3 (5–25 %) conforming to IS: 3812-1981 [8]. The physical properties of fly ash are given in Table 2. Locally available coarse sand (called Badarpur) with a silt content of 2.3 % was used. The grading and fineness modulus of the sand are given in Table 3. The crushed granite aggregate was used as coarse aggregate in RC beams. The grading and fineness modulus of the coarse aggregate are given in Table 4. The fineness modulus of fine and coarse aggregate was determined as per IS:2386 (Part I and II)-1963 [9]. Woven galvanized steel wire mesh with a wire diameter of 0.5 mm was used. The properties of the woven mesh are given in Table 5.

Table 1 Properties of cement
Table 2 Properties of fly ash
Table 3 Sieve analysis of fine aggregate (coarse sand)
Table 4 Sieve analysis of coarse aggregate
Table 5 Properties of wire mesh

Mix Proportions

Two cement mortar mixes 1.0:0.0:2.5 and 0.8:0.20:2.5, comprising of cement: fly ash: sand (fine aggregate) were used in ferrocement panels. To achieve proper workability, water cement ratio of mortar was kept as 0.40. For RC beams, concrete mix in proportion of 1:2:4 comprising of cement: fine aggregate: coarse aggregate was used. To achieve proper workability, water cement ratio in the concrete mix was kept as 0.5. Control specimens were cast to determine the strength of mortar. These cubes and briquettes were cured for 28 days and tested in accordance with the codal provisions. The strength of mortar control specimens is given in Table 6.

Table 6 Tests on mortar control specimens

Details of Frerrocement Panels and RC Beams

For each set of roof floor system a total of 12 pre-cast ferrocement panels were used to cover the enclosed area of 2,400 × 2,250 mm. The top levels of the two pre-cast RC beams spanning along 2,400 mm span and resting directly on two opposite side walls at 1/3 locations of 2,250 mm span from both sides, were flushed with the top of the walls. Each ferrocement panel thus had sufficient bearing either on beams and walls or on the beams. The panels dimensions were 750 × 600 × 18 mm with two layers of woven wire mesh whereas the beam cross-section was 150 × 100 mm. The beams were reinforced with 2 Nos. 8 mm diameter Fe415 steel at top and bottom corners with two legged 6 mm diameter shear stirrups @ 100 mm c/c. The details of ferrocement panels and RC beams are given in Table 7.

Table 7 Details of ferrocement panels and RC beams

Casting of Test Panels and RC Beams

For the casting of test panels, mortar was spread in the wooden mould. The first wire mesh layer is laid on this 6 mm thick uniform mortar layer. After the mesh has been laid, the next set of ply sheet is put and again the mortar layer is spread on the wire mesh layer. This process is repeated till the required thickness of panel is obtained. These panels were demoulded after 24 h and cured with gunny bags for 28 days. The cured panels were air dried for 4 days before the actual testing. For the casting of the RC beam, the material was weighed, dried and then mixed in a concrete mixture. Before casting, oil was smeared on inner surface of the mould and concrete was poured in layers. Care was taken to ensure that concrete was properly laid and compacted beneath the reinforcement and also along the side of the mould.

Experimental Setup

The test setup consists of loading frame of 500 kN capacity. Half brick thick wall (115 mm) was erected on the beams of the loading frames. Two RC beams were put on the brick walls and slab panels were placed on the beams and walls, which form roof slab systems.

A schematic view of loading arrangement at 48 points on the slab panel can be seen in Fig. 2. The loading arrangement on the slab panel is shown in Fig. 3. The position of dial gauges is shown in Fig. 4. The loads were applied through a reaction frame using hydraulic jack of 100 kN capacity activated by a high pressure manually operated pump fitted with a bourdon tube pressure gauge. A proving ring of 100 kN capacity was used to measure the applied load accurately. The load was uniformly transferred at 48 points. The deflections were recorded with the help of 12 dial gauges set below the centre of each panel. The first crack load, ultimate load and deflection at each increment of load were recorded. Similar tests were made on another roofing system comprising of red sand stone panels in place of ferrocement panels keeping the dimensions of red sand stone panels same as that of ferrocement panels.

Fig. 3
figure 3

Loading arrangement on slab panels

Fig. 4
figure 4

Set-up of dial gauges under slab panels (underside view)

The roof slab system was tested under flexure as shown in Fig. 5. Mechanical dial gauges mounted on magnetic base having least count of 0.01 mm were used to obtain the deflection at various stages of loading at the centre of each panel. The load was increased gradually till the slab panels failed. In all the tests carried out, the first crack load, ultimate load and corresponding deflection were observed. The crack pattern and failure mechanisms were also studied. All the ferrocement panels failed in flexure modes with the cracks parallel to the shorter sides as shown in Figs. 6 and 7. The test results have been presented in Tables 8 and 9. Similarly test on roof slab system consisting of sand stone panels under same support condition was also undertaken. However, for the roof in sand stone panels, only the ultimate load and the cracking pattern were observed. The tested roof slab system consisting of sand stone panels resting over RC beams is shown in Fig. 8.

Fig. 5
figure 5

Ferrocement slab panel under test

Fig. 6
figure 6

Crack pattern in ferrocement panels with 0 % fly ash (underside view)

Fig. 7
figure 7

Crack pattern in ferrocement panels with 20 % fly ash (underside view)

Table 8 Load deflection values for ferrocement slab system without fly ash
Table 9 Load deflection values for Ferrocement slab system with 20 % fly ash
Fig. 8
figure 8

Crack pattern in sand stone panels (underside view)

Theoretical Calculations

The theoretical analysis of the ferrocement panels was undertaken to ascertain their flexural characteristics using classical approaches given by ACI 549.1R-88 [10] and other researchers [2, 3]. The behavior at the first crack load and the ultimate load was investigated.

Panel without Fly Ash

The analysis was carried out using the following set of data

$$ f_{ck} = { 3}0\;\;{\text{N/mm}}^{ 2} $$
$$ E_{m} = { 473}0\quad \sqrt {f_{ck} } = { 259}0 7\;\;{\text{N/mm}}^{ 2} $$
$$ f_{t} = { 3}\;\;{\text{N/mm}}^{ 2} $$
$$ E_{f} = \, 0. 9\times 10^{ 5} \;{\text{N/mm}}^{ 2} \quad f_{y} = 3 50\;\;{\text{N/mm}}^{ 2} \quad {\kern 1pt} V_{f} = \, 0. 8\;\;\% \quad \eta \; = \, 0. 9 $$

Section b = 750 mm, h = 18 mm

Theoretical Moment Calculation

As per the recommendations of ACI 549.1R-88 [11], the nominal moment strength of ferrocement section subjected to pure flexure is given by

$$ \frac{{M_{{n{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} }} }}{{f_{ck} bh^{2} \eta }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} 0.005{\kern 1pt} {\kern 1pt} {\kern 1pt} + {\kern 1pt} {\kern 1pt} {\kern 1pt} 0.422{\kern 1pt} {\kern 1pt} {\kern 1pt} \quad V_{f} {\kern 1pt} \frac{{f_{y} }}{{f_{ck} }}{\kern 1pt} - 0.0772{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \left( {{\kern 1pt} V_{f} {\kern 1pt} \frac{{f_{y} }}{{f_{ck} }}} \right)^{2} $$
$$ \begin{gathered} {\text{For}}\,\,{\kern 1pt} V_{f} {\kern 1pt} \frac{{f_{y} }}{{f_{ck} }}{\kern 1pt} \, = \, 0.0 9 3\hfill \\ M_{{n{\kern 1pt} }} = { 22953}0\;\;{\text{N/mm}} \hfill \\ \end{gathered} $$

This matches well with the external moment calculated by considering the panels to be simply supported along shorter side. The maximum moment corresponding to the first crack load is 225,000 N/mm and the maximum moment corresponding to the ultimate load is 275,000 N/mm.

Crack Width Calculation

Analysing the section as cracked section with the depth of neutral axis as c

$$ \frac{{bc^{2} }}{2} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{E_{f} }}{{E_{m} }}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \sum\limits_{i = 1}^{m} {A_{si} (d_{i} - c)} $$

The area of each layer of reinforcement A si  = 39.27 mm2

Hence c = 2.22 mm

$$ {\text{Now}},\,\,I_{{cr{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{1}{3}bc^{3} {\kern 1pt} {\kern 1pt} {\kern 1pt} + {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \sum\limits_{i = 1}^{m} {{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{E_{f} }}{{E_{m} }}{\kern 1pt} A_{si} \left( {d_{i} - c} \right)^{2} } \,\, = { 17733}. 2 8\;\;{\text{mm}}^{ 4} $$
$$ {\text{At the first crack load maximum stress in concrete }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{225000 \times 2.22}{17733.28}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} = { 28}. 1 7\;\;{\text{N/mm}}^{ 2} $$
$$ {\text{Maximum stress in extreme tension layer }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{225000 \times \left( {12 - 2.22} \right){\kern 1pt} {\kern 1pt} {\kern 1pt} \times 3.474}}{17733.28}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} = { 431}.0 8\;\;{\text{N/mm}}^{ 2} $$

Using the simplified approach, the maximum crack width \( W_{{\hbox{max} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} S\beta \varepsilon_{s} {\kern 1pt} \)

where, S = wire spacing, \( \beta {\kern 1pt} \, = \,{\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{\left( {h - c} \right)}}{{\left( {d_{\hbox{max} } - c} \right)}}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \) and \( \varepsilon_{s} {\kern 1pt} \, = \,{\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{f_{s\hbox{max} } }}{{E_{f} }}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \)

Therefore, the maximum crack width at the first crack load = 0.03 mm

Similarly, the maximum crack width at the ultimate load = 0.0375 mm.

Panel with Fly Ash

The analysis was carried out using the following set of data

$$ f_{ck} = { 21}\;\;{\text{N/mm}}^{ 2} $$
$$ E_{m} = { 473}0\quad \sqrt {f_{ck} } = { 21675}. 6\;\;{\text{N/mm}}^{ 2} $$
$$ f_{t} = { 2}. 3\;\;{\text{N/mm}}^{ 2} $$
$$ E_{f} = \, 0. 9\times 10^{ 5} \;\;{\text{N/mm}}^{ 2} \,\,\,\,\,\,{\kern 1pt} f_{y} = 3 50\;\;{\text{N/mm}}^{ 2} \,\,\,\,\,V_{f} = \, 0. 8\, \% \,\,\,\,\,\eta = \, 0. 9 $$

Section b = 750 mm, h = 18 mm

Theoretical Moment Calculation

As per the recommendations of ACI 549.1R-88, the nominal moment strength of ferrocement section subjected to pure flexure is given by

$$ \frac{{M_{{n{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} }} }}{{f_{ck} bh^{2} \eta }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} 0.005{\kern 1pt} {\kern 1pt} {\kern 1pt} + {\kern 1pt} {\kern 1pt} {\kern 1pt} 0.422{\kern 1pt} {\kern 1pt} \quad {\kern 1pt} V_{f} {\kern 1pt} \frac{{f_{y} }}{{f_{ck} }}{\kern 1pt} - 0.0772{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \left( {{\kern 1pt} V_{f} {\kern 1pt} \frac{{f_{y} }}{{f_{ck} }}} \right)^{2} $$

For \( {\kern 1pt} V_{f} {\kern 1pt} \frac{{f_{y} }}{{f_{ck} }}{\kern 1pt} = \, 0. 1 3 3 \)

$$ M_{{n{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} }} = { 22}0 4 4 9\;\;{\text{N/mm}} $$

This matches well with the external moment calculated by considering the panels to be simply supported along shorter side. The maximum moment corresponding to the first crack load is 200,000 N/mm and the maximum moment corresponding to the ultimate load is 225,000 N/mm.

Crack Width Calculation

Analysing the section as cracked section with the depth of neutral axis as c

$$ \frac{{bc^{2} }}{2} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{E_{f} }}{{E_{m} }}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \sum\limits_{i = 1}^{m} {A_{si} (d_{i} - c)} $$

The area of each layer of reinforcement A si  = 39.27 mm2

c = 2.4 mm

Now, \( I_{{cr{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{1}{3}bc^{3} {\kern 1pt} {\kern 1pt} {\kern 1pt} + {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \sum\limits_{i = 1}^{m} {{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{E_{f} }}{{E_{m} }}{\kern 1pt} A_{si} \left( {d_{i} - c} \right)^{2} } = { 2}0 5 9 5. 7 1 5\;\;{\text{mm}}^{ 4} \)

$$ {\text{Now at the first crack load}},{\text{ maximum stress in concrete }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{200000 \times 2.4}{20595.715}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} = { 23}. 3 1\;\;{\text{N/mm}}^{ 2} $$
$$ {\text{Maximum stress in extreme tension layer }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{200000 \times \left( {12 - 2.4} \right){\kern 1pt} {\kern 1pt} {\kern 1pt} \times 4.152}}{20595.715}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} = { 387}.0 6\;\;{\text{N/mm}}^{ 2} $$

Using the simplified approach, the maximum crack width \( W_{{\hbox{max} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} }} = {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} S\beta \varepsilon_{s} {\kern 1pt} \)

where, S = wire spacing, \( \beta {\kern 1pt} = {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{\left( {h - c} \right)}}{{\left( {d_{\hbox{max} } - c} \right)}}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \) and \( \varepsilon_{s} {\kern 1pt} = {\kern 1pt} {\kern 1pt} {\kern 1pt} \frac{{f_{s\hbox{max} } }}{{E_{f} }}{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \)

Therefore, the maximum crack width at the first crack load = 0.035 mm

Similarly, the maximum crack width at the ultimate load = 0.0437 mm.

The above calculations clearly establish the adequacy of sections to sustain the flexural loading applied in the present investigation.

Result and Discussion

The investigation was aimed at exploring the static live load carrying capacity of the floor slab. As per the provisions of IS: 875 (1987) Part 2, for the residential buildings the imposed floor load for different occupancies normally varies between 2 and 3 kN/m2 whereas the same under specific exceptional cases is taken around 4–5 kN/m2. Hence, the slabs are normally designed to carry live load of the respective magnitude. As a matter of fact, the first crack load and the ultimate load should have been expressed in kN only. In the present paper these have been expressed in kN/m2 by dividing the load in kN with the overall area of the floor slab taking into account the 12 pre-cast ferrocement panels. This overall area has been taken as 2,400 × 2,250 mm neglecting deductions on account of bearing on supports. The load–deflection values for ferrocement panels with 0 and 20 % fly ash are given in Tables 8 and 9 respectively. The ferrocement panels without fly ash possess larger load carrying capacity as compared to panels with 20 % fly ash. The first crack load and the ultimate load of the slab system with 0 % fly ash are found to be 7.9 and 9.8 kN/m2 respectively. The maximum deflection is found in panel No. 6 and is observed to be 9.23 mm at ultimate load. Similarly the first crack load and the ultimate load of the panels with 20 % fly ash are observed to be 7.0 and 8.4 kN/m2 respectively. The maximum deflection is found in panel No. 6 which is 7.26 mm at the ultimate load. As the load was increased the first cracks were seen due to failure of mortar on the tension face. However, the load carrying capacity of the panels continues to increase. This is apparently because meshes start carrying additional loads. With the load increment, the mortar layer above the lower most mesh also starts cracking. At this stage cracks also develop on the top most mortar layer. Subsequent cracking is due to the propagation of cracks from bottom as well as top. After the first crack, the crack propagation is characterized by the number of cracks and the crack width. Immediately after the first cracking, in the next stage, the cracks increase in number, followed by the third stage where the width of the crack increases. Multiple cracks were observed in all the slab panels. The crack width at the center of panels widened with the increase of load as shown in Figs. 6 and 7. The roof slab system comprising of red sand stone panels resting over RC beams shows brittle failure with an ultimate load level of 6.55 kN/m2. A single transverse crack parallel to the support at the centre of the individual panel was observed at failure. The crack pattern is shown in Fig. 8. The load deflection curves for different ferrocement panels with 0 and 20 % fly ash in the roof slab system are shown in Figs. 9 and 10. The load deflection values reveal that the load carrying capacity and the deflection decreases with increase in fly ash content. The load deflection curve for ferrocement tested under flexure can be divided into three stages namely pre cracking, post cracking and post yielding stage. It exhibits highest stiffness in the pre cracking range where mortar contributes to both compressive and tensile resistance of the composite along with the reinforcement. The post cracking range starts with the occurrence of first crack. This stage extends up to point where the extreme tension fibre of reinforcement starts yielding. After cracking the tensile force contribution of mortar is negligible compared to the contribution of reinforcement. In the post yielding range multiple cracking, crack widening and yielding of subsequent mesh layers take place. It may, therefore, be concluded that with the enhanced distribution and subdivision of wire meshes, the concrete can undergo large strains in the neighborhood of reinforcement thus imparting it an enhanced ductility. Thus the ferrocement panels exhibit a ductile failure and their load carrying capacity is greater than the red sand stone panels. The red sand stone panels exhibit a brittle failure. The first crack load and ultimate load carrying capacity of ferrocement slab system with 0 % fly ash are 12.86 and 16.67 % greater than that for the ferrocement slab system with 20 % fly ash. The ultimate load carrying capacity of the ferrocement slab system with 0 % fly ash is 49.62 % higher than the red sand stone slab system whereas ultimate load carrying capacity of the ferrocement slab system with 20 % fly ash is 28.24 % higher than the red sand stone slab system. The theoretical calculations establish the adequacy of the sections to sustain the flexural loading applied in the present investigation.

Fig. 9
figure 9

Load–deflection curves for ferrocement system without fly ash

Fig. 10
figure 10

Load–deflection curves for ferrocement system with 20 % fly ash

Cost Comparison

To cover the same area of 2,400 × 2,250 mm, the cost comparison of different slab systems e.g. ferrocement panels with 0 % fly ash resting over RC beams and walls, ferrocement panels with 20 % fly ash resting over RC beams and sand stone panels resting over RC beams. Although experimental tests were not carried out on other slab systems e.g. sand stone panels resting over steel girders, RB slab and RC slab etc. However for the purpose of cost comparison the latter slab systems were also included and their cost was considered on the basis of prevailing market rates. The estimated cost includes the cost of slab as well as the beams wherever provided. The cost comparison is presented in Table 10. The cost of ferrocement panels resting over RC beams is found to be cheaper than the cost of red sand stone panels resting over RC beams. It is also observed that cost of ferrocement slab system with 0 and 20 % fly ash is less than the cost of conventional RC slab by 59 and 62 % respectively.

Table 10 Comparison of cost for various types of roofing systems

Although in the present investigation the supported span of the beam has been taken as 2,400 mm (8 feet), the beam cross section was found to be safe even for 3,000–3,600 mm (10–12 feet) span. Thus even if the longitudinal dimension is increased to any size, as per the requirement, by using additional number of beams, it is apparent that the proposed floor system can be safely adapted for almost all sorts of commonly used room sizes.

Conclusion

The investigations undertaken clearly highlight the suitability of using roof slab system comprising of ferrocement panels with 0 and 20 % fly ash resting over RC beams for low cost housing as it has lower crack width, compared to other alternatives. The aforesaid system is ductile and economically viable as compared to the other prevalent floor systems. The technology can be used not only for greater cost reduction benefits but also for effective utilization of fly ash waste thereby conserving the environment as well without any compromise on the structural integrity of the resulting system. The approach will be especially useful for low cost row housing schemes and emergency shelter housing projects for disaster affected areas.