1. Introduction
Fiber pull-out is generally considered to be the dominating failure mechanism in fiber reinforced concrete (FRC) to mitigate brittle failure. Accordingly, pull-out tests are typically performed on FRC to characterize the fiber-matrix behavior and estimate average tensile stresses near a crack opening. However, little direct insight can be gained on the actual mechanisms of the pull-out from such test, whereas, a deeper understanding of the underlying interaction mechanisms between discrete fibers and the surrounding concrete matrix could clearly lead to optimized FRC. Such deeper understanding could be gained through the addition of non-destructive techniques to pull-out tests to enable the visualization and quantification of the mechanical interaction between the fibers and the concrete matrix.
X-ray micro-tomography (µXRT) is a non-destructive 3D imaging technique that has in recent years become a useful tool in engineering and material science to characterize the internal structures and mechanisms of a wide range of materials [
1,
2]. µXRT has most commonly been applied on unloaded material samples, but with in-situ devices it is possible to run mechanical tests within a tomograph thus enabling scanning during loading of specimens [
3]. Coupling of µXRT with Digital Volume Correlation (DVC) has been applied to analyze the interior structural evolution of an array of materials, e.g., concrete [
4], bone [
5], wood [
6], rock [
7] and granular materials [
8]. DVC can essentially be considered as an extension of Digital Image Correlation (DIC) applied to tomographic image volumes to calculate full 3D vector displacements, from which tensor strain fields can be derived.
This paper presents the development of a method enabling the visualization and quantitative analysis of the fiber-matrix interaction on a meso-mechanical level in FRC samples. Reference tests are first described that provided characterization of the pull-out behavior of a steel fiber centrically cast in small cylindrical concrete specimens. These tests were also used to determine load levels at which µXRT imaging was performed during pull-out tests in-situ in an X-ray tomograph. The pull-out test rig, tailored to the constraints of the µXRT equipment and mechanical loading configuration, is described. Results from the tests and analysis, including using DVC, are presented and discussed for one fiber type in terms of the mechanical processes occurring in and around the fiber.
2. Materials and Methods
2.1. Selected Materials and Test Specimens
Cylindrical concrete specimens (
h = 50 mm, Ø = 43 mm) each containing a singular steel fiber partly cast perpendicular and centric to the concrete surface (
Figure 1a) were specifically prepared to accommodate a test setup having the possibility to apply a pull-out load while being placed in a tomograph. A high performance concrete mix developed for use in fiber-based reinforced concrete composites was used. This concrete mixture includes a CEM II/A-V 52.5 N Portland-fly ash cement, additional fly ash, chemical admixtures and a maximum aggregate size of 4 mm. The concrete was measured to have a compressive strength of 70 MPa and a tensile strength of 3.2 MPa at 28 days.
Six different steel fiber alternatives were selected for investigation, as illustrated in
Figure 1b. These fibers have varying anchorage characteristics such as hooked-ends, hooked and flattened ends and wavy structure. A summary of general material and mechanical properties for the selected fibers is provided in
Table 1. The embedded length,
Le, was set to 30 mm for all specimens. The scope of this paper is limited to Dramix 3D.
2.2. Reference Pull-Out Tests
A single-sided pull-out test was developed within the project, based on knowledge gathered from other studies (e.g., [
9]), to simulate a stress-state present at a crack opening. This method makes it possible to characterize the behavior of individual fibers when pulled-out of the concrete matrix in terms of a load versus displacement relationship. Pull-out tests were firstly conducted without µXRT according to
Figure 2a to characterize the load-displacement relationship for the different FRC specimens. Based on the outcome of the results of these tests, the final test schedule and load levels for the pull-out tests with µXRT were established. For example, suitable load levels for specimens with Dramix 3D fibers are indicated on the load-displacement curve in
Figure 2b. Load levels prior to the peak load are relevant to be able to capture the initial debonding of the fiber and transition from mechanical adhesion to frictional bond. At load levels approaching the peak load, it is hypothesized that the plastic deformation of the fiber can likely be observed. In the case of pull-out failure, it could also be relevant to capture the extent of plastic deformation and pull-out of the fiber within the post-peak region.
2.3. Pull-Out Tests with µXRT
The in-situ pull-out tests were performed in the Zeiss XRM520 at the 4D Imaging Lab at Lund University. A test specimen affixed to the loading device and a schematic of the test setup are shown in
Figure 3. Each concrete specimen was mounted on the top of the device, above the piston and supported around its outer edge by a PMMA tube. The fibers protruding from each specimen were glued with HBM X60 into a threaded end anchorage that was screwed onto the piston of the test rig. The pull-out load was applied by controlled downward displacement of this piston.
The µXRT acquisitions involved 1601 radiographic projections over 360° with a 2 s exposure time using a source voltage of 160 kV and power of 10 W plus the He3-filter (as provided by the manufacturer) to reduce beam hardening artefacts. A 0.4× objective was used and the camera binning was set to 2 × 2 giving images of 1024 × 1024 px. The voxels in the final reconstructed volumes were cubic with side lengths of 53 or 55 µm (depending on the test).
For each in-situ test, an initial scan was taken of the specimen prior to loading, which provided the undeformed reference image for the subsequent DVC-analyses. Thereafter, each specimen was loaded stepwise to the prescribed load levels at which new scans were made. One complete scan of the specimen took about 1 h at each load level, which amounts to approximately one day to execute a full test.
2.4. Processing with DVC
The StrainMaster software from LaVision was used for the DVC. The imported volume image is discretized into smaller sub-volumes containing unique grey-scale pattern. The software then correlates the pattern from the reference image to the deformed images and calculates the displacement within each sub-volume. This results in a full 3D vector field representing the specimen displacement, from which tensor strain fields are derived. In this study, the sub-volume size was set to 32 × 32 × 32 voxels and the sub-volume overlap to 75%. This is approximately equivalent to a sub-volume size of 1.7 × 1.7 × 1.7 mm and a resultant grid resolution of 0.4 × 0.4 × 0.4 mm.
The region outside the specimen and the steel fiber itself was excluded from the DVC analysis using an algorithmic masking. It is to say that lower and upper threshold limits of the grey-scales in the volume image were specified. Furthermore, for a sub volume to be used, the requirement of minimum number of valid voxels inside the sub volume was set to 90%. This provides more reliable results at the edge of the analyzed volume and, most importantly in this case, at the fiber-matrix interface.
3. Results
From the high-resolution µXRT images it was possible to have clear visualization of aggregates, pores, the fibers and the fiber-matrix interfaces. Furthermore, the natural grey-scale speckle in the images due to the chosen aggregate distribution and pores was found to be suitable for DVC analysis.
Two specimens with Dramix 3D fibers were tested, denoted as 3D-4 and 3D-5. Each specimen was imaged by µXRT at different load levels selected based on the load-displacement relations obtained in the reference pull-out tests. Images were acquired before and after peak load, as depicted in
Figure 4. Since the displacement was kept constant during the time of scanning, some relaxation in load could be observed at some of the scanning occasions.
The reconstruction of µXRT images provides a great deal of information related to both the geometry of the test specimen and the internal mechanisms taking place during loading. It is possible to distinguish the fibers final position in the specimen as well as the aggregate and pore distribution at the fiber interface. Moreover, the slipping or rupturing of the fiber within the so-called fiber canal can also be visualized. Furthermore, the DVC analysis of the time-series of volume images enabled the quantification of strains in the sample as well as the visualization of process details that were not visible simply from the tomography images.
Figure 5 presents how the hooked steel fiber in specimen 3D-5 deformed and slipped inside the canal at three different stages of the loading. The passive end slip was evaluated as the pixel distance (i.e., 1 px = 53 µm) between the fiber end and the bottom of the fiber canal. It was concluded that the fiber end started to slip around 500 N for specimen 3D-5, while no end slip was observed before fiber rupture occurred at 670 N for specimen 3D-4.
From the DVC analysis, it is possible to observe a change in the load transfer mechanism between the steel fibre and the concrete matrix. During the initial linear part of the load-displacement curve, elevated shear strains can be observed along and around the fibre, which according to theory can be due to adhesion and frictional bond, as exemplified in
Figure 6 at a load level of 400 N. When the fibre starts to slip around 500 N, the end-hook acts as a mechanical interlock since it is forced to deform to be able to slip. The load transfer between the fibre and matrix becomes thereby localised at the hook, resulting in high local compressive strains (minimum principal strains) and shear strains at 500 and 600 N. At 435 N, it can be observed that mechanical locking is still active for larger end slip values. This mechanical locking effect is presumed to be active until the fibre hook has deformed plastically and becomes straight and slips in the main vertical canal. The strains that are surrounding the bottom of the fibre canal are thought to be caused by the contraction of the void left by the fibre.
4. Conclusions
Pull-out mechanisms for steel fibers were investigated using adapted pull-out tests performed in-situ in a µXRT. High-resolution volume images from the µXRT scans enable clear visualization of aggregates, pores, the fiber and the fiber-matrix interface. Furthermore, the natural density speckle pattern from aggregate distribution and pores was found suitable for DVC analysis. From the DVC analysis, it was possible to visualize and quantify the strain distribution in the matrix around the fiber at the different load levels up to final failure, which was marked by either pull-out or fiber rupture. The load transfer mechanism was initially dominated by shear along the fiber. As the load increased, slip occurred in the end-hook region and mechanical locking became the governing mechanism. This study demonstrates that strain measurements within the concrete matrix can be obtained successfully using µXRT imaging and DVC analysis, which leads to an increased understanding of the interaction mechanisms between the fiber and the concrete matrix.