2017
DOI: 10.1108/rpj-12-2015-0183
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Structure and mechanical behavior of Big Area Additive Manufacturing (BAAM) materials

Abstract: Purpose This paper aims to investigate the deposited structure and mechanical performance of printed materials obtained during initial development of the Big Area Additive Manufacturing (BAAM) system at Oak Ridge National Laboratory. Issues unique to large-scale polymer deposition are identified and presented to reduce the learning curve for the development of similar systems. Design/methodology/approach Although the BAAM’s individual extruded bead is 10-20× larger (∼9 mm) than the typical small-scale system… Show more

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Cited by 283 publications
(186 citation statements)
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“…In mathematical terms, this can be expressed as E 1 = σ 11 /(u 1 /w o ), where E 1 is the bulk, effective, longitudinal Young's modulus, σ 11 is the reaction stress on the left side of the sample, u 1 is the average displacement of the entire left side of the sample in the x 1 direction, and w o is the original x 1 dimension of the sample. Solving this equation yields a Young's modulus at the end of the bead of E 1 = 6.82 GPa for the IRD model with C I = 10 −2 , not too dissimilar from those results provided in Duty et al [3] for a similar system. A similar procedure can be done using the stiffness tensor values at the nozzle exit and this yields a Young's modulus of E 2 = 7.10 GPa at the nozzle exit for the IRD model with C I = 10 −2 .…”
Section: Effective Longitudinal Propertiesmentioning
confidence: 48%
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“…In mathematical terms, this can be expressed as E 1 = σ 11 /(u 1 /w o ), where E 1 is the bulk, effective, longitudinal Young's modulus, σ 11 is the reaction stress on the left side of the sample, u 1 is the average displacement of the entire left side of the sample in the x 1 direction, and w o is the original x 1 dimension of the sample. Solving this equation yields a Young's modulus at the end of the bead of E 1 = 6.82 GPa for the IRD model with C I = 10 −2 , not too dissimilar from those results provided in Duty et al [3] for a similar system. A similar procedure can be done using the stiffness tensor values at the nozzle exit and this yields a Young's modulus of E 2 = 7.10 GPa at the nozzle exit for the IRD model with C I = 10 −2 .…”
Section: Effective Longitudinal Propertiesmentioning
confidence: 48%
“…The Young's modulus, CTE, Poisson's ratio, and density of the carbon fiber were taken to be 230 GPa, −2.6 × 10 −6 (mm/mm)/ • C, 0.2, and 1700 kg/m 3 , respectively. The weight fraction was taken to be 13% to match that of the composite system studied in Duty et al [3] for a carbon fiber reinforced FFF bead with similar bead deposition geometry to that considered here. The shape of the fiber was taken into account using a geometric aspect ratio of 20, within the range of the carbon fiber reinforcement in [3].…”
Section: Flow Modelingmentioning
confidence: 99%
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“…Our material stiffness predictions agree remarkably well with test data appearing in the literature. Duty et al [4] measured the Young's modulus of a 13 per cent carbon fiber reinforced ABS printed bead, reporting a mean value of 7.24 GPa and standard deviation of 0.59 GPa. Our predictions of the elastic modulus for the same material system shown as E 22 in Table 4 are in good agreement with these previously published experimental results.…”
Section: Elastic Properties Across the Exrudatementioning
confidence: 99%
“…To achieve a relatively high dimensional accuracy and superior mechanical performances in large-scale parts, carbon fiber filled polymers are employed. Duty et al show that adding short carbon fibers into the neat Acrylonitrile Butadiene Styrene (ABS) polymer yields a composite with improved elastic properties, especially along the printing direction, and less distortion in the printed part following the bead deposition process of the BAAM system [3,4].…”
Section: Introductionmentioning
confidence: 99%