2006 Annual Conference &Amp; Exposition Proceedings
DOI: 10.18260/1-2--378
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Structured Approach In Teaching Intermediate Mechanics Of Materials

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Cited by 3 publications
(8 citation statements)
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“…As visible in Figure 8, all models correctly predict compressive stress at the top glass surface, which becomes tensile by the bottom backsheet surface. Plate theory predictions are exactly linear and symmetric and are defined for the full thickness dimension, with the neutral plane occurring at the geometric center as expected from equation (15). Results are modulus independent since flexural rigidity dropped from equation (15) due to linearity between stress, strain, and deflection.…”
Section: Stress Comparison Across Methodsmentioning
confidence: 84%
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“…As visible in Figure 8, all models correctly predict compressive stress at the top glass surface, which becomes tensile by the bottom backsheet surface. Plate theory predictions are exactly linear and symmetric and are defined for the full thickness dimension, with the neutral plane occurring at the geometric center as expected from equation (15). Results are modulus independent since flexural rigidity dropped from equation (15) due to linearity between stress, strain, and deflection.…”
Section: Stress Comparison Across Methodsmentioning
confidence: 84%
“…Plate theory predictions are exactly linear and symmetric and are defined for the full thickness dimension, with the neutral plane occurring at the geometric center as expected from equation (15). Results are modulus independent since flexural rigidity dropped from equation (15) due to linearity between stress, strain, and deflection. Homogenized finite element models are also largely modulus-independent and linear but show some discretization effects in the region formerly assigned as the module backsheet.…”
Section: Stress Comparison Across Methodsmentioning
confidence: 84%
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“…An exciting approach to understand the mechanism of host–guest interactions in H 2 @C 50 and 2H 2 @C 50 is to calculate their SEs. By definition, the energy stored in a body because of deformation is called the SE . The SEs stored in n H 2 @C 50 ( n = 1 and 2) systems are determined by the overall summation of the SE of the host (C 50 ) and that of the guest ( n H 2 ), as shown in eq …”
Section: Results and Discussionmentioning
confidence: 99%
“…By connecting concepts to their historical evolution and their usage in advanced topics one builds a story of a concept which is important for motivation as well as for retention of the concepts as described in Section 3. Ideas discussed in this paragraph have been elaborated by Vable for the introductory mechanics of materials course 5,6 and for intermediate mechanics of materials course 7,8 .…”
Section: Student Motivationmentioning
confidence: 99%