6,565 research outputs found

    Experimental tests on slip factor in friction joints: Comparison between european and American standards

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    Friction joints are used in steel structures submitted to cyclic loading such as, for example, in steel and composite bridges, in overhead cranes, and in equipment subjected to fatigue. Slip-critical steel joints with preloaded bolts are characterized by high rigidity and good performance against fatigue and vibrational phenomena. The most important parameter for the calculation of the bolt number in a friction connection is the slip factor, depending on the treatment of the plane surfaces inside the joint package. The paper focuses on the slip factor values reported in European and North American Specifications, and in literature references. The differences in experimental methods of slip test and evaluation of them for the mentioned standards are discussed. The results from laboratory tests regarding the assessment of the slip factor related to only sandblasted and sandblasted and coated surfaces are reported. Experimental data are compared with other results from the literature review to find the most influent parameters that control the slip factor in friction joint and differences between the slip tests procedure

    Design and analysis of bent functions using M\mathcal{M}-subspaces

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    In this article, we provide the first systematic analysis of bent functions ff on F2n\mathbb{F}_2^{n} in the Maiorana-McFarland class MM\mathcal{MM} regarding the origin and cardinality of their M\mathcal{M}-subspaces, i.e., vector subspaces on which the second-order derivatives of ff vanish. By imposing restrictions on permutations π\pi of F2n/2\mathbb{F}_2^{n/2}, we specify the conditions, such that Maiorana-McFarland bent functions f(x,y)=x⋅π(y)+h(y)f(x,y)=x\cdot \pi(y) + h(y) admit a unique M\mathcal{M}-subspace of dimension n/2n/2. On the other hand, we show that permutations π\pi with linear structures give rise to Maiorana-McFarland bent functions that do not have this property. In this way, we contribute to the classification of Maiorana-McFarland bent functions, since the number of M\mathcal{M}-subspaces is invariant under equivalence. Additionally, we give several generic methods of specifying permutations π\pi so that f∈MMf\in\mathcal{MM} admits a unique M\mathcal{M}-subspace. Most notably, using the knowledge about M\mathcal{M}-subspaces, we show that using the bent 4-concatenation of four suitably chosen Maiorana-McFarland bent functions, one can in a generic manner generate bent functions on F2n\mathbb{F}_2^{n} outside the completed Maiorana-McFarland class MM#\mathcal{MM}^\# for any even n≥8n\geq 8. Remarkably, with our construction methods it is possible to obtain inequivalent bent functions on F28\mathbb{F}_2^8 not stemming from two primary classes, the partial spread class PS\mathcal{PS} and MM\mathcal{MM}. In this way, we contribute to a better understanding of the origin of bent functions in eight variables, since only a small fraction, of which size is about 2762^{76}, stems from PS\mathcal{PS} and MM\mathcal{MM}, whereas the total number of bent functions on F28\mathbb{F}_2^8 is approximately 21062^{106}
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