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Engineering Mechanics: Dynamics

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Vyd. 1. Na obálce nad názvem: Univerzita obrany, Fakulta vojenských technologií Na obálce označení: S-2703/2 50 výt.

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... A fully elastic impact is defined as the impact in which both kinetic energy and momentum are conserved. In reality, all collisions are inelastic because permanent deformation on the microscopic scale will happen [61], but this solution will provide a bound on the actual behavior. The two beams will not remain in contact after impact and they will behave independently. ...
... Impact of a failed member in a precast concrete structure According to Boresi and Schmidt[61], a collision, or impact between two bodies is defined as "a strong interaction between the bodies, either by direct contact or by the nature of their proximity, that lasts a relatively short time". In general, when two bodies collide many questions arise such as: For given velocities of two bodies before they collide, what are their velocities after the collision? ...
... How much damage occurs in the collision? How far do the two bodies travel after they collide?[61]. In general, collisions between two bodies result in a loss of some kinetic energy and in this case the collision is called an inelastic collision. ...
Thesis
Presented in this work are the possible collapse mechanisms initiated by a precast flexural member dropping on a lower member. The ultimate goal of this research is to develop design guidelines and advice to prevent progressive collapse in such cases. The problem is complicated due to the dynamic analyses involved in the dropping, the impact, and the resulting vibration. Analytical solutions and numerical solutions were developed to solve three possible collapse scenarios: perfectly plastic, inelastic, and elastic. These impact scenarios should provide a reasonable understanding of the dynamic behaviour for the member after impact. The analytical solution involves using Fourier series and the numerical solution involves a developed method of converting an initial velocity profile to an impulse load using SAP2000. The members are from typical parking garages. The first solutions developed were for the perfectly plastic and elastic impact scenarios based on assumed initial velocity profiles. The resulting reactions from the impact were evaluated against ACI provisions. It has been found that a shear failure can be prevented by providing some shear reinforcement. However, the resulting bending moment is high and the member is prone to fail under flexure. The second solutions developed were for perfectly plastic impact based on the pre-impact velocity profile of the top beam. The post-impact velocity profiles were not assumed. SAP2000 was used to calculate the post-impact velocity profiles for the upper and lower beams. The resulting shear and bending moment for the perfectly plastic scenario were extremely high and caused the member to fail. However, the resulting shear and bending moment for the case of inelastic impact did not cause failure. Finally, a simulation of the impact using the finite element analysis COMSOL Multiphysics program was performed. When simulating impact, the COMSOL documents caution the user to check conservation of momentum and energy to ensure that the results are reasonable. Conservation of momentum has been checked and found not to be satisfied. Therefore, COMSOL Multiphysics is not recommended for this type of analysis.
... The dynamic rollover metrics are based on the Newton's second law of motion, and these include, for instance, the Dynamic Stability Index (DSI) [7]. Examples of energybased metrics include the Critical Sliding Velocity (CSV) [8], [9], [10], [5], which is a minimum lateral velocity required to tip a vehicle over when the vehicle is sliding laterally and hitting a curb, and the Rollover Prevention Energy Reserve (RPER) [7], which is defined as the difference between the potential energy required to bring a vehicle to its tipover position and the sum of the instantaneous linear and rotational kinetic energy. One issue with the previous metrics is that they do not provide a situation-dependent warning. ...
... Considering a kinematic chain in Fig. 1 and using general equations of motion [28], [29], [26] and D'Alembert's principle [10], the moment equation about point A in Fig. 1 induced by inertial forces and gravity is: ...
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Rollover accidents are one of the leading causes of death in highway accidents due to their very high fatality rate. A key challenge in preventing rollover via chassis control is that the prediction of the onset of rollover can be quite difficult, especially in the presence of terrain features typical of roadway environments. These road features include superelevation of the road (e.g road bank), the median slope, and the shoulder down-slope. This work develops a vehicle rollover prediction algorithm that is based on a kinematic analysis of vehicle motion, a method that allows explicit inclusion of terrain effects. The solution approach utilizes the concept of zero-moment point (ZMP) that is typically applied to walking robot dynamics. This concept is introduced in terms of a lower-order model of vehicle roll dynamics to measure the vehicle rollover propensity, and the resulting ZMP prediction allows a direct measure of a vehicle rollover threat index. Simulation results using a complex multi-body vehicle simulation show the effectiveness of the proposed algorithm during different road geometry scenarios and driver excitations.
... In this case, a portion of the tool swept volume penetrates itself so that it becomes difficult to get a topologically consistent SV without extra geometrical treatment, which leads to a higher time complexity. Due to the geometric and computational complexity the theme 1 Any point on a rigid body or on its extension that has zero velocity is called the instantaneous center of velocity or instantaneous axis of rotation (IAR) of the body [11]. ''self-penetration (SP) or self-intersection (SI) in SV generation'' has been neglected, skipped or reported very restrictively in most scientific research [2][3][4][5][6][7]. ...
... Peternell et al. [20] generate SV from a solid Φ with a piecewise smooth boundary by eliminating local self-intersection. Using the tangency condition f (=v(X) · n(X) = 0, X ∈ ∂Φ(t)) [11], grazing points plus surface normals are gathered into a set Q at each adaptive time interval which is determined by considering the evolution speed of the trajectory. Then with a marching cube (MC) algorithm the points which lie on the boundary of the SV are extracted. ...
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In this paper the swept volume with self-penetration (or self-intersection) of the cutter is presented. The complete swept volume (SV), which describes the side and bottom shape of a milling cutter undergoing self-penetration, is generated by using the Gauss map method proposed in the authors’ previous paper [Lee SW, Nestler A. Complete swept volume generation—part I: swept volume of a piecewise C1-continuous cutter at five-axis milling via Gauss map. Computer-Aided Design 2011; 43(4): 427–41]. Based on the Gauss map method, the comprehensive analysis of envelope profiles of the tool is accomplished. Through the analysis the necessary condition of the self-penetration of the cutter at five-axis movement is identified. After having classified movement types of the milling cutter in an in-depth manner, the topologically consistent boundary of SV is generated by trimming the invalid facets interior to the SV. To demonstrate the validity of the proposed method, a cutting simulation kernel for five-axis machining has been implemented and applied to cavity machining examples such as intake ports of automobile engines and so forth where the self-penetration occurs. The proposed method is proved to be robust and amenable for the practical purpose of the NC simulation.
... In a second dynamics textbook, [2], the chapters are as follows: The above-mentioned three textbooks cases establish the consistency of the current organization of topics. This is based on deriving equations for a single particle then extending the derivations to a system of particles and in the second half of the course applying the system of particle equations to rigid bodies. ...
... We developed an "Influence Factor" to measure the difference in student performance between students taught by the first author ("Author") and students taught by another instructor ("Other") [2,3]. The rationale for distinguishing student performance on this basis is that, because the targeted issues are central and highly emphasized in courses taught by the Author, performance of the Author's students is possibly correlated with the effectiveness of the targeted methods. ...
... The vast majority of dynamics textbooks (Hibbeler (2016), Boresi and Schmidt (2000), Beer and Johnston (2015), Meriam and Kraige (2015), Shames (1996), Bedford and Fowler (2007), Soutas-Little and Inman (1999), Tongue (2009), and Gray, Costanso, and Plesha (2012)) are organized with an almost identical ordering of topics [1]- [9]. This ordering is generally particle kinematics, particle kinetics, rigid body kinematics, rigid body kinetics, 3-D kinematics and kinetics, and finally vibrations. ...
... Determine the speed V G of it's mass center G so that it rolls without slipping completely around the loop of radius R + r without leaving the track. I G = (2/5)mr 2 . Express your answer in terms of radius R and the acceleration of gravity g. ...
... Imani, and Braga-Neto [7] gave an estimation of state and parameters of Partially Observed Boolean Dynamical Systems. We have taken the help from other references including [8][9][10][11][12][13][14][15][16][17][18] in the field of friction and lifting machine to complete the work. The bell crank lever is an apparatus shown in Figure-1 which is used to verify the law of moments. ...
... The second relevant impact equation is obtained from the coefficient of restitution [26] ...
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We consider a two-degree-of-freedom model where the focus is on analyzing the vibrations of a fixed but flexible structure that is struck repeatedly by a second object. The repetitive impacts due to the second mass are driven by a flowing fluid. Morison’s equation is used to model the effect of the fluid on the properties of the structure. The model is developed based on both linearized and quadratic fluid drag forces, both of which are analyzed analytically and simulated numerically. Conservation of linear momentum and the coefficient of restitution are used to characterize the nature of the impacts between the two masses. A resonance condition of the model is analyzed with a Fourier transform. This model is proposed to explain the nature of ice-induced vibrations, without the need for a model of the ice-failure mechanism. The predictions of the model are compared to ice-induced vibrations data that are available in the open literature and found to be in good agreement. Therefore, the use of a repetitive impact model that does not require modeling the ice-failure mechanism can be used to explain some of the observed behavior of ice-induced vibrations.
... The a max –l curve in expected, a max decreases monotonically as l increases. The smallest possible a max as l approaches infinity (a cable) can be found to be 0.37 through a simple statics analysis (Boresi and Schmidt, 2000). On the other hand, as l approaches 0, a max approaches 1. ...
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... Dynamics involves the analysis of time-dependent motion, and represents textbook knowledge in most physical science and engineering curricula (e.g., see Sandor, 1983). One area of Dynamics called Kinematics offers potential to inform dynamic organizational performance, fit and change. ...
... During the pre-collision phase, vehicle speed, V t , decreases due to sliding friction force applied on tires (Hibbeler, 1986). ...
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The study aims at developing analysis approaches of vehicle-accident reconstruction in an attempt to recreate the initial impact configuration and clarify accident responsibility. One purpose is to conclude a straightforward and confident recon- struction module as a base of dealing with vehicle impact accidents. Both forward and backward deriving methods have been applied as the means of accident reconstruction. The initial impact configuration can be resulted from dynamic equations of pre-impact, impact and post-impact phases. The obtained formulated relations have been further schemed to be an interactive human-machine environment. The initial impact configuration can thus be yielded, as some necessary data are input to the developed program.
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... The sum of the kinetic energy K and potential energy P of an upright pendulum, as shown in Fig. 1, consisting of a slender bar with mass m and length l is [18] ...
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... In this work, they adopt the method of moving frame introduced by [13], as well as the method of explicit closed-form representation, introduced by [17], to formulate envelope profile for five-axis tool motions. The partial extension is dedicated to solution analysis and special case analysis of generalized cutters for five-axis tool motions by using rigid body motion theory [24] and envelope theory [25]. SV is modeled in the framework of an open source [26]. ...
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... This can be found in basic textbooks on dynamics and fluid mechanics. Examples: Section 17.10 in Engineering Mechanics: Dynamics by Boresi and Schmidt [10], Section 5.6 in Mechanics of Fluids by Shames [11], Section 3.2 in An Introduction to Fluid Dynamics by Batchelor [12], and Section 3.2 in Mechanics of Fluids by Potter and Wiggert [13]. ...
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... This experiment focuses on one type of collision which can be modeled classically as a direct, central impact of particles. The theory of direct, central impact of particles ± which follows from Newton's laws of motion ± can be found in numerous textbooks (e.g., [2] [3]) that present the fundamentals of dynamics. More advanced treatments of planar and three-dimensional impact for both particles and rigid bodies are developed in specialized textbooks (e.g., [4±6]). ...
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