By Cees Oomens, Marcel Brekelmans, Frank Baaijens

This can be the 1st textbook that integrates either normal and particular subject matters, theoretical history and biomedical engineering functions, in addition to analytical and numerical ways. This quantitative technique integrates the classical thoughts of mechanics and computational modelling options, in a logical development via a variety of basic biomechanics rules. on-line MATLAB-based software program in addition to examples and difficulties utilizing biomedical functions will inspire undergraduate biomedical engineering scholars to perform and try their abilities. The e-book covers themes comparable to kinematics, equilibrium, stresses and lines, and likewise makes a speciality of huge deformations and rotations and non-linear constitutive equations, together with visco-elastic behaviour and the behaviour of lengthy slim fibre-like constructions. this can be the definitive textbook for college students.

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**Extra resources for Biomechanics: Concepts and Computation**

**Sample text**

At each of the attachment points, A and B, reaction forces have been introduced on both the body and the support. 3): action = − reaction, forces are defined in the opposite direction with respect to each other, but have equal magnitude. The (three) reaction forces at point A and point B are, for the time being, unknown. They can be calculated by enforcing force and moment equilibrium of the body. Hence, both the sum of all forces in the horizontal direction as well as the sum of all the forces in the vertical direction acting on the body have to be equal to zero.

Only if the number of unknown reaction loads equals three is the solution of the unknowns possible. Likewise, in the threedimensional case, imposing force and moment equilibrium generates six independent equations, such that six unknown reactions can be computed. If a free body diagram is drawn and all the reactions can be directly identified from enforcing the equilibrium conditions, this is referred to as the statically determinate case. If the reactions defined on a free body diagram cannot be calculated by imposing the equilibrium conditions, then this is referred to as the statically indeterminate case.

47) The magnitude |F| of the force vector is obtained from |F| = F·F. 49) or, equivalently |F| = TF . 11 The force vector F resulting from the two force vectors P and Q. Suppose that two thin wires are connected to a point. The first wire is loaded with force P and on the second wire a force Q is applied. The total force vector F exerted on the point is calculated from F =P+Q. 51) See Fig. 11 for a visualization. 53) F = ( Px + Qx ) ex + ( Py + Qy ) ey + ( Pz + Qz ) ez . 54) such that The magnitude of the resulting force vector is given by |F| = ( Px + Qx )2 +( Py + Qy )2 +( Pz + Qz )2 .