5.2 “Mathematical tools” in biomechanics

5.2.1 Vectors and scalars


5.2.1.1 Vectors

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  • Vectors are quantities that have an associated magnitude and direction.\(^{**}\)

  • Vector have components

    • \(\vec{F}_x = {F}_x i\)
    • \(\vec{F}_y = {F}_y j\)
    • \(\vec{F} = \vec{F}_x + \vec{F}_y = {F}_x i +{F}_y j\)
  • Examples of vectors

    • Forces (Weight)
    • Moments (Torques)
    • Velocities

5.2.1.2 Vector sums

  • Vector addition is component by component
  • Proper (2D) summation results in a parallelogram

5.2.1.3 Scalars

  • Scalars have magnitude without direction.
  • Examples
    • Levels of gray in a image
    • Patient mass
    • Patient bone density
    • Concentration of a drug per unit volume
    • Time
    • Altitude

5.2.2 Relationship between vectors and scalars

  • Scalars and vectors can be linked mathematically

Gradients Charles J Sharp, March 2001

Example: diffusion of nutrients into intervertebral disk driven by gradient of glucose


5.2.2.1 Gradient of a scalar

\[\nabla f = \left(\frac{\partial f}{\partial x_1 }, \dots, \frac{\partial f}{\partial x_n } \right).\]

Gradient of a vector becomes a 2nd rank tensor \[\mathbf{f}=({{f}_{1}},{{f}_{2}},{{f}_{3}})\] \[\nabla \mathbf{f}=\frac{\partial {{f}_{j}}}{\partial {{x}_{i}}}{{\mathbf{e}}_{i}}{{\mathbf{e}}_{j}}\]


Example: strain is gradient of displacement vector

  • \[\vec{u} = u {{e_x}}+ v {{e_y}}+ w {{e_z}}\]
  • \[= {\varepsilon_{ij}}= \nabla \vec{u} = \left[ \begin{array}{ccc} {\varepsilon_{xx}}& {\varepsilon_{xy}}& {\varepsilon_{xz}}\\ {\varepsilon_{yx}}& {\varepsilon_{yy}}& {\varepsilon_{yz}}\\ {\varepsilon_{zx}}& {\varepsilon_{yz}}& {\varepsilon_{zz}}\\ \end{array} \right]\]

5.2.2.2 Divergence

  • Similarly, the divergence operator (\(\nabla \cdot ()\)) reduces the
    rank of a tensor

    • i.e., makes a scalar out of a vector
  • Example: the divergence calculates the strength
    of a source or sink of a velocity field in fluid flow


5.2.3 Rigid body and flexible body assumptions

  • All bodies are flexible, meaning, all bodies deform when loaded
  • For convenience, we often assume that a body is rigid
    • (ie we assume that it does not deform when loaded.)
  • With this assumption, the mechanics/mathematics is simplified