Biomedical Engineering Reference
In-Depth Information
In ordinary vector differentiation, we meet the gradient of a scalar field f , defined in
Cartesian coordinates as
f
z e z
where e x , e y and e z areCartesian unit vectors.When dealingwith functions ofmany variables
it proves useful to make a generalization and write the gradient of (for example) U as
f
x e x +
f
y e y +
grad f
=
U
q 1
U
q 2
.
U
q p
grad U
=
(4.6)
so grad U is a column matrix that stores all the partial derivatives. This 'vector' will occur
many times through the text, and I am going to give it the symbol g (for gradient).
The second derivatives can be collected into a symmetric p
p matrix that is called the
Hessian of U and I will give this the symbol H . In the case where p
×
=
3, we have
2 U
q 1
2 U
q 1 q 2
2 U
q 1 q 3
2 U
q 2 q 1
2 U
q 2
2 U
q 2 q 3
H
=
(4.7)
2 U
q 3 q 1
2 U
q 3 q 2
2 U
q 3
The Taylor expansion then becomes
1
2 ξ T H ξ
ξ T g
U ( q )
U ( q e )
=
+
+···
(4.8)
Both the gradient and the Hessian have to be evaluated at the point q e , and so you will
sometimes see the equation written with an 'e' subscript:
1
2 ξ T H e ξ
ξ T g e +
U ( q )
U ( q e )
=
+···
The superscript T as in ξ T indicates the transpose of a matrix; the transpose of a column
matrix is a row matrix. The Hessian is often referred to as the force constant matrix.
Finally, if I denote the 3 N Cartesian coordinates X 1 , X 2 , ..., X 3 N , we usually write the
transformation from Cartesian coordinates to internal coordinates as
=
q
BX
(4.9)
where the rectangular matrix B is called the Wilson B-matrix. The B matrix has p rows and
3 N columns.
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