Problem 46
Question
Derivatives of triple scalar products a. Show that if \(\mathbf{u}, \mathbf{v},\) and \(\mathbf{w}\) are differentiable vector functor functons of \(t,\) then $$ \begin{array}{r}{\frac{d}{d t}(\mathbf{u} \cdot \mathbf{v} \times \mathbf{w})=\frac{d \mathbf{u}}{d t} \cdot \mathbf{v} \times \mathbf{w}+\mathbf{u} \cdot \frac{d \mathbf{v}}{d t} \times \mathbf{w}+} \\\ {\mathbf{u} \cdot \mathbf{v} \times \frac{d \mathbf{w}}{d t}}\end{array} $$ b. Show that Equation \((7)\) is equivalent to $$ \frac{d}{d t}\left|\begin{array}{ccc}{u_{1}} & {u_{2}} & {u_{3}} \\ {v_{1}} & {v_{2}} & {v_{3}} \\ {w_{1}} & {w_{2}} & {w_{3}}\end{array}\right|=\left|\begin{array}{ccc}{\frac{d u_{1}}{d t}} & {\frac{d u_{2}}{d t}} & {\frac{d u_{3}}{d t}} \\ {v_{1}} & {v_{2}} & {v_{3}} \\\ {w_{1}} & {w_{2}} & {w_{3}}\end{array}\right| $$ $$ +\left|\begin{array}{lll}{u_{1}} & {u_{2}} & {u_{3}} \\ {\frac{d v_{1}}{d t}} & {\frac{d v_{2}}{d t}} & {\frac{d v_{3}}{d t}} \\ {w_{1}} & {w_{2}} & {w_{3}}\end{array}\right| $$ $$ +\left|\begin{array}{lll}{u_{1}} & {u_{2}} & {u_{3}} \\ {v_{1}} & {v_{2}} & {v_{3}} \\ {\frac{d w_{1}}{d t}} & {\frac{d w_{2}}{d t}} & {\frac{d w_{3}}{d t}}\end{array}\right| $$
Step-by-Step Solution
VerifiedKey Concepts
Derivative
When dealing with the triple scalar product, which involves a dot product (\(\cdot\)) and a cross product (\(\times\)), we need to use the modified product rule. It states the derivative of a combined product breaks into parts: one part focuses on differential of one vector while holding others constant.
In mathematical terms, the derivative (\(\frac{d}{dt}(\mathbf{u} \cdot (\mathbf{v} \times \mathbf{w})) \)) becomes the sum of three terms: (\(\frac{d\mathbf{u}}{dt} \cdot (\mathbf{v} \times \mathbf{w})\)), (\(\mathbf{u} \cdot (\frac{d\mathbf{v}}{dt} \times \mathbf{w})\)), and (\(\mathbf{u} \cdot (\mathbf{v} \times \frac{d\mathbf{w}}{dt})\)). This method allows for precise change tracking in multidimensional contexts.
Triple Scalar Product
Think of (\(\mathbf{v} \times \mathbf{w}\)) as generating a vector orthogonal to the plane containing (\(\mathbf{v}\)) and (\(\mathbf{w}\)). When dot-multiplied by (\(\mathbf{u}\)), the triple scalar product assesses how (\(\mathbf{u}\)) aligns with this perpendicular direction. This alignment provides a measure of the three-dimensional spanned space.
Mathematically, the expression is represented as: (\( \mathbf{u} \cdot (\mathbf{v} \times \mathbf{w}) \)) and it's both useful and insightful in physics and engineering, especially in contexts dealing with torque and rotational motion.
Cross Product
To understand, consider vectors (\(\mathbf{v}\)) and (\(\mathbf{w}\)). Their cross product, (\(\mathbf{v} \times \mathbf{w}\)), creates a vector orthogonal to the plane formed by (\(\mathbf{v}\)) and (\(\mathbf{w}\)). The direction follows the right-hand rule.
The magnitude equals the area of the parallelogram formed by (\(\mathbf{v}\)) and (\(\mathbf{w}\)). This operation is crucial in determining torque, where force impacts rotational motion around an axis.
Mathematically, the cross product is defined for vectors (\(\mathbf{v} = (v_1, v_2, v_3)\)) and (\(\mathbf{w} = (w_1, w_2, w_3)\)) as: \[ \mathbf{v} \times \mathbf{w} = (v_2w_3 - v_3w_2, v_3w_1 - v_1w_3, v_1w_2 - v_2w_1) \].
Determinants
For a triple scalar product, a determinant represents the scalar outcome of vectors (\(\mathbf{u}, \mathbf{v}, \mathbf{w}\)). Arranged in a matrix, their determinant equals the volume of a parallelepiped they form.
In the context of the exercise, visualizing the triple scalar product as a determinant aids in understanding its derivative. Each row shift corresponds to a differentiated vector, leading to efficient differentiation.
The basic property is: If (\(\mathbf{M}\)) is the matrix, its determinant (\(|\mathbf{M}|\)) is: \[ \left| \begin{array}{ccc} a & b & c \ d & e & f \ g & h & i \end{array} \right| = a(ei-fh) - b(di-fg) + c(dh-eg) \].
This structural understanding is intuitive in areas such as physics and engineering, assisting in streamlined solutions of vector problems.