Classical Dynamics of Particles and Systems · Problem 1-11

Newtonian Mechanics—Single Particle — Marion & Thornton

Physics — Mechanics · triple-scalar-product

Problem

Show that the triple scalar product (A×B)⋅C(\mathbf{A} \times \mathbf{B}) \cdot \mathbf{C} can be written as (A×B)⋅C=∣A1A2A3B1B2B3C1C2C3∣(\mathbf{A} \times \mathbf{B}) \cdot \mathbf{C} = \begin{vmatrix} A_1 & A_2 & A_3 \\ B_1 & B_2 & B_3 \\ C_1 & C_2 & C_3 \end{vmatrix} Show also that the product is unaffected by an interchange of the scalar and vector product operations or by a change in the order of A\mathbf{A}, B\mathbf{B}, C\mathbf{C}, as long as they are in cyclic order; that is, (A×B)⋅C=A⋅(B×C)=B⋅(C×A)=(C×A)⋅B,etc.(\mathbf{A} \times \mathbf{B}) \cdot \mathbf{C} = \mathbf{A} \cdot (\mathbf{B} \times \mathbf{C}) = \mathbf{B} \cdot (\mathbf{C} \times \mathbf{A}) = (\mathbf{C} \times \mathbf{A}) \cdot \mathbf{B}, \quad \text{etc.} We may therefore use the notation ABC\mathbf{ABC} to denote the triple scalar product. Finally, give a geometric interpretation of ABC\mathbf{ABC} by computing the volume of the parallelepiped defined by the three vectors A\mathbf{A}, B\mathbf{B}, C\mathbf{C}.

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