Does Changing Vector Components Affect Parallelepiped Volume?

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SUMMARY

The volume of a parallelepiped defined by vectors w, u, and v, where w = u × v, is calculated using the formula V = w · (u × v). Changing the definition to w - u, u, and v does not alter the volume, as demonstrated by the equation (w - u) · (u × v) = w · (u × v) - u · (u × v). The term u · (u × v) equals zero, confirming that the volume remains unchanged. This property can be geometrically interpreted through determinants and vector products, as detailed in the discussion.

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  • Knowledge of the properties of coplanar vectors and their implications on volume calculations.
  • Basic proficiency in linear algebra concepts related to vector spaces.
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Rotnort
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Homework Statement


The volume of a parallelepiped defined by the vectors w, u, \text{ and }v, \text{ where } w=u \times v is computed using:
V = w \cdot (u \times v)

However, if the parallelepiped is defined by the vectors w-u, u, \text{ and }v, \text{ where } w=u \times v instead, the volume remains the same. Why? Can this be proven mathematically?

The Attempt at a Solution


I can visualise the subtraction of the vector v as not modifying the magnitude of the length of the cross product, rather the horizontal span of the parallelepiped itself. However, I don't know how to prove this without numerical computation.
 
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Rotnort said:

Homework Statement


The volume of a parallelepiped defined by the vectors w, u, \text{ and }v, \text{ where } w=u \times v is computed using:
V = w \cdot (u \times v)

However, if the parallelepiped is defined by the vectors w-u, u, \text{ and }v, \text{ where } w=u \times v instead, the volume remains the same. Why? Can this be proven mathematically?

The Attempt at a Solution


I can visualise the subtraction of the vector v as not modifying the magnitude of the length of the cross product, rather the horizontal span of the parallelepiped itself. However, I don't know how to prove this without numerical computation.
$$ \mathbf{(w-u) \cdot (u \times v)} = \mathbf{w \cdot (u \times v)} - \mathbf{ u \cdot (u \times v)}$$
What is ##\mathbf{u\cdot (u \times v)} ?##
 
Ray Vickson said:
$$ \mathbf{(w-u) \cdot (u \times v)} = \mathbf{w \cdot (u \times v)} - \mathbf{ u \cdot (u \times v)}$$
What is ##\mathbf{u\cdot (u \times v)} ?##
I see, very simple. Aside, is my geometrical justification valid?
 
Rotnort said:
I see, very simple. Aside, is my geometrical justification valid?
I don't know: I did not understand what you were saying or what you were trying to do.
 
Ray Vickson said:
I don't know: I did not understand what you were saying or what you were trying to do.
Ok. I am curious: how would you describe this property geometrically?
 
One way to look at it is ##\mathbf{w}\cdot(\mathbf{u}\times \mathbf{v})= \det(\mathbf{w},\mathbf{u},\mathbf{v})=\operatorname{Vol}(\mathbf{w},\mathbf{u},\mathbf{v})##.
Now your equation becomes ##\det(\mathbf{w},\mathbf{u},\mathbf{v}) = \det(\mathbf{w-u},\mathbf{u},\mathbf{v})## which is a simple column vector manipulation that doesn't change the linear equation system, esp. the determinant. Some insights on the various vector products can also be found here: https://arxiv.org/pdf/1205.5935.pdf

Unfortunately, the English Wikipedia entry https://en.wikipedia.org/wiki/Triple_product#Geometric_interpretation is a bit short on the geometric interpretation. The Spanish and German versions are better, if you like to switch languages and see if you can understand them. They basically derive the formula of the Volume by
$$
\operatorname{Vol}(\mathbf{u},\mathbf{v},\mathbf{w}) = \operatorname{A}(\mathbf{u},\mathbf{v}) \cdot h_\mathbf{w} = \operatorname{A}(\mathbf{u},\mathbf{v}) \cdot |\mathbf{w}| \cdot \cos(\sphericalangle(\mathbf{u} \times \mathbf{v}), \mathbf{w}) = |\mathbf{u} \times \mathbf{v}| \cdot \mathfrak{n}_{\mathbf{u} \times \mathbf{v}}\cdot \mathbf{w} = |(\mathbf{u} \times \mathbf{v})\cdot \mathbf{w}|
$$
which is the geometric description.

If the vectors ##\{\mathbf{u},\mathbf{v},\mathbf{w}=\mathbf{u}\}## are coplanar, then ##\sphericalangle((\mathbf{u} \times \mathbf{v}),\mathbf{u}) = \frac{\pi}{2}##, because ##\mathbf{u} \times \mathbf{v}## is perpendicular to ##\mathbf{u}## and consequently ##\operatorname{Vol}(\mathbf{u},\mathbf{v},\mathbf{u}) = 0##.
 

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