How is the Cross Product Between Two Vectors Determined?

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SUMMARY

The cross product between two vectors \(\vec{A}\) and \(\vec{B}\) in \(\mathbb{R}^3\) is defined by the equation \((\vec{A} \times \vec{B}) \times \vec{C} = (\vec{A} \cdot \vec{C}) \vec{B} - (\vec{B} \cdot \vec{C}) \vec{A}\). This proof demonstrates that the resulting vector is a linear combination of \(\vec{A}\) and \(\vec{B}\) and is perpendicular to both \(\vec{A} \times \vec{B}\) and \(\vec{C}\). The scalars \(\lambda\) and \(\mu\) are derived as \(\lambda = -\vec{B} \cdot \vec{C}\) and \(\mu = \vec{A} \cdot \vec{C}\). The discussion emphasizes the importance of understanding the relationships between these vectors and their geometric implications.

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  • Understanding of vector operations in \(\mathbb{R}^3\)
  • Familiarity with the concepts of linear independence and linear combinations
  • Knowledge of the dot product and cross product of vectors
  • Basic algebraic manipulation skills for solving equations
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  • Learn about the properties of linear transformations and their applications in vector spaces
  • Explore advanced vector calculus topics, such as the curl and divergence of vector fields
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This discussion is beneficial for students and professionals in mathematics, physics, and engineering who are looking to deepen their understanding of vector operations and their applications in three-dimensional space.

Mathoholic!
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The cross product between two vectors \vec{A}x\vec{B} and \vec{C} is given by the following equation:
(\vec{A}x\vec{B})x\vec{C}=(\vec{A}.\vec{C})\vec{B}-(\vec{B}.\vec{C})\vec{A}

Well, as I'm sure you know, proving something is true is different than proving how something is true. In this proof, I will not only prove it holds up but I also will demonstrate how it came to be.

What is given is \vec{A},\vec{B} and \vec{C}, which are vectors belonging to ℝ3, or mathematically:
\vec{A},\vec{B},\vec{C}\inℝ3
Let's define the coordinates of \vec{A},\vec{B} and \vec{C} as the following:
\vec{A}=(a1,a2,a3)
\vec{B}=(b1,b2,b3)
\vec{C}=(c1,c2,c3)
Note that by the definition of cross product, \vec{A}x\vec{B} is simultaneously perpendicular to \vec{A} and \vec{B}, or:
(\vec{A}x\vec{B}).\vec{A}=0
(\vec{A}x\vec{B}).\vec{B}=0
Let \vec{A} and \vec{B} be linearly independent, and so they both define a certain plane \Omega. Using the same chain of thought, (\vec{A}x\vec{B})x\vec{C} is simultaneously perpendicular to \vec{A}x\vec{B} and \vec{C}, or:
((\vec{A}x\vec{B})x\vec{C}).(\vec{A}x\vec{B})=0
((\vec{A}x\vec{B})x\vec{C}).\vec{C}=0
Hence, we can conclude that (\vec{A}x\vec{B})x\vec{C} is a linear combination of \vec{A} and \vec{B}, and so:
(\vec{A}x\vec{B})x\vec{C}=λ\vec{A}+μ\vec{B} \in\Omega
We can start by noting the resemblance of this equation with the one given, in which λ is a scalar given by -\vec{B}.\vec{C} and μ by \vec{A}.\vec{C}, as we'll soon show. For the next step, let's write the coordinates of (\vec{A}x\vec{B})x\vec{C} in respect to λ and μ on the LHS/RHS and in respect to the coordinates of \vec{A},\vec{B} and \vec{C} on the RHS/LHS, like so (skipping intermediary steps):
(a1λ+b1μ,a2λ+b2μ,a3λ+b3μ)=(c3(a3b1-a1b3)-c2(a1b2-a2b1),c1(a1b2-a2b1)-c3(a2b3-a3b2),c2(a2b3-a3b2)-c1(a3b1-a1b3))
Now we have three equations with only 2 unknowns (λ,μ), which algebraically means that there's no degree of freedom in the system. These equations may not be easy on the eyes but with strong motivation, they're feesable. And they go as follows (from x and y coordinates):
λ=c3(a3b1/a1-b3)-c2(b2-a2b1/a1)-μ(b1/a1)
\Rightarrow c1(a1b2-a2b1)-c3(a2b3-a3b2)=a2c3(a3b1/a1-b3)-a2c2(b2-a2b1/a1)-μ(a2b1/a1)+μb2\Leftrightarrowμ(b2-a2b1/a1)=-c3(a2a3b1/a1-b3a2+a2b3-a3b2)+a2c2(b2-a2b1/a1)+c1(a1b2-a2b1)\Rightarrowμ=a1c1+a2c2+a3c3=\vec{A}.\vec{C}
Replacing μ in the first line, we get:
λ=c3(a3b1/a1-b3)-c2(b2-a2b1/a1)-(a1c1+a2c2+a3c3)(b1/a1)
Which computed gives:
λ=-(b1c1+b2c2+b3c3)=-\vec{B}.\vec{C}
Note that initially we thought of \vec{A} and \vec{B} as linearly independent but if we hadn't, that would be saying that \vec{A}=κ\vec{B} and such would mean that:
κ(\vec{B}x\vec{B})x\vec{C}=(0,0,0)
And so:
\vec{A}=(μ/λ)\vec{B}
With κ=μ/λ.

If you find any incongruence in this resolution (or any doubt), let me know.
 
Last edited:
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Welcome to PF!

Hi Mathoholic! Welcome to PF! :smile:

Yes, that's fine …

you're saying that it has to be in the plane of A and B,

and (if they're not parallel) that means it has to be a linear combination of A and B.

But it also has to be perpendicular to C, so (aA + bB).C = 0, so a/b = -(B.C)/(A.C).
 


Yes, I understood your simplification. But there's a reason I chose the first equation and not the second one, mainly because the second equation doesn't quite tell you what's λ and μ, it only shows that:
λ/μ=-(\vec{B}.\vec{C})/(\vec{A}.\vec{C})

The factor (-1) could either be from \vec{B}.\vec{C} or \vec{A}.\vec{C} and that's significant to the result. I only assumed that it belong to the plane \Omega because that vector is equipolent. Finally, when you have:

α/β=4

You cannot assume that α is 4 and that β is 1. There's ∞1 possibilities of that ratio happening (degree of freedom: 1). So, in the first case there's a possibility that:

λ=±\vec{A}.\vec{C}±1 \wedge μ=±\vec{B}.\vec{C}±1 (alternately)
 

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