Vector equations, possible to solve for x?

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The discussion revolves around solving vector equations, specifically how to isolate vectors like ##\vec{\omega}## in equations involving cross and dot products. It is noted that while solving the equation ##\vec{v} = \vec{\omega} \times \vec{r}## can yield multiple solutions due to the nature of vector operations, the approach of multiplying both sides by ##\vec{r}## is not reversible, leading to potential circular reasoning. The conversation highlights that for dot products, there are infinitely many solutions, as any vector perpendicular to another can be added to a solution without changing the outcome. The participants express a desire to understand the underlying principles of vector algebra better, questioning the validity of their methods and whether these concepts apply to complex vectors. The discussion emphasizes the complexities and nuances involved in solving vector equations.
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Hello there,

In scalar algebra, I find solving for variables a useful tool. Say ohms law, I want to find ##R## so:

$$
U=RI \iff R = \frac{U}{I}
$$

Can I do something analogous in vector equations? I.e. May I solve for ##\vec{\omega}## in equations using cross or dot products?

$$
\vec{v} = \vec{\omega} \times \vec{r} \iff \vec{\omega} = ?
$$

or:

$$
\vec{\alpha} \cdot \vec{\beta} = \gamma \iff \vec{\beta} = ?
$$


It would be fantastic if I could solve for vectors in some way.

Hope you are able to help.

Thank you for your time!

Kind regards,
Marius
 
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Solving v=wxr makes sense, since this can be seen as solving 3 equations with 3 unknowns (each components).
You can find the solution easily by "multiplying" both sides by r: rxv = rx(wxr) = w (r.r) - r (w.r) .

Solving a.b=c makes less sense, since this can be seen as solving 1 equation with three unknowns.
Actually there is an infinite number of solutions to this equation.
If you have one solution b=bo, then you can add any vector b1 such that a.b1=0 to this solution, and you will get another solution b = bo+b1. Any b1 just need to be perpendicular to a.
 
maajdl said:
Solving v=wxr makes sense, since this can be seen as solving 3 equations with 3 unknowns (each components).
What exactly do you mean by three equations?
 
With V=W X R you end up with three equations corresponding to the three components of V.
With v=W o R you end up with one equation because v is a scalar, and three unknowns for W.
 
maajdl said:
Solving v=wxr makes sense, since this can be seen as solving 3 equations with 3 unknowns (each components).
You can find the solution easily by "multiplying" both sides by r: rxv = rx(wxr) = w (r.r) - r (w.r) .
That's one solution. There are infinitely many others.

Given any solution w for v = w cross r and any scalar k then w + kr is another solution.
 
I want to learn about this topic in vector algebra.

1. What is the topic called?

2. Is this correct? And how then do I solve for ##\vec{\omega}##?

$$
\vec{v} = \vec{\omega} \times \vec{r} \iff \vec{r} \times \vec{v} = \vec{r} \times (\vec{\omega} \times \vec{r}) = \vec{\omega} (\vec{r}^2) - \vec{r}(\vec{r} \cdot \vec{\omega})
$$
Now what?

3. Does it hold for compex vectors?

Thanks.M
 
Jonsson said:
I want to learn about this topic in vector algebra.

1. What is the topic called?

2. Is this correct? And how then do I solve for ##\vec{\omega}##?

$$
\vec{v} = \vec{\omega} \times \vec{r} \iff \vec{r} \times \vec{v} = \vec{r} \times (\vec{\omega} \times \vec{r}) = \vec{\omega} (\vec{r}^2) - \vec{r}(\vec{r} \cdot \vec{\omega})
$$
Now what?

3. Does it hold for compex vectors?

Thanks.M

You have a linear equation for the components of w there.
 
Jonsson said:
2. Is this correct? And how then do I solve for ##\vec{\omega}##?

$$
\vec{v} = \vec{\omega} \times \vec{r} \iff \vec{r} \times \vec{v} = \vec{r} \times (\vec{\omega} \times \vec{r}) = \vec{\omega} (\vec{r}^2) - \vec{r}(\vec{r} \cdot \vec{\omega})
$$

The above is false. The implication is unidirectional, not bidirectional. The operation of multiplying both sides by r is not reversible.

The reason it's not reversible is that you can't uniquely divide by r. Since the purpose of the exercise was to demonstrate that you can uniquely divide by r, asserting that you can divide by r would amount to a circular argument.
 
And, you have the difficulty that the solutions will seldom be unique. As obvious example if \vec{a}\times\vec{x}= \vec{0} or \vec{a}\cdot\vec{x}= 0, \vec{x} can be any vector perpendicular to \vec{a}
 
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