How does the reflection formula for vectors work?

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The reflection formula for vectors, R_a v = v - 2a(va)/(aa), describes how a vector v is reflected across an axis orthogonal to another vector a. The derivation involves decomposing v into components parallel and perpendicular to a, using the dot product to find the projection of v onto a. The perpendicular component remains unchanged during reflection, while the parallel component is reversed, leading to the final formula. The discussion also highlights the geometric interpretation of reflection using triangles and the relationship between angles and magnitudes. Understanding the signs in the formula is crucial for determining the direction of the reflected vector.
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Could someone explain how the reflection formula comes about?

R_a v = v - 2a(va)/ (aa) , where v and a are vectors and v is relected along the axis orthogonal to a

thanks
 
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I presume that by "va" and "aa" you mean the dot product.

Decompose \vec{v} into components parallel to and orthogonal to \vec{a}.

Recall that \vec{a}\cdot\vec{v} can be defined as "|\vec{a}||\vec{v}| cos(\theta) where \theta is the angle between \vec{a} and \vec{v}.

From simple trigonometry, the component of \vec{v} parallel to \vec{a} is |\vec{v}|cos(\theta)= \vec{a}\cdot\vec{v}/|\vec{a}|. To get a "vector projection", a vector in the direction of \vec{a} with that length, multiply by the unit vector in the direction of \vec{a}, \vec{a}/|\vec{a}|. That gives (\vec{a}\cdot\vec{v}/|\vec{a}|^2)\vec{a} as the "vector component of \vec{v} parallel to \vec{a}". Since the components parallel and perpendicular to \vec{a} must add to \vec{v}, the component perpendicular to \vec{a} is \vec{v}-(\vec{a}\cdot\vec{v}/|\vec{a}|^2)\vec{a}.

Now, reflecting \vec{v} along an axis orthogonal to \vec{a} gives a new vector having the same component perpendicular to \vec{a} but with the component parallel reversed:
\vec{v}-(\vec{a}\cdot\vec{v}/|\vec{a}|^2)\vec{a} -\vec{a}\cdot\vec{v}/|\vec{a}|^2)\vec{a}
= \vec{v}-2(\vec{a}\cdot\vec{v}/|\vec{a}|^2)\vec{a}
 
I have an incomplete answer, but maybe you can finish it.

Let v' be the reflection of v over some axis. If you try to draw a vector s such that v = v' + s, using the triangle method to add the vectors v and s, you'll see that s is orthogonal to the reflection axis, and thus colinear to a.

The drawing should show an isosceles triangle, bisected by the reflection axis, where the two equally-sized sides are |v| and |v'|, the third side being of size |s|. From this triangle you should be able to calculate the magnitude of s as equal to 2 . |v| . cos theta, where "theta" is the angle between v (or v') and the normal to the reflection axis. (Try it on the drawing!)

Now, the expression 2 . |v| . cos theta is equal in magnitude to 2 . (va) / |a|. Multiplying this quantity by an unitary vector in the direction of a, namely a / |a|, you should get your vector s... or almost. There is a +/-1 factor not accounted yet for: has s the same direction of a or the opposite?

(This sign is the missing part that I was lazy to complete - I'd guess it has to do with v being or not on the same side of the axis than a; examining the sign of (va) should give a clue.)

Doing the multiplication above (and correcting the sign), you should get s = 2 (va) . a / |a|^2 = 2 (va) . a / (aa), and when replacing this expression for s into v' = v - s, you get your reflection formula.

Edit: Oh, I was pwned again. :)
 
Last edited:
thanks a lot!
 
Good morning I have been refreshing my memory about Leibniz differentiation of integrals and found some useful videos from digital-university.org on YouTube. Although the audio quality is poor and the speaker proceeds a bit slowly, the explanations and processes are clear. However, it seems that one video in the Leibniz rule series is missing. While the videos are still present on YouTube, the referring website no longer exists but is preserved on the internet archive...

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