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Linear Algebra, 2020a

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322 Chapter Three. Maps Between Spaces<br />

often use this term to mean not just that the columns are orthogonal but also<br />

that they have length one).<br />

We can leverage this characterization to understand the geometric actions<br />

of distance-preserving maps. Because ‖t(⃗v )‖ = ‖⃗v ‖, the map t sends any ⃗v<br />

somewhere on the circle about the origin that has radius equal to the length of<br />

⃗v. In particular, ⃗e 1 and ⃗e 2 map to the unit circle. What’s more, once we fix the<br />

unit vector ⃗e 1 as mapped to the vector with components a and b then there<br />

are only two places where ⃗e 2 can go if its image is to be perpendicular to the<br />

first vector’s image: it can map either to one where ⃗e 2 maintains its position a<br />

quarter circle clockwise from ⃗e 1<br />

( ) −b<br />

a<br />

( a<br />

b)<br />

(<br />

a<br />

Rep E2 ,E 2<br />

(t) =<br />

b<br />

)<br />

−b<br />

a<br />

or to one where it goes a quarter circle counterclockwise.<br />

( a<br />

b)<br />

( ) b<br />

−a<br />

(<br />

a<br />

Rep E2 ,E 2<br />

(t) =<br />

b<br />

)<br />

b<br />

−a<br />

The geometric description of these two cases is easy. Let θ be the counterclockwise<br />

angle between the x-axis and the image of ⃗e 1 . The first matrix above<br />

represents, with respect to the standard bases, a rotation of the plane by θ<br />

radians.<br />

( ) −b<br />

a<br />

( a<br />

b)<br />

( )<br />

x t<br />

↦−→<br />

y<br />

(<br />

)<br />

x cos θ − y sin θ<br />

x sin θ + y cos θ<br />

The second matrix above represents a reflection of the plane through the line<br />

bisecting the angle between ⃗e 1 and t(⃗e 1 ).

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