Rotational invariance

In mathematics, a function defined on an inner product space is said to have rotational invariance if its value does not change when arbitrary rotations are applied to its argument. == Mathematics == === Functions === For example, the function f ( x , y ) = x 2 + y 2 {\displaystyle f(x,y)=x^{2}+y^{2}} is invariant under rotations of the plane around the origin, because for a rotated set of coordinates through any angle θ x ′ = x cos ⁡ θ − y sin ⁡ θ {\displaystyle x'=x\cos \theta -y\sin \theta } y ′ = x sin ⁡ θ + y cos ⁡ θ {\displaystyle y'=x\sin \theta +y\cos \theta } the function, after some cancellation of terms, takes exactly the same form f ( x ′ , y ′ ) = x 2 + y 2 {\displaystyle f(x',y')={x}^{2}+{y}^{2}} The rotation of coordinates can be expressed using matrix form using the rotation matrix, [ x ′ y ′ ] = [ cos ⁡ θ − sin ⁡ θ sin ⁡ θ cos ⁡ θ ] [ x y ] , {\displaystyle {\begin{bmatrix}x'\\y'\\\end{bmatrix}}={\begin{bmatrix}\cos \theta &-\sin \theta \\\sin \theta &\cos \theta \\\end{bmatrix}}{\begin{bmatrix}x\\y\\\end{bmatrix}},} or symbolically, x′ = Rx.

Source: Wikipedia — Rotational invariance (CC BY-SA 4.0)

Rotational invariance

In mathematics, a function defined on an inner product space is said to have rotational invariance if its value does not change when arbitrary rotations are applied to its argument. == Mathematics == === Functions === For example, the function f ( x , y ) = x 2 + y 2 {\displaystyle f(x,y)=x^{2}+y^{2}} is invariant under rotations of the plane around the origin, because for a rotated set of coordinates through any angle θ x ′ = x cos ⁡ θ − y sin ⁡ θ {\displaystyle x'=x\cos \theta -y\sin \theta } y ′ = x sin ⁡ θ + y cos ⁡ θ {\displaystyle y'=x\sin \theta +y\cos \theta } the function, after some cancellation of terms, takes exactly the same form f ( x ′ , y ′ ) = x 2 + y 2 {\displaystyle f(x',y')={x}^{2}+{y}^{2}} The rotation of coordinates can be expressed using matrix form using the rotation matrix, [ x ′ y ′ ] = [ cos ⁡ θ − sin ⁡ θ sin ⁡ θ cos ⁡ θ ] [ x y ] , {\displaystyle {\begin{bmatrix}x'\\y'\\\end{bmatrix}}={\begin{bmatrix}\cos \theta &-\sin \theta \\\sin \theta &\cos \theta \\\end{bmatrix}}{\begin{bmatrix}x\\y\\\end{bmatrix}},} or symbolically, x′ = Rx.

Source: Wikipedia "Rotational invariance" · CC BY-SA 4.0

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