Are Angular Quantities Vectors? — Question 8

Section 10-2 · Physics pages 1406–1407

Question 8 Mirror reflection distinguishes axial from polar vectors A disk rotates in the xy plane. At⃗r = (R, 0, 0) a mark has velocity⃗v = (0, V, 0) with R, V > 0. Reflect the physical motion in the yz plane, so polar vectors transform by x →−x. x mirror R −R V ˆy V ˆy The mirror reverses the position coordinate while retaining the upward velocity. (a) Find the angular-velocity direction before and after reflection. (b) Explain why applying the polar-vector reflection rule directly to the original angular velocity would fail.
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Question 8 - Solution Mirror reflection distinguishes axial from polar vectors x mirror R −R V ˆy V ˆy (a) Derivation and calculation For the original motion,⃗v =⃗ω ×⃗r gives (ωzˆz) × (Rˆx) = ωzRˆy = V ˆy ⇒⃗ ω = V R ˆz . After reflection, (ω′ zˆz) × (−Rˆx) = V ˆy ⇒⃗ ω′ = −V R ˆz . (b) Result and interpretation For the reflection matrix S = diag(−1, 1, 1), polar vectors obey⃗v′ = S⃗v. An axial vector instead obeys⃗ ω′ = det(S)S⃗ω = −S⃗ω . Applying only S to the original z vector would incorrectly leave the handedness unchanged. Physical check The mirrored mark moves upward at the left side of the circle, requiring clockwise rotation.

Question 8

Mirror reflection distinguishes axial from polar vectors

A disk rotates in the xyxy plane. At r→=(R,0,0)\vec r=(R,0,0) a mark has velocity v→=(0,V,0)\vec v=(0,V,0) with R,V>0R,V>0. Reflect the physical motion in the yzyz plane, so polar vectors transform by x→−xx\to-x.

Diagram shown in the original SVG worksheet.

  1. Find the angular-velocity direction before and after reflection.

  2. Explain why applying the polar-vector reflection rule directly to the original angular velocity would fail.

Question 8 - Solution

Mirror reflection distinguishes axial from polar vectors

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For the original motion, v→=ω→×r→\vec v=\vec\omega\times\vec r gives (ωzẑ)×(Rx̂)=ωzRŷ=Vŷ⇒ω→=VRẑ.(\omega_z\hat z)\times(R\hat x)=\omega_z R\hat y=V\hat y \quad\Rightarrow\quad\boxed{\vec\omega=\frac VR\hat z}. After reflection, (ωz′ẑ)×(−Rx̂)=Vŷ⇒ω→′=−VRẑ.(\omega_z^{\prime}\hat z)\times(-R\hat x)=V\hat y \quad\Rightarrow\quad\boxed{\vec\omega^{\prime}=-\frac VR\hat z}.

(b) Result and interpretation

For the reflection matrix S=diag⁡(−1,1,1)S=\operatorname{diag}(-1,1,1), polar vectors obey v→′=Sv→\vec v^{\prime}=S\vec v. An axial vector instead obeys ω→′=det⁡(S)Sω→=−Sω→.\boxed{\vec\omega^{\prime}=\det(S)S\vec\omega=-S\vec\omega}. Applying only SS to the original zz vector would incorrectly leave the handedness unchanged.

Physical check

The mirrored mark moves upward at the left side of the circle, requiring clockwise rotation.