Vectors and the Laws of Physics — Question 5

Section 3-6 · Physics pages 420–421

Question 5 Which combinations are independent of axis orientation? A fixed planar vector has components (3, 4) m. Consider P = A2 x + A2 y, Q = Ax + Ay, and T = A2 x −A2 y. Rotate the axes counterclockwise by 90◦, so the new components are (4, −3) m. x y (3, 4) m x′ y′ The arrow remains fixed while the new x axis points upward and the new y axis points left. (a) Evaluate P, Q and T in both frames with their units. (b) Which expression is guaranteed to be invariant under every planar rotation? Justify beyond this one example. (c) Explain why a component being a signed number does not make it a rotationally invariant physical scalar.
Show solutionHide solution
Question 5 - Solution Which combinations are independent of axis orientation? x y (3, 4) m x′ y′ (a) Calculate before classifying. (P, Q, T) = (25 m2, 7 m, −7 m2), (P ′, Q′, T ′) = (25 m2, 1 m, 7 m2) Originally P = 25 m2, Q = 7 m, and T = −7 m2. After the turn they are P′ = 25 m2, Q′ = 1 m, and T′ = 7 m2. Q and T fail even this simple rotation test. (b) Use the orthogonality of the transformation. P ′ = (Axc + Ays)2 + (−Axs + Ayc)2 = (c2 + s2)(A2 x + A2 y) = P Write c = cos ϕ and s = sin ϕ. For a general angle, substituting Ax′ = Ax cos ϕ + Ay sin ϕ and Ay′ = −Ax sin ϕ + Ay cos ϕ into P cancels the mixed terms. Since sin2 ϕ + cos2 ϕ = 1, P′ = A2 x + A2 y. P is the squared physical magnitude. (c) Specify the meaning of scalar. A′ x = Ax cos ϕ + Ay sin ϕ̸ = Ax in general, A′ = A A component is a scalar coefficient in a chosen basis, but generally changes when that basis rotates. A rotationally invariant physical scalar, such as the vector magnitude, has the same value for all such orientations. The word scalar can refer to these different roles; the transformation behavior resolves the distinction.

Question 5

Which combinations are independent of axis orientation?

A fixed planar vector has components (3,4)(3,4) m. Consider P=Ax2+Ay2P=A_x^2+A_y^2, Q=Ax+AyQ=A_x+A_y, and T=Ax2−Ay2T=A_x^2-A_y^2. Rotate the axes counterclockwise by 90∘90^\circ, so the new components are (4,−3)(4,-3) m.

Diagram shown in the original SVG worksheet.

  1. Evaluate P, Q and T in both frames with their units.

  2. Which expression is guaranteed to be invariant under every planar rotation? Justify beyond this one example.

  3. Explain why a component being a signed number does not make it a rotationally invariant physical scalar.

Question 5 - Solution

Which combinations are independent of axis orientation?

Diagram shown in the original SVG worksheet.

(a) Calculate before classifying.

(P,Q,T)=(25m2,7m,−7m2),(P′,Q′,T′)=(25m2,1m,7m2)(P,Q,T)=(25\,\mathrm{m^2},7\,\mathrm m,-7\,\mathrm{m^2}),\quad(P',Q',T')=(25\,\mathrm{m^2},1\,\mathrm m,7\,\mathrm{m^2}) Originally P=25m2P=25\ \mathrm{m^2}, Q=7Q=7 m, and T=−7m2T=-7\ \mathrm{m^2}. After the turn they are P′=25m2P\prime=25\ \mathrm{m^2}, Q′=1Q\prime=1 m, and T′=7m2T\prime=7\ \mathrm{m^2}. Q and T fail even this simple rotation test.

(b) Use the orthogonality of the transformation.

P′=(Axc+Ays)2+(−Axs+Ayc)2=(c2+s2)(Ax2+Ay2)=P\boxed{P'=(A_xc+A_ys)^2+(-A_xs+A_yc)^2=(c^2+s^2)(A_x^2+A_y^2)=P} Write c=cos⁡ϕc=\cos\phi and s=sin⁡ϕs=\sin\phi. For a general angle, substituting Ax′=Axcos⁡ϕ+Aysin⁡ϕA_{x\prime}=A_x\cos\phi+A_y\sin\phi and Ay′=−Axsin⁡ϕ+Aycos⁡ϕA_{y\prime}=-A_x\sin\phi+A_y\cos\phi into P cancels the mixed terms. Since sin⁡2ϕ+cos⁡2ϕ=1\sin^2\phi+\cos^2\phi=1, P′=Ax2+Ay2P\prime=A_x^2+A_y^2. P is the squared physical magnitude.

(c) Specify the meaning of scalar.

Ax′=Axcos⁡ϕ+Aysin⁡ϕ≠Ax in general,A′=AA_x'=A_x\cos\phi+A_y\sin\phi\ne A_x\text{ in general},\qquad A'=A A component is a scalar coefficient in a chosen basis, but generally changes when that basis rotates. A rotationally invariant physical scalar, such as the vector magnitude, has the same value for all such orientations. The word scalar can refer to these different roles; the transformation behavior resolves the distinction.