Vectors and the Laws of Physics — Question 3

Section 3-6 · Physics pages 416–417

Question 3 A vector equation survives a common rotation An experiment reports⃗A = (2, 3) m,⃗B = (−1, 4) m and⃗C = (1, 7) m. Its proposed relation is⃗ C =⃗A +⃗B. Use 45◦counterclockwise rotated axes, for which (Xx′, Xy′) = ((Xx + Xy)/ √ 2, (−Xx + Xy)/ √ 2). A: (2, 3) B: (−1, 4) C: (1, 7) x y x′ y′ One displacement triangle, expressed in two bases 45 degrees apart. Components are in metres. (a) Check the relation in the original axes and transform all three vectors. (b) Check both primed component equations. (c) Explain why checking only one component, or transforming only C, is insufficient.
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Question 3 - Solution A vector equation survives a common rotation A: (2, 3) B: (−1, 4) C: (1, 7) x y x′ y′ Here Qϕ transforms components when axes turn counterclockwise by ϕ; Rϕ = Q−ϕ rotates the arrow in fixed axes. An unsubscripted Q denotes the same component transformation, and I is the identity. (a) Transform every vector by the same rule.⃗ A +⃗B = (1, 7) =⃗C;⃗ A′ = (5,1) √ 2 ,⃗B′ = (3,5) √ 2 ,⃗C′ = (8,6) √ 2 m Originally (2, 3) + (−1, 4) = (1, 7). The new components are⃗A : (5/ √ 2, 1/ √ 2) m,⃗ B : (3/ √ 2, 5/ √ 2) m, and⃗C : (8/ √ 2, 6/ √ 2) m. (b) Check equality along both independent axes. A′ x + B′ x = 5 + 3 √ 2 = C′ x, A′ y + B′ y = 1 + 5 √ 2 = C′ y The horizontal sum is (5 + 3)/ √ 2 = 8/ √ 2 m and the vertical sum is (1 + 5)/ √ 2 = 6/ √ 2 m. Both agree with C. Projection is linear, so a true vector sum remains true after a common change of axes. (c) Require a complete, consistent representation. Qϕ(⃗A +⃗B) = Qϕ⃗A + Qϕ⃗B, C′ x = A′ x + B′ x alone leaves C′ y unchecked One matching component permits an undetected mismatch along the perpendicular direction. Transforming C but leaving A and B in the old frame combines incompatible coordinate descriptions. Frame-independent validity means the same vector relation holds when all entries are expressed consistently.

Question 3

A vector equation survives a common rotation

An experiment reports A→=(2,3)\vec A=(2,3) m, B→=(−1,4)\vec B=(-1,4) m and C→=(1,7)\vec C=(1,7) m. Its proposed relation is C→=A→+B→\vec C=\vec A+\vec B. Use 45∘45^\circ counterclockwise rotated axes, for which (Xx′,Xy′)=((Xx+Xy)/2,(−Xx+Xy)/2)(X_{x\prime},X_{y\prime})=((X_x+X_y)/\sqrt2,(-X_x+X_y)/\sqrt2).

Diagram shown in the original SVG worksheet.

  1. Check the relation in the original axes and transform all three vectors.

  2. Check both primed component equations.

  3. Explain why checking only one component, or transforming only C, is insufficient.

Question 3 - Solution

A vector equation survives a common rotation

Diagram shown in the original SVG worksheet.

Here QϕQ_\phi transforms components when axes turn counterclockwise by ϕ\phi; Rϕ=Q−ϕR_\phi=Q_{-\phi} rotates the arrow in fixed axes. An unsubscripted QQ denotes the same component transformation, and II is the identity.

(a) Transform every vector by the same rule.

A→+B→=(1,7)=C→;A→′=(5,1)2,B→′=(3,5)2,C→′=(8,6)2m\vec A+\vec B=(1,7)=\vec C;\quad\boxed{\vec A'=\tfrac{(5,1)}{\sqrt2},\ \vec B'=\tfrac{(3,5)}{\sqrt2},\ \vec C'=\tfrac{(8,6)}{\sqrt2}}\quad\mathrm m Originally (2,3)+(−1,4)=(1,7)(2,3)+(-1,4)=(1,7). The new components are A→:(5/2,1/2)\vec A:(5/\sqrt2,1/\sqrt2) m, B→:(3/2,5/2)\vec B:(3/\sqrt2,5/\sqrt2) m, and C→:(8/2,6/2)\vec C:(8/\sqrt2,6/\sqrt2) m.

(b) Check equality along both independent axes.

Ax′+Bx′=5+32=Cx′,Ay′+By′=1+52=Cy′A_x'+B_x'=\frac{5+3}{\sqrt2}=C_x',\quad A_y'+B_y'=\frac{1+5}{\sqrt2}=C_y' The horizontal sum is (5+3)/2=8/2(5+3)/\sqrt2=8/\sqrt2 m and the vertical sum is (1+5)/2=6/2(1+5)/\sqrt2=6/\sqrt2 m. Both agree with C. Projection is linear, so a true vector sum remains true after a common change of axes.

(c) Require a complete, consistent representation.

Qϕ(A→+B→)=QϕA→+QϕB→,Cx′=Ax′+Bx′ alone leaves Cy′ uncheckedQ_\phi(\vec A+\vec B)=Q_\phi\vec A+Q_\phi\vec B,\qquad C_x'=A_x'+B_x'\text{ alone leaves }C_y'\text{ unchecked} One matching component permits an undetected mismatch along the perpendicular direction. Transforming C but leaving A and B in the old frame combines incompatible coordinate descriptions. Frame-independent validity means the same vector relation holds when all entries are expressed consistently.