Transverse and Longitudinal Waves β€” Question 1

Section 16-2 Β· Physics pages 2412–2413

Question 1 Wave type is defined relative to propagation, not the page A plane mechanical disturbance propagates along Λ†n = (3Λ†i + 4Λ†j)/5. Its displacement is u = a(4Λ†i βˆ’3Λ†j) cos Ξ¦/5. x y Λ†n u Vector geometry in the labeled plane; lengths are schematic. (a) Classify the displacement as transverse or longitudinal. (b) If the drawing is rotated, can the classification change? Explain with a coordinate-independent test.
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Question 1 - Solution Wave type is defined relative to propagation, not the page x y Λ†n u Method and mathematical working Project displacement onto the unit propagation vector. The longitudinal scalar component vanishes exactly when the motion is perpendicular to propagation. uβˆ₯= u Β· Λ†n, uβŠ₯= u βˆ’uβˆ₯Λ†n. bn Β· u = a cos Ξ¦ 25 (3 Β· 4 + 4 Β· (βˆ’3)) = 0. (a) Calculation and conclusion The dot product is u Β· Λ†n = a(12 βˆ’12) cos Ξ¦/25 = 0, so displacement is transverse. Neither vector has to be horizontal or vertical. (b) Interpretation and limits Rigid rotation preserves dot products and angles. Perpendicular displacement remains transverse in every rotated coordinate system. The classification refers to displacement relative to propagation, not relative to the sheet of paper. Physical check Both given direction vectors have unit length. Their zero dot product therefore establishes a right angle independently of their visual orientation.

Question 1

Wave type is defined relative to propagation, not the page

A plane mechanical disturbance propagates along 𝒏̂=(3π’ŠΜ‚+4𝒋̂)/5\hat{\mathbf n}=(3\hat{\mathbf i}+4\hat{\mathbf j})/5. Its displacement is 𝒖=a(4π’ŠΜ‚βˆ’3𝒋̂)cos⁡Ξ¦/5\mathbf u=a(4\hat{\mathbf i}-3\hat{\mathbf j})\cos\Phi/5.

Diagram shown in the original SVG worksheet.

  1. Classify the displacement as transverse or longitudinal.

  2. If the drawing is rotated, can the classification change? Explain with a coordinate-independent test.

Question 1 - Solution

Wave type is defined relative to propagation, not the page

Diagram shown in the original SVG worksheet.

Method and mathematical working

Project displacement onto the unit propagation vector. The longitudinal scalar component vanishes exactly when the motion is perpendicular to propagation.uβˆ₯=𝒖⋅𝒏̂,π’–βŸ‚=π’–βˆ’uβˆ₯𝒏̂.𝒏̂⋅𝒖=acos⁡Ξ¦25(3β‹…4+4β‹…(βˆ’3))=0.\begin{aligned}u_\parallel&=\mathbf u\cdot\hat{\mathbf n},\qquad \mathbf u_\perp=\mathbf u-u_\parallel\hat{\mathbf n}.\\[4pt]\widehat{\mathbf n}\cdot\mathbf u&=\frac{a\cos\Phi}{25}(3\cdot4+4\cdot(-3))=0.\end{aligned}

(a) Calculation and conclusion

The dot product is 𝒖⋅𝒏̂=a(12βˆ’12)cos⁡Ξ¦/25=0\mathbf u\cdot\hat{\mathbf n}=a(12-12)\cos\Phi/25=0, so displacement is transverse. Neither vector has to be horizontal or vertical.

(b) Interpretation and limits

Rigid rotation preserves dot products and angles. Perpendicular displacement remains transverse in every rotated coordinate system. The classification refers to displacement relative to propagation, not relative to the sheet of paper.

Physical check

Both given direction vectors have unit length. Their zero dot product therefore establishes a right angle independently of their visual orientation.