Length — Question 7

Section 1-4 · Physics pages 84–85

Question 7 A distant target and two different distances A surveyor sets out a perpendicular baseline b = 30.0 m as shown. The observed angular quantity is u = tan θ = 0.0250. You may use the supplied right-triangle relations D = b u, S = √ D2 + b2. No trigonometric calculation of θ is needed. A B Target D b S θ Plan view, not to scale. Baseline AB is perpendicular to AT; the dashed direction through B is parallel to AT. S is the sloping sightline distance. (a) Find the central values of D and S. Is the quotient b/u the distance from B to the target? Explain the geometric distinction. (b) Treat b as exact and take u ∈[0.0245, 0.0255] as a closed hard bound. Find the resulting interval for D and explain which endpoint of u produces the greatest distance. (c) The baseline is extended to 60.0 m, still perpendicular to AT. The same target then gives u ∈[0.0495, 0.0505]. Find the new distance interval. Explain why this improves the inference when the absolute bound on u remains the same.
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Question 7 - Solution A distant target and two different distances A B Target D b S θ (a) Identify the side computed by each relation. D = 30.0 0.0250 m = 1200 m , S = √ 12002 + 302 m ≈1200.375 m . D is AT, the perpendicular range from A. B-to-target distance is S, the hypotenuse, about 0.375 m longer. A small numerical difference does not make the two measurands identical. (b) Invert the bounds in the correct order. For positive u, increasing u decreases b/u. Thus D ∈ [ 30.0 0.0255, 30.0 0.0245 ] m ≈[1176.47, 1224.49] m . The smallest allowed angle quantity produces the greatest inferred distance. The exact fractions specify the hard interval; displayed decimal endpoints are approximate. (c) A larger baseline gives a larger angular signal. Dmax −Dmin = b u0 −δu − b u0 + δu = 2bδu u2 0 −(δu)2 . D ∈ [ 60.0 0.0505, 60.0 0.0495 ] m ≈[1188.12, 1212.12] m . Both central estimates are 1200 m, but the interval width decreases from about 48.02 m to 24.00 m. The same absolute bound ±0.0005 is a smaller fraction of 0.0500 than of 0.0250. The improvement assumes the baseline itself remains accurately known and the stated geometry and angular bounds remain valid.

Question 7

A distant target and two different distances

A surveyor sets out a perpendicular baseline b=30.0mb=30.0\ \mathrm{m} as shown. The observed angular quantity is u=tan⁡θ=0.0250u=\tan\theta=0.0250. You may use the supplied right-triangle relations D=bu,S=D2+b2.D=\frac{b}{u},\qquad S=\sqrt{D^2+b^2}. No trigonometric calculation of θ\theta is needed.

Diagram shown in the original SVG worksheet.

  1. Find the central values of DD and SS. Is the quotient b/ub/u the distance from B to the target? Explain the geometric distinction.

  2. Treat bb as exact and take u∈[0.0245,0.0255]u\in[0.0245,0.0255] as a closed hard bound. Find the resulting interval for DD and explain which endpoint of uu produces the greatest distance.

  3. The baseline is extended to 60.0m60.0\ \mathrm{m}, still perpendicular to AT. The same target then gives u∈[0.0495,0.0505]u\in[0.0495,0.0505]. Find the new distance interval. Explain why this improves the inference when the absolute bound on uu remains the same.

Question 7 - Solution

A distant target and two different distances

Diagram shown in the original SVG worksheet.

(a) Identify the side computed by each relation.

D=30.00.0250m=1200m,S=12002+302m≈1200.375m.D=\frac{30.0}{0.0250}\ \mathrm{m}=\boxed{1200\ \mathrm{m}},\qquad S=\sqrt{1200^2+30^2}\ \mathrm{m}\approx\boxed{1200.375\ \mathrm{m}}. DD is AT, the perpendicular range from A. B-to-target distance is SS, the hypotenuse, about 0.375m0.375\ \mathrm{m} longer. A small numerical difference does not make the two measurands identical.

(b) Invert the bounds in the correct order.

For positive uu, increasing uu decreases b/ub/u. Thus D∈[30.00.0255,30.00.0245]m≈[1176.47,1224.49]m.D\in\left[\frac{30.0}{0.0255},\frac{30.0}{0.0245}\right]\ \mathrm{m} \approx\boxed{[1176.47,\ 1224.49]\ \mathrm{m}}. The smallest allowed angle quantity produces the greatest inferred distance. The exact fractions specify the hard interval; displayed decimal endpoints are approximate.

(c) A larger baseline gives a larger angular signal.

Dmax−Dmin=bu0−δu−bu0+δu=2bδuu02−(δu)2.D_{\max}-D_{\min}=\frac{b}{u_0-\delta u}-\frac{b}{u_0+\delta u}=\frac{2b\delta u}{u_0^2-(\delta u)^2}.

D∈[60.00.0505,60.00.0495]m≈[1188.12,1212.12]m.D\in\left[\frac{60.0}{0.0505},\frac{60.0}{0.0495}\right]\ \mathrm{m} \approx\boxed{[1188.12,\ 1212.12]\ \mathrm{m}}. Both central estimates are 1200 m, but the interval width decreases from about 48.02m48.02\ \mathrm{m} to 24.00m24.00\ \mathrm{m}. The same absolute bound ±0.0005\pm0.0005 is a smaller fraction of 0.0500 than of 0.0250. The improvement assumes the baseline itself remains accurately known and the stated geometry and angular bounds remain valid.