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M2 2025 June Q3

A Level / Edexcel / M2

IAL 2025 June Paper · Question 3

题目

Problem

3.

[The distance of the centre of mass of a semicircular arc of radius rr is 2rπ\frac{2r}{\pi} from its centre.]

A uniform rigid wire framework, shown in Figure 1, consists of two wire semicircular arcs ABAB and CDCD, both with centre OO, joined by two straight pieces of wire, ACAC and DBDB.

Arc ABAB has radius 2a2a, arc CDCD has radius aa, AC=DB=aAC=DB=a, and ACDBACDB is a straight line.

The framework lies in a single plane.

(a) Show that the centre of mass of the framework is a distance 6a3π+2\frac{6a}{3\pi+2} from ABAB.

(5)

The point EE is on the arc ABAB and the angle AOEAOE is a right angle.

The framework is freely suspended from AA.

The framework hangs at rest in a vertical plane with AEAE making an angle θ\theta with the downward vertical.

(b) Find the exact value of tan⁡θ\tan\theta, simplifying your answer.

(5)
题目中文翻译

[ 半径为 rr 的半圆弧的质心到圆心的距离为 2rπ\frac{2r}{\pi}。 ]

图 1 所示的均匀刚性金属丝框架,由圆心均为 OO 的两个金属丝半圆弧 ABAB、CDCD,通过两段直金属丝 ACAC、DBDB 连接而成。

圆弧 ABAB 的半径为 2a2a,圆弧 CDCD 的半径为 aa,AC=DB=aAC=DB=a,且 ACDBACDB 共线。

框架位于同一平面内。

(a) 证明框架的质心到 ABAB 的距离为 6a3π+2\frac{6a}{3\pi+2}。

(5)

EE 点位于圆弧 ABAB 上,且 ∠AOE\angle AOE 为直角。

框架从 AA 点自由悬挂。

框架静止悬挂于竖直平面内,AEAE 与竖直向下方向成 θ\theta 角。

(b) 求 tan⁡θ\tan\theta 的精确值,并化简答案。

(5)

解答

(a)

解法一

思路

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这是均匀金属丝框架,质量与长度成正比,不与面积成正比。以连接 A,BA,B 的直线为参考,两半圆弧在相反侧,直线段也贡献质量但力矩为零。

答题过程

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Let the common mass per unit length be ρ\rho. Measure signed perpendicular distances from the straight line ABAB towards EE as positive.

The outer semicircular arc has length 2πa2\pi a and centroid distance 4a/π4a/\pi. The inner arc has length πa\pi a and centroid distance −2a/π-2a/\pi.

The straight pieces ACAC and DBDB have total length 2a2a and lie on ABAB, so their centroid distance is zero. The total wire length is

L=2πa+πa+2a=(3π+2)a.L=2\pi a+\pi a+2a=(3\pi+2)a.

By symmetry, the centre of mass GG lies on OEOE. Taking moments of masses about ABAB,

ρ(3π+2)a d=ρ(2πa)4aπ+ρ(πa)(−2aπ)+ρ(2a)(0).\rho(3\pi+2)a\,d=\rho(2\pi a)\frac{4a}{\pi}+\rho(\pi a)\left(-\frac{2a}{\pi}\right)+\rho(2a)(0).

Cancelling ρ\rho gives

(3π+2)a d=8a2−2a2=6a2.(3\pi+2)a\,d=8a^2-2a^2=6a^2.

Hence

d=6a3π+2.\boxed{d=\frac{6a}{3\pi+2}}.

(b)

解法一

思路

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悬挂时 AGAG 竖直。先求 AGAG 与 AOAO 的角;由于 AO=OEAO=OE 且二者垂直,AEAE 与 AOAO 成 45∘45^\circ。所求角是两角之差,须使用正切差角公式。

答题过程

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Let α=∠OAG\alpha=\angle OAG. Since AO=2aAO=2a and OG=dOG=d,

tan⁡α=d2a=33π+2.\tan\alpha=\frac{d}{2a}=\frac3{3\pi+2}.

Triangle AOEAOE is right-angled and isosceles, so

∠OAE=45∘.\angle OAE=45^\circ.

Since 0<d<2a0<d<2a, AGAG lies between AOAO and AEAE. When suspended, AGAG is vertically downwards, and therefore

θ=45∘−α.\theta=45^\circ-\alpha.

Using the tangent subtraction formula,

tan⁡θ=1−tan⁡α1+tan⁡α.\tan\theta=\frac{1-\tan\alpha}{1+\tan\alpha}.

Thus

tan⁡θ=1−3/(3π+2)1+3/(3π+2)=3π+2−33π+2+3,\tan\theta=\frac{1-3/(3\pi+2)}{1+3/(3\pi+2)}=\frac{3\pi+2-3}{3\pi+2+3},

and hence

tan⁡θ=3π−13π+5.\boxed{\tan\theta=\frac{3\pi-1}{3\pi+5}}.

解法二

思路

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也可将 AGAG 沿 AEAE 与垂直 AEAE 的方向投影。两分量的比直接给角度正切,避免先引入另一个角。

答题过程

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Use the original orientation with coordinates

O=(0,0),A=(0,2a),E=(2a,0),G=(d,0).O=(0,0),\quad A=(0,2a),\quad E=(2a,0),\quad G=(d,0).

Then the vector from AA to GG has components (d,−2a)(d,-2a). A unit vector along AEAE is (1,−1)/2(1,-1)/\sqrt2, so the component of AGAG along AEAE is

d+2a2.\frac{d+2a}{\sqrt2}.

The magnitude of its perpendicular component is

2a−d2,\frac{2a-d}{\sqrt2},

since d<2ad<2a.

As AGAG becomes vertical when suspended, the angle between AGAG and AEAE is θ\theta. Thus

tan⁡θ=(2a−d)/2(2a+d)/2=2a−d2a+d.\tan\theta=\frac{(2a-d)/\sqrt2}{(2a+d)/\sqrt2}=\frac{2a-d}{2a+d}.

Substituting d=6a/(3π+2)d=6a/(3\pi+2) and cancelling 2a2a,

tan⁡θ=1−3/(3π+2)1+3/(3π+2).\tan\theta=\frac{1-3/(3\pi+2)}{1+3/(3\pi+2)}.

Hence

tan⁡θ=3π−13π+5.\boxed{\tan\theta=\frac{3\pi-1}{3\pi+5}}.