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M3 2026 June A Q3

A Level / Edexcel / M3

IAL 2026 June A Paper · Question 3

题目

Problem

3.

(a) Use algebraic integration to show that the centre of mass of a uniform semicircular lamina of radius rr is 4r3π\dfrac{4r}{3\pi} from the centre of the semicircle.

[You may assume, without proof, that the area of a circle of radius rr is πr2\pi r^2.]

(5)

In the template shown shaded in Figure 2, C1C_1 is a semicircular lamina with a semicircular lamina C3C_3 removed. A semicircular lamina C2C_2 is attached to C1C_1.

  • C1C_1 has radius 4a4a, diameter ABAB and centre OO
  • C2C_2 has radius 2a2a and centre OO
  • C3C_3 has radius aa and centre OO

Laminas C1C_1 and C2C_2 are made from the same material and lie in the same plane.

The template is freely suspended from AA and hangs in equilibrium with ABAB at an angle of θ∘\theta^\circ to the downward vertical.

(b) Find the value of θ\theta

(7)
题目中文翻译

(a) 用代数积分证明:半径为 rr 的均匀半圆形薄片的质心到半圆圆心的距离为 4r3π\dfrac{4r}{3\pi}。

[可直接假设半径为 rr 的圆的面积为 πr2\pi r^2,无须证明。]

(5)

在图 2 阴影所示的模板中,从半圆形薄片 C1C_1 中挖去半圆形薄片 C3C_3,并将半圆形薄片 C2C_2 连接于 C1C_1。

  • C1C_1 的半径为 4a4a,直径为 ABAB,圆心为 OO;
  • C2C_2 的半径为 2a2a,圆心为 OO;
  • C3C_3 的半径为 aa,圆心为 OO。

薄片 C1C_1、C2C_2 由相同材料制成,并位于同一平面内。

模板从 AA 自由悬挂并处于平衡,ABAB 与竖直向下方向成 θ∘\theta^\circ 角。

(b) 求 θ\theta 的值。

(7)

解答

(a)

解法一

思路

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先把半圆放在 yy 轴右侧,以圆心为原点。竖条的长度为 2r2−x22\sqrt{r^2-x^2},质心横坐标就是 xx;用替换 u=r2−x2u=r^2-x^2 完成面积矩积分。

答题过程

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Place the semicircle in x≥0x\ge0, with centre O=(0,0)O=(0,0) and diameter on the yy-axis. By symmetry, its centre of mass lies on the positive xx-axis.

A vertical strip has area 2r2−x2 dx2\sqrt{r^2-x^2}\,\mathrm dx. With uniform surface density cancelling, its first area moment about the yy-axis is

J=2∫0rxr2−x2 dx.J=2\int_0^r x\sqrt{r^2-x^2}\,\mathrm dx.

Using u=r2−x2u=r^2-x^2, du=−2x dx\mathrm du=-2x\,\mathrm dx,

∫xr2−x2 dx=−12∫u1/2 du=−13(r2−x2)3/2.\int x\sqrt{r^2-x^2}\,\mathrm dx =-\frac12\int u^{1/2}\,\mathrm du =-\frac13(r^2-x^2)^{3/2}.

Consequently,

J=2[−13(r2−x2)3/2]0r=2r33.J=2\left[-\frac13(r^2-x^2)^{3/2}\right]_0^r =\frac{2r^3}{3}.

The semicircle has area πr2/2\pi r^2/2. Hence its centre of mass is at distance

xˉ=Jπr2/2=4r3π\boxed{\bar x=\frac{J}{\pi r^2/2}=\frac{4r}{3\pi}}

from OO.

解法二

思路

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也可把半圆放在 xx 轴上方,用每根竖条的中点计算面积矩。这时被积式成为多项式,特别要保留竖条质心高度中的 1/21/2。

答题过程

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Place the semicircle above the xx-axis, with centre O=(0,0)O=(0,0), so

y=r2−x2,−r≤x≤r.y=\sqrt{r^2-x^2},\qquad -r\le x\le r.

By symmetry, xˉ=0\bar x=0.

A vertical strip has area y dxy\,\mathrm dx and centre of mass at height y/2y/2. Its moment about the xx-axis is therefore 12y2 dx\tfrac12y^2\,\mathrm dx. Thus

J=12∫−rr(r2−x2) dx=12[r2x−x33]−rr.J=\frac12\int_{-r}^{r}(r^2-x^2)\,\mathrm dx =\frac12\left[r^2x-\frac{x^3}{3}\right]_{-r}^{r}.

Evaluating the limits,

J=12[(r3−r33)−(−r3+r33)]=2r33.J=\frac12\left[\left(r^3-\frac{r^3}{3}\right) -\left(-r^3+\frac{r^3}{3}\right)\right] =\frac{2r^3}{3}.

Divide by the area πr2/2\pi r^2/2:

yˉ=2r3/3πr2/2=4r3π.\boxed{\bar y=\frac{2r^3/3}{\pi r^2/2}=\frac{4r}{3\pi}}.

Since xˉ=0\bar x=0, this is the distance from the centre.

解法三

思路

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第三种方法把半圆分成很窄的扇形。先说明每个微小扇形的质心位于约 2r/32r/3 处,再对这些小扇形的面积矩积分,不能只引用待证明的半圆质心公式。

答题过程

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Place the semicircle above the xx-axis with centre OO. Let ϕ\phi be the polar angle from the positive xx-axis, where 0≤ϕ≤π0\le\phi\le\pi.

A narrow sector of angle dϕ\mathrm d\phi has area 12r2 dϕ\tfrac12r^2\,\mathrm d\phi. In the limit of a narrow sector its centre is at radial distance 2r/32r/3. This follows by weighting radial distance ss with the area element s ds dϕs\,\mathrm ds\,\mathrm d\phi:

∫0rs2 ds∫0rs ds=r3/3r2/2=2r3.\frac{\int_0^r s^2\,\mathrm ds}{\int_0^r s\,\mathrm ds} =\frac{r^3/3}{r^2/2}=\frac{2r}{3}.

Its centroid height is therefore (2r/3)sin⁡ϕ(2r/3)\sin\phi. The moment of the whole semicircle about the xx-axis is

J=∫0π(12r2)(2r3sin⁡ϕ) dϕ=r33[−cos⁡ϕ]0π=2r33.J=\int_0^\pi\left(\frac12r^2\right)\left(\frac{2r}{3}\sin\phi\right)\,\mathrm d\phi =\frac{r^3}{3}\left[-\cos\phi\right]_0^\pi =\frac{2r^3}{3}.

By symmetry the centre of mass is on the yy-axis. Dividing by the area,

yˉ=Jπr2/2=4r3π,\boxed{\bar y=\frac{J}{\pi r^2/2}=\frac{4r}{3\pi}},

which is its distance from OO.

(b)

解法一

思路

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以直径 ABAB 为参考线,向大半圆一侧取正。附加的中半圆在负侧,挖掉的小半圆在正侧,两者对总质量矩的贡献都是负的;但总面积是 16+4−116+4-1。

答题过程

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Take perpendicular distance from ABAB as positive towards C1C_1. By symmetry the template’s centre of mass GG is on the line through OO perpendicular to ABAB.

The areas of C1,C2,C3C_1,C_2,C_3 are in the ratio 16:4:116:4:1, and from (a) their signed centroid distances are respectively

16a3π,−8a3π,4a3π.\frac{16a}{3\pi},\qquad -\frac{8a}{3\pi},\qquad \frac{4a}{3\pi}.

The template contains C1+C2−C3C_1+C_2-C_3. Since all pieces have the same surface density, its signed distance d=OGd=OG satisfies

(16+4−1)d=1616a3π+4(−8a3π)−4a3π.(16+4-1)d =16\frac{16a}{3\pi}+4\left(-\frac{8a}{3\pi}\right) -\frac{4a}{3\pi}.

Hence

19d=256a−32a−4a3π=220a3π,d=220a57π>0.19d=\frac{256a-32a-4a}{3\pi}=\frac{220a}{3\pi}, \qquad d=\frac{220a}{57\pi}>0.

When suspended from AA, AGAG is vertically downwards. The triangle AOGAOG is right-angled at OO, with AO=4aAO=4a, so the required angle between ABAB and AGAG is given by

tan⁡θ∘=OGAO=220a/(57π)4a=5557π.\tan\theta^\circ=\frac{OG}{AO}=\frac{220a/(57\pi)}{4a}=\frac{55}{57\pi}.

Thus

θ=tan⁡−1 ⁣(5557π)=17.1(3 s.f.).\boxed{\theta=\tan^{-1}\!\left(\frac{55}{57\pi}\right)=17.1\quad\text{(3 s.f.)}.}