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M2 2021 Oct Q7

A Level / Edexcel / M2

IAL 2021 Oct Paper · Question 7

题目

Problem

7.

In this question you may use, without proof, the formula for the centre of mass of a uniform sector of a circle, as given in the formulae book.

The uniform lamina ABCDEABCDE, shown shaded in Figure 3, is formed by joining a rectangle to a sector of a circle.

  • The rectangle ABCEABCE has AB=EC=aAB=EC=a and AE=BC=dAE=BC=d
  • The sector CDECDE has centre CC and radius aa
  • Angle ECD=π3ECD=\frac\pi3 radians

The centre of mass of the lamina lies on ECEC.

(a) Show that a=3da=\sqrt3d

(4)

The lamina is freely suspended from BB and hangs in equilibrium with BCBC at an angle β\beta radians to the downward vertical.

(b) Find the value of β\beta

(7)
题目中文翻译

本题中可直接使用公式手册给出的均匀圆扇形质心公式,无须证明。

图 3 阴影所示的均匀薄片 ABCDEABCDE 由一个长方形与一个圆扇形连接而成。

  • 长方形 ABCEABCE 满足 AB=EC=aAB=EC=a,AE=BC=dAE=BC=d;
  • 扇形 CDECDE 的圆心为 CC,半径为 aa;
  • ∠ECD=π3\angle ECD=\frac\pi3 弧度。

薄片的质心位于 ECEC 上。

(a) 证明 a=3da=\sqrt3d。

(4)

薄片从 BB 点自由悬挂并处于平衡状态,BCBC 与竖直向下方向成 β\beta 弧度角。

(b) 求 β\beta 的值。

(7)

解答

(a)

解法一

思路

展开

扇形质心位于角平分线上,距圆心的公式须用半角 π/6\pi/6。组合质心在 ECEC 上,意味着长方形和扇形关于 ECEC 的面积矩大小相等、方向相反。

答题过程

展开

For a uniform sector of radius aa and angle 2θ2\theta, the centroid is at distance

2asin⁡θ3θ\frac{2a\sin\theta}{3\theta}

from the centre along the angle bisector. Here θ=π/6\theta=\pi/6, so this distance is

2asin⁡(π/6)3(π/6)=2aπ.\frac{2a\sin(\pi/6)}{3(\pi/6)}=\frac{2a}{\pi}.

Its perpendicular distance from ECEC is

2aπsin⁡π6=aπ.\frac{2a}{\pi}\sin\frac\pi6=\frac a\pi.

The sector has area πa2/6\pi a^2/6. The rectangle has area adad, and its centroid is d/2d/2 from ECEC on the opposite side.

Since the combined centre of mass lies on ECEC, moments of areas about ECEC give

ad(d2)=πa26(aπ).ad\left(\frac d2\right)=\frac{\pi a^2}{6}\left(\frac a\pi\right).

Hence

ad22=a36,a2=3d2.\frac{ad^2}{2}=\frac{a^3}{6},\qquad a^2=3d^2.

Since a,d>0a,d>0,

a=3d.\boxed{a=\sqrt3d}.

(b)

解法一

思路

展开

先求组合质心到 BCBC 的距离。扇形质心距 BCBC 是沿 ECEC 方向的投影,与上一问距 ECEC 的投影不同。悬挂平衡时,悬点到质心的连线竖直向下,所求角等于 BCBC 与该连线的夹角。

答题过程

展开

Let GG be the centre of mass and let its distance from BCBC be yy. The rectangular centroid is at distance a/2a/2 from BCBC. The sector centroid is at distance

2aπcos⁡π6=3aπ\frac{2a}{\pi}\cos\frac\pi6=\frac{\sqrt3a}{\pi}

from BCBC.

Using d=a/3d=a/\sqrt3 and taking moments of areas about BCBC,

(a23+πa26)y=a23(a2)+πa26(3aπ).\left(\frac{a^2}{\sqrt3}+\frac{\pi a^2}{6}\right)y=\frac{a^2}{\sqrt3}\left(\frac a2\right)+\frac{\pi a^2}{6}\left(\frac{\sqrt3a}{\pi}\right).

Simplifying,

y=6a6+3π.y=\frac{6a}{6+\sqrt3\pi}.

Also GG lies on ECEC, so its perpendicular distance from the line BCBC is yy, and its distance along BCBC from BB is dd.

When the lamina hangs freely from BB, BGBG is vertically downwards. Therefore

tan⁡β=yd=636+3π.\tan\beta=\frac yd=\frac{6\sqrt3}{6+\sqrt3\pi}.

Hence

β=0.737 radians.\boxed{\beta=0.737\text{ radians}}.