Skip to content
CalcGospel 國際數學圖譜
返回

M3 2020 Oct Q4

A Level / Edexcel / M3

IAL 2020 Oct Paper · Question 4

题目

Problem

4.

(a) Use algebraic integration to show that the centre of mass of a uniform solid hemisphere of radius aa is a distance 38a\dfrac38a from the centre of its plane face.

[You may assume that the volume of a sphere of radius rr is 43πr3\dfrac43\pi r^3.]

(5)

A uniform solid hemisphere has mass mm and radius aa. A particle of mass kmkm is attached to a point AA on the circumference of the plane face of the hemisphere to form the loaded solid SS. The centre of the plane face of the hemisphere is the point OO, as shown in Figure 4.

The loaded solid SS is placed on a horizontal plane. The curved surface of SS is in contact with the plane and SS rests in equilibrium with OAOA making an angle α\alpha with the horizontal, where tan⁡α=3\tan\alpha=\sqrt3

(b) Find the exact value of kk.

(5)
题目中文翻译

(a) 用代数积分证明:半径为 aa 的均匀实心半球的质心到其平面面的圆心的距离为 38a\dfrac38a。

[ 可直接使用半径为 rr 的球的体积为 43πr3\dfrac43\pi r^3。 ]

(5)

一个均匀实心半球的质量为 mm,半径为 aa。将一个质量为 kmkm 的质点连接于半球平面面的圆周上的 AA 点,形成加载物体 SS。如图 4 所示,半球平面面的圆心为 OO。

将加载物体 SS 放在水平面上,SS 的曲面与水平面接触。SS 处于平衡,OAOA 与水平面成 α\alpha 角,其中 tan⁡α=3\tan\alpha=\sqrt3。

(b) 求 kk 的精确值。

(5)

解答

(a)

解法一

思路

展开

将实心半球沿对称轴切成薄圆盘。用圆盘质量乘轴向位置作质量矩积分,再除以整个半球质量;这里不是半圆薄片的质心公式。

答题过程

展开

Take the origin at the centre of the plane face, and let yy measure distance into the hemisphere along its symmetry axis, with 0≤y≤a0\leq y\leq a. A thin disc at coordinate yy has radius satisfying

r2=a2−y2.r^2=a^2-y^2.

For constant density ρ\rho, its mass is

dm=ρπ(a2−y2) dy.\mathrm{d}m=\rho\pi(a^2-y^2)\,\mathrm{d}y.

The hemisphere has mass

M=ρ(12⋅43πa3)=23ρπa3.M=\rho\left(\frac12\cdot\frac43\pi a^3\right)=\frac23\rho\pi a^3.

By symmetry its centre of mass lies on the axis. Taking mass moments about the plane face,

Myˉ=∫0ay dm=ρπ∫0a(a2y−y3) dy.M\bar y=\int_0^a y\,\mathrm{d}m=\rho\pi\int_0^a(a^2y-y^3)\,\mathrm{d}y.

Evaluating the integral,

Myˉ=ρπ[a2y22−y44]0a=14ρπa4.M\bar y=\rho\pi\left[\frac{a^2y^2}{2}-\frac{y^4}{4}\right]_0^a=\frac14\rho\pi a^4.

Therefore

yˉ=ρπa4/42ρπa3/3=38a.\bar y=\frac{\rho\pi a^4/4}{2\rho\pi a^3/3}=\boxed{\frac38a}.

(b)

解法一

思路

展开

平面支持力沿接触半径通过 O,所以绕 O 取矩时不出现支持力。半球重力和附重的力臂分别由半球轴向质心距离及 OA 的水平投影得到。

答题过程

展开

Let GG be the centre of mass of the hemisphere. Then OG=3a/8OG=3a/8, perpendicular to the plane face. The vertical normal reaction at the spherical contact point passes through OO, so it has zero moment about OO. Since OAOA makes angle α\alpha with the horizontal, the horizontal moment arms of the particle and hemisphere weights about OO are respectively

acos⁡αand3a8sin⁡α.a\cos\alpha\quad\text{and}\quad\frac{3a}{8}\sin\alpha.

These weights act on opposite sides of the vertical through OO. Taking moments about OO,

kmg(acos⁡α)=mg(3a8sin⁡α).kmg(a\cos\alpha)=mg\left(\frac{3a}{8}\sin\alpha\right).

Thus

k=38tan⁡α=338.k=\frac38\tan\alpha=\boxed{\frac{3\sqrt3}{8}}.

解法二

思路

展开

也可先求加载后整体质心相对于半球的两个分量,再要求整体质心位于 O 的正下方。

答题过程

展开

Use perpendicular axes fixed in the solid: xx along OAOA towards AA, and yy along the hemisphere’s axis into the solid. The hemisphere’s centre is at (0,3a/8)(0,3a/8) and the particle is at (a,0)(a,0). For the combined centre of mass,

(1+k)mxˉ=kma,(1+k)myˉ=m3a8.(1+k)m\bar x=kma,\qquad (1+k)m\bar y=m\frac{3a}{8}.

Therefore

xˉ=ka1+k,yˉ=3a8(1+k).\bar x=\frac{ka}{1+k},\qquad \bar y=\frac{3a}{8(1+k)}.

The normal reaction passes through OO, so equilibrium requires the combined centre of mass to be vertically below OO. When OAOA is inclined at α\alpha to the horizontal, cancellation of its horizontal component gives

xˉcos⁡α=yˉsin⁡α.\bar x\cos\alpha=\bar y\sin\alpha.

Consequently

tan⁡α=xˉyˉ=8k3,\tan\alpha=\frac{\bar x}{\bar y}=\frac{8k}{3}, k=338.\boxed{k=\frac{3\sqrt3}{8}}.