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M3 2022 Jan UNUSED Q4

A Level / Edexcel / M3

IAL 2022 Jan Unused Paper · Question 4

题目

Problem

4.

A uniform solid hemisphere HH has radius rr and centre OO

(a) Show that the centre of mass of HH is 3r8\dfrac{3r}8 from OO

[You may assume that the volume of HH is 2πr33\dfrac{2\pi r^3}3.]

(4)

A uniform solid SS, shown below in Figure 3, is formed by attaching a uniform solid right circular cylinder of height hh and radius rr to HH, so that one end of the cylinder coincides with the plane face of HH.

The point AA is the point on HH such that OA=rOA=r and OAOA is perpendicular to the plane face of HH

(b) Show that the distance of the centre of mass of SS from AA is

5r2+12rh+6h28r+12h\frac{5r^2+12rh+6h^2}{8r+12h}
(5)

The solid SS can rest in equilibrium on a horizontal plane with any point of the curved surface of the hemisphere in contact with the plane.

(c) Find rr in terms of hh.

(2)
题目中文翻译

均匀实心半球 HH 的半径为 rr,球心为 OO。

(a) 证明 HH 的质心到 OO 的距离为 3r8\dfrac{3r}8。

[ 可直接使用 HH 的体积为 2πr33\dfrac{2\pi r^3}3。 ]

(4)

将高为 hh、半径为 rr 的均匀实心正圆柱连接于 HH,使圆柱的一端与 HH 的平面面重合,形成下方图 3 所示的均匀立体 SS。

AA 是 HH 上满足 OA=rOA=r 且 OAOA 垂直于 HH 的平面面的点。

(b) 证明 SS 的质心到 AA 的距离为

5r2+12rh+6h28r+12h\frac{5r^2+12rh+6h^2}{8r+12h}
(5)

立体 SS 可在水平面上静止平衡,且半球曲面上的任意一点均可与该平面接触。

(c) 用 hh 表示 rr。

(2)

解答

(a)

解法一

思路

展开

沿半球轴从 O 向曲面量 x,把实心半球分成薄圆盘,积分求质量矩,再除以半球质量。

答题过程

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Measure xx along the symmetry axis from OO into the hemisphere. A disc at xx has radius r2−x2\sqrt{r^2-x^2}, so for uniform density ρ\rho,

dm=ρπ(r2−x2) dx,0≤x≤r.\mathrm{d}m=\rho\pi(r^2-x^2)\,\mathrm{d}x,\qquad 0\leq x\leq r.

The hemisphere’s mass is M=2ρπr3/3M=2\rho\pi r^3/3. Its centre of mass lies on the axis by symmetry, and

Mxˉ=ρπ∫0rx(r2−x2) dx.M\bar x=\rho\pi\int_0^r x(r^2-x^2)\,\mathrm{d}x.

Therefore

Mxˉ=ρπ[r2x22−x44]0r=14ρπr4,M\bar x=\rho\pi\left[\frac{r^2x^2}{2}-\frac{x^4}{4}\right]_0^r=\frac14\rho\pi r^4, xˉ=ρπr4/42ρπr3/3=3r8.\bar x=\frac{\rho\pi r^4/4}{2\rho\pi r^3/3}=\boxed{\frac{3r}{8}}.

(b)

解法一

思路

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均匀组合立体的质量比等于体积比。半球质心到 A 为 r−3r/8,圆柱质心到 A 为 r+h/2,再用质量加权平均。

答题过程

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Use distance along the axis from AA towards the cylinder. The hemisphere’s centre of mass is at distance

r−3r8=5r8r-\frac{3r}{8}=\frac{5r}{8}

from AA, while the cylinder’s centre of mass is at r+h/2r+h/2. Since the solid is uniform, the masses are proportional to the volumes 2πr3/32\pi r^3/3 and πr2h\pi r^2h. If the combined centre is at distance yˉ\bar y from AA,

(2πr33+πr2h)yˉ=2πr335r8+πr2h(r+h2).\left(\frac{2\pi r^3}{3}+\pi r^2h\right)\bar y=\frac{2\pi r^3}{3}\frac{5r}{8}+\pi r^2h\left(r+\frac h2\right).

Cancelling πr2\pi r^2,

(2r3+h)yˉ=5r212+rh+h22.\left(\frac{2r}{3}+h\right)\bar y=\frac{5r^2}{12}+rh+\frac{h^2}{2}.

Multiplying numerator and denominator by 1212 gives

yˉ=5r2+12rh+6h28r+12h.\boxed{\bar y=\frac{5r^2+12rh+6h^2}{8r+12h}}.

(c)

解法一

思路

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任意曲面接触点都能平衡,要求重心在球心 O:这样重力作用线始终与通过球心的支持力共线。将质心距 A 设为 r 后解正根。

答题过程

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At any spherical contact point, the normal reaction passes through OO. For equilibrium at every such orientation, the centre of mass must coincide with OO; otherwise some orientation produces a nonzero gravitational moment about the contact point. Thus yˉ=AO=r\bar y=AO=r, giving

r=5r2+12rh+6h28r+12h.r=\frac{5r^2+12rh+6h^2}{8r+12h}.

Therefore

8r2+12rh=5r2+12rh+6h2,8r^2+12rh=5r^2+12rh+6h^2, 3r2=6h2,r2=2h2.3r^2=6h^2,\qquad r^2=2h^2.

Since r,h>0r,h>0,

r=2 h.\boxed{r=\sqrt2\,h}.