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M2 2024 June Q3

A Level / Edexcel / M2

IAL 2024 June Paper · Question 3

题目

Problem

3.

A uniform circular disc CC has centre XX and radius RR.

A disc with centre YY and radius rr, where 0<r<R0<r<R and XY=R−rXY=R-r, is removed from CC to form the template shown shaded in Figure 1.

The centre of mass of the template is a distance krkr from XX.

(a) Show that r=k1−kRr=\frac{k}{1-k}R

(4)

(b) Hence find the range of possible values of kk.

(2)

The point PP is on the outer edge of the template and PXPX is perpendicular to XYXY.

The template is freely suspended from PP and hangs in equilibrium.

Given that k=49k=\frac49

(c) find the angle that XYXY makes with the vertical.

(3)

The mass of the template is MM.

(d) Find, in terms of MM, the mass of the lightest particle that could be attached to the template so that it would hang in equilibrium from PP with XYXY horizontal.

(3)
题目中文翻译

均匀圆片 CC 的圆心为 XX,半径为 RR。

从 CC 中挖去一个圆心为 YY、半径为 rr 的圆片,形成图 1 阴影所示的模板,其中 0<r<R0<r<R,且 XY=R−rXY=R-r。

模板质心到 XX 的距离为 krkr。

(a) 证明 r=k1−kRr=\frac{k}{1-k}R。

(4)

(b) 由此求 kk 的可能取值范围。

(2)

PP 点位于模板外边缘上,且 PXPX 垂直于 XYXY。

模板从 PP 点自由悬挂并处于平衡状态。

已知 k=49k=\frac49,

(c) 求 XYXY 与竖直方向所成的角。

(3)

模板的质量为 MM。

(d) 用 MM 表示可连接于模板、使其从 PP 点平衡悬挂且 XYXY 水平的最轻质点的质量。

(3)

解答

(a)

解法一

思路

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孔洞用负质量处理。剩余薄片的质心在远离洞的一侧,以 XX 为原点、指向 YY 为正,质心坐标应为 −kr-kr。再约去面积公因子,逐步推出给定式。

答题过程

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By symmetry the template’s centre of mass GG lies on XYXY, on the opposite side of XX from YY.

Let the mass per unit area be σ\sigma, and measure signed distances from XX towards YY as positive. The complete disc has mass σπR2\sigma\pi R^2 at coordinate 0; the removed disc has mass σπr2\sigma\pi r^2 at coordinate R−rR-r.

Taking moments of masses about an axis through XX,

σπR2(0)−σπr2(R−r)=σπ(R2−r2)(−kr).\sigma\pi R^2(0)-\sigma\pi r^2(R-r)=\sigma\pi(R^2-r^2)(-kr).

Cancelling σπ\sigma\pi and reversing signs,

r2(R−r)=kr(R2−r2).r^2(R-r)=kr(R^2-r^2).

Since 0<r<R0<r<R, both rr and R−rR-r are nonzero. Dividing by r(R−r)r(R-r) gives

r=k(R+r).r=k(R+r).

Hence

r(1−k)=kR,r(1-k)=kR,

and therefore

r=k1−kR.\boxed{r=\frac{k}{1-k}R}.

(b)

解法一

思路

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利用上一问的关系与 0<r<R0<r<R。先确定分母为正再处理不等式,两个端点都不能取。

答题过程

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From the relation obtained in (a),

k=rR+r.k=\frac{r}{R+r}.

Thus k>0k>0 and k<1k<1, so 1−k>01-k>0. Now r<Rr<R and (a) give

k1−kR<R.\frac{k}{1-k}R<R.

Dividing by R>0R>0 and multiplying by 1−k>01-k>0,

k<1−k,k<1-k,

so

0<k<12.\boxed{0<k<\frac12}.

(c)

解法一

思路

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悬挂时 PGPG 竖直。PXPX 与 XGXG 垂直,构成直角三角形;要求的是 XYXY 与竖直的角,所以正切是 PX/XGPX/XG,不是其倒数。

答题过程

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For k=4/9k=4/9, (a) gives

r=4/91−4/9R=45R.r=\frac{4/9}{1-4/9}R=\frac45R.

Hence

XG=kr=4945R=1645R.XG=kr=\frac49\frac45R=\frac{16}{45}R.

Since PX⊥XYPX\perp XY and GG lies on XYXY, triangle PXGPXG is right-angled at XX, with PX=RPX=R.

When suspended, PGPG is vertically downwards. If α\alpha is the smaller angle between XYXY and the vertical, then

tan⁡α=PXXG=R16R/45=4516.\tan\alpha=\frac{PX}{XG}=\frac{R}{16R/45}=\frac{45}{16}.

Therefore

α=70.4∘.\boxed{\alpha=70.4^\circ}.

(d)

解法一

思路

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让 XYXY 水平时,薄片重力对悬点的力臂为 krkr。为使附加质量最小,应在另一侧取得最大的水平力臂 RR;先说明这个最大值,再列力矩平衡。

答题过程

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With XYXY horizontal, the vertical through PP also passes through XX. The template’s weight MgMg has perpendicular distance

XG=1645RXG=\frac{16}{45}R

from this vertical.

Let the attached mass be m1m_1, at horizontal distance bb on the opposite side of XX from GG. Taking moments about PP,

m1gb=Mg(1645R).m_1gb=Mg\left(\frac{16}{45}R\right).

Every point of the template is within the original disc, so b≤Rb\le R. To minimise m1m_1, choose the largest possible distance b=Rb=R, at the farthest outer edge in the direction from XX towards YY.

Thus

m1gR=Mg(1645R),m_1gR=Mg\left(\frac{16}{45}R\right),

and the minimum mass is

m1=1645M.\boxed{m_1=\frac{16}{45}M}.