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M1 2019 Oct Q4

A Level / Edexcel / M1

IAL 2019 Oct Paper · Question 4

题目

Problem

4.

A particle, PP, of mass kmkm lies on a fixed rough plane. The plane is inclined to the horizontal at an acute angle θ\theta. A horizontal force of magnitude XX acts on PP, as shown in Figure 1. The line of action of the force lies in the vertical plane which contains the line of greatest slope of the inclined plane that passes through PP. The coefficient of friction between PP and the inclined plane is μ\mu.

When X=mgX=mg, the particle PP is in equilibrium and on the point of sliding down the plane.

(a) Show that

μ=ktan⁡θ−1k+tan⁡θ\mu=\frac{k\tan\theta-1}{k+\tan\theta}
(10)

(b) Deduce that, when k=1k=1, θ\theta must be greater than 45∘45^\circ.

(2)
题目中文翻译

一个质量为 kmkm 的质点 PP 位于固定粗糙斜面上。斜面与水平面成锐角 θ\theta。如图 1 所示,一个大小为 XX 的水平力作用在 PP 上。该力的作用线位于包含经过 PP 点的斜面最大坡度线的竖直平面内。PP 与斜面之间的摩擦系数为 μ\mu。

当 X=mgX=mg 时,质点 PP 处于平衡状态,且恰好要沿斜面向下滑动。

(a) 证明

μ=ktan⁡θ−1k+tan⁡θ\mu=\frac{k\tan\theta-1}{k+\tan\theta}
(10)

(b) 推断:当 k=1k=1 时,θ\theta 必须大于 45∘45^\circ。

(2)

解答

(a)

解法一

思路

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将要向下滑,所以摩擦力沿斜面向上且达到极限值。水平推力不仅有沿斜面向上的分量,也有压向斜面的分量。消去支持力与摩擦力后,再把正弦余弦之比化成正切。

答题过程

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Let the normal reaction be RR and the limiting friction be FF. Since the particle is about to slide down, FF acts up the plane and F=μRF=\mu R.

Resolving perpendicular to the plane, with X=mgX=mg,

R=kmgcos⁡θ+mgsin⁡θ.R=kmg\cos\theta+mg\sin\theta.

Resolving parallel to the plane,

F+mgcos⁡θ=kmgsin⁡θ,F+mg\cos\theta=kmg\sin\theta,

so

F=mg(ksin⁡θ−cos⁡θ).F=mg(k\sin\theta-\cos\theta).

Using F=μRF=\mu R and cancelling mgmg gives

μ(kcos⁡θ+sin⁡θ)=ksin⁡θ−cos⁡θ.\mu(k\cos\theta+\sin\theta)=k\sin\theta-\cos\theta.

As θ\theta is acute, cos⁡θ>0\cos\theta>0. Dividing numerator and denominator by cos⁡θ\cos\theta,

μ= ksin⁡θ−cos⁡θkcos⁡θ+sin⁡θ= ksin⁡θ/cos⁡θ−1k+sin⁡θ/cos⁡θ= ktan⁡θ−1k+tan⁡θ.\begin{align*} \mu=&\,\frac{k\sin\theta-\cos\theta}{k\cos\theta+\sin\theta}\\[4mm] =&\,\frac{k\sin\theta/\cos\theta-1}{k+\sin\theta/\cos\theta}\\[4mm] =&\,\boxed{\frac{k\tan\theta-1}{k+\tan\theta}}. \end{align*}

解法二

思路

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也能沿水平和竖直方向分解。支持力指向左上方,摩擦力沿斜面指向右上方;用极限摩擦关系先消去两个力,再整理。

答题过程

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Let RR be the normal reaction and F=μRF=\mu R the limiting friction up the plane. Horizontal and vertical equilibrium give

mg+Fcos⁡θ=Rsin⁡θ,mg+F\cos\theta=R\sin\theta, Rcos⁡θ+Fsin⁡θ=kmg.R\cos\theta+F\sin\theta=kmg.

Substituting F=μRF=\mu R,

mg=R(sin⁡θ−μcos⁡θ),mg=R(\sin\theta-\mu\cos\theta), kmg=R(cos⁡θ+μsin⁡θ).kmg=R(\cos\theta+\mu\sin\theta).

Multiply the first equation by kk and compare with the second. Cancelling the positive reaction RR gives

ksin⁡θ−kμcos⁡θ=cos⁡θ+μsin⁡θ.k\sin\theta-k\mu\cos\theta=\cos\theta+\mu\sin\theta.

Collecting terms in μ\mu,

μ(kcos⁡θ+sin⁡θ)=ksin⁡θ−cos⁡θ.\mu(k\cos\theta+\sin\theta)=k\sin\theta-\cos\theta.

Dividing through and then dividing numerator and denominator by cos⁡θ>0\cos\theta>0,

μ=ksin⁡θ/cos⁡θ−1k+sin⁡θ/cos⁡θ=ktan⁡θ−1k+tan⁡θ.\mu=\frac{k\sin\theta/\cos\theta-1}{k+\sin\theta/\cos\theta} =\boxed{\frac{k\tan\theta-1}{k+\tan\theta}}.

(b)

解法一

思路

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粗糙斜面有 μ>0\mu>0。代入 k=1k=1 后,先确认分母为正,再推出分子必须为正;锐角区间内正切单调递增。

答题过程

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Putting k=1k=1 in (a),

μ=tan⁡θ−11+tan⁡θ>0.\mu=\frac{\tan\theta-1}{1+\tan\theta}>0.

Since 0<θ<90∘0<\theta<90^\circ, the denominator is positive. Therefore

tan⁡θ−1>0,tan⁡θ>1=tan⁡45∘.\tan\theta-1>0, \qquad \tan\theta>1=\tan45^\circ.

Hence θ>45∘\boxed{\theta>45^\circ}.