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M3 2026 June A Q7

A Level / Edexcel / M3

IAL 2026 June A Paper · Question 7

题目

Problem

7.

The fixed points AA and BB lie on a smooth horizontal surface with AB=10aAB=10a.

A particle PP has mass mm.

One end of a light elastic string, of natural length 5a5a and modulus of elasticity 13mg\dfrac13mg, is attached to PP and the other end is attached to AA.

One end of another light elastic string, of natural length 3a3a and modulus of elasticity 25mg\dfrac25mg, is attached to PP and the other end is attached to BB.

The particle PP is resting in equilibrium at the point EE on the surface, as shown in Figure 6.

(a) Show that EB=11a3EB=\dfrac{11a}3

(3)

Particle PP is now held on the surface at the point CC, between AA and BB, where CB=3aCB=3a, and released from rest.

(b) Show that PP moves with simple harmonic motion about EE.

(4)

(c) Show that the simple harmonic motion has period 2π5ag2\pi\sqrt{\dfrac{5a}g}

(2)

In any one complete oscillation of the simple harmonic motion, the particle is less than a distance 13a\dfrac13a from EE for a time SS.

(d) Find SS in terms of π\pi, aa and gg.

(3)
题目中文翻译

固定点 AA、BB 位于光滑水平面上,AB=10aAB=10a。

质点 PP 的质量为 mm。

一根原长为 5a5a、弹性模量为 13mg\dfrac13mg 的弹性轻绳的一端连接于 PP,另一端连接于 AA。

另一根原长为 3a3a、弹性模量为 25mg\dfrac25mg 的弹性轻绳的一端连接于 PP,另一端连接于 BB。

如图 6 所示,质点 PP 静止平衡于该平面上的 EE 点。

(a) 证明 EB=11a3EB=\dfrac{11a}3。

(3)

现在将质点 PP 保持在平面上位于 AA、BB 之间的 CC 点,其中 CB=3aCB=3a,然后由静止释放。

(b) 证明 PP 绕 EE 做简谐运动。

(4)

(c) 证明该简谐运动的周期为 2π5ag2\pi\sqrt{\dfrac{5a}g}。

(2)

任意一次完整简谐振动中,质点距 EE 小于 13a\dfrac13a 的持续时间为 SS。

(d) 用 π\pi、aa 和 gg 表示 SS。

(3)

解答

(a)

解法一

思路

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两个张力相等,但因原长和弹性模量不同,伸长量不相等。设右绳伸长为 ee,则左绳伸长为 2a−e2a-e,分别使用各自的胡克定律。

答题过程

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Let the extension of the string attached to BB be ee. Then

EB=3a+e,AE=10a−(3a+e)=7a−e,EB=3a+e,\qquad AE=10a-(3a+e)=7a-e,

so the extension of the string attached to AA is 2a−e2a-e. In horizontal equilibrium the tensions are equal:

(mg/3)(2a−e)5a=(2mg/5)e3a.\frac{(mg/3)(2a-e)}{5a}=\frac{(2mg/5)e}{3a}.

Multiplying by 15a/(mg)15a/(mg) gives

2a−e=2e⟹e=2a3.2a-e=2e\quad\Longrightarrow\quad e=\frac{2a}{3}.

Therefore

EB=3a+2a3=11a3,AE=19a3.\boxed{EB=3a+\frac{2a}{3}=\frac{11a}{3}}, \qquad AE=\frac{19a}{3}.

(b)

解法一

思路

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取从 EE 向 BB 的位移为正,分别写两根绳随位移变化的伸长,合力为右张力减左张力。还要检查释放后的振幅范围是否导致绳出现一段松弛运动。

答题过程

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Let xx be the displacement from EE towards BB. The extensions of the left and right strings are respectively

19a3+x−5a=4a3+x,11a3−x−3a=2a3−x.\frac{19a}{3}+x-5a=\frac{4a}{3}+x, \qquad \frac{11a}{3}-x-3a=\frac{2a}{3}-x.

Taking towards BB as positive, Newton’s second law gives

mx¨=2mg15a(2a3−x)−mg15a(4a3+x).m\ddot x=\frac{2mg}{15a}\left(\frac{2a}{3}-x\right) -\frac{mg}{15a}\left(\frac{4a}{3}+x\right).

The constant terms cancel:

mx¨=4mg45−2mg15ax−4mg45−mg15ax=−mg5ax.m\ddot x=\frac{4mg}{45}-\frac{2mg}{15a}x -\frac{4mg}{45}-\frac{mg}{15a}x =-\frac{mg}{5a}x.

Hence

x¨=−g5ax.\boxed{\ddot x=-\frac{g}{5a}x}.

The acceleration is proportional to the displacement from EE and directed towards EE, so the motion is SHM with ω2=g/(5a)\omega^2=g/(5a).

The release point has CB=3aCB=3a, so

EC=EB−CB=2a3.EC=EB-CB=\frac{2a}{3}.

Thus the amplitude is 2a/32a/3. Throughout −2a/3≤x≤2a/3-2a/3\le x\le2a/3, the left extension is at least 2a/3>02a/3>0, and the right extension is nonnegative. The right string is at natural length only at the release endpoint; the resultant force there is towards EE, so it immediately stretches again. There is no interval of slack-string motion, and the SHM equation applies throughout the oscillation.

(c)

解法一

思路

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从恢复加速度的系数读取角频率,再用 2π/ω2\pi/\omega 求周期。

答题过程

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From (b),

ω=g5a.\omega=\sqrt{\frac{g}{5a}}.

Therefore the period is

T=2πω=2π5ag.\boxed{\mathcal T=\frac{2\pi}{\omega}=2\pi\sqrt{\frac{5a}{g}}}.

(d)

解法一

思路

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半径为 a/3a/3 的中心区间,其边界恰好是半振幅。重设过中心的时刻为零,求中心到边界的时间;一周期累计四段,而不是只算首次到达。

答题过程

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The amplitude is b=2a/3b=2a/3. Reset time to τ=0\tau=0 when the particle passes through EE towards BB. Then

x=bsin⁡ωτ.x=b\sin\omega\tau.

The first arrival at x=a/3=b/2x=a/3=b/2 satisfies

sin⁡ωτ=12,ωτ=π6,τ=π65ag.\sin\omega\tau=\frac12, \qquad \omega\tau=\frac\pi6, \qquad \tau=\frac\pi6\sqrt{\frac{5a}{g}}.

There are two passages through ∣x∣<a/3|x|<a/3 in a complete oscillation, each with equal times on either side of EE. Thus the total duration is four times the time just found:

S=4τ=2π35ag.\boxed{S=4\tau=\frac{2\pi}{3}\sqrt{\frac{5a}{g}}}.

The isolated instants at the two boundary positions do not affect this duration.