题目
A particle is moving on a fixed smooth horizontal surface with speed . The particle collides with a fixed smooth vertical barrier. Immediately before the collision, the direction of motion of makes an angle with the barrier, where .
The kinetic energy of after the collision is times its kinetic energy before the collision.
(a) Find the coefficient of restitution between and the barrier.
(b) A second smooth vertical barrier is fixed to the surface and to the first barrier. The angle between the two barriers is . Particle subsequently collides with the second barrier and rebounds immediately after with speed at an angle with the second barrier. The coefficient of restitution is the same as in the first collision.
Find the value of correct to significant figures.
题目中文翻译
质点 以速率 在一个固定的光滑水平面上运动。质点与一个固定的光滑竖直挡板碰撞。碰撞前一瞬间, 的运动方向与挡板成 角,其中 。
碰撞后 的动能是碰撞前动能的 倍。
(a) 求 与挡板之间的恢复系数。
(b) 第二个光滑竖直挡板固定于该水平面及第一个挡板上。两个挡板之间的夹角为 。质点 随后与第二个挡板碰撞,碰撞后立即以速率 弹回,运动方向与第二个挡板成 角。恢复系数与第一次碰撞时相同。
求 的值,保留 位有效数字。
原卷通用作答要求
Answer all questions. You should use a calculator where appropriate.
You must show all necessary working clearly; no marks will be given for unsupported answers from a calculator.
Give non-exact numerical answers correct to 3 significant figures, or 1 decimal place for angles in degrees, unless a different level of accuracy is specified in the question.
请回答所有题目。适当时应使用计算器。必须清楚展示所有必要的计算过程;仅给出计算器答案而没有过程,不予评分。除非题目另有精度要求,非精确数值答案保留 3 位有效数字,以度为单位的角度保留 1 位小数。
Where a numerical value for the acceleration due to gravity () is needed, use .
需要使用重力加速度 的数值时,取 。
解答
(a)
解法一
思路
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平行于障碍物的分量不变,垂直分量反向并乘恢复系数 。用两分量的平方和表示碰后动能比。
答题过程
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The given tangent gives and . After impact, the parallel component is and the normal component has magnitude . The kinetic energy ratio therefore gives
Thus , giving and . The non-negative coefficient is .
(b)
解法一
思路
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第一次反弹后,先求运动方向与第一面障碍物的夹角。两障碍物之间是 ,所以在第二面入射时,与它的锐角为 减去前一个夹角。第二次碰撞把这个角的正切乘 。
答题过程
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Let be the angle of the first rebound to the first barrier. Then
The path between the barriers and the two barrier segments form a triangle with angle at their meeting point. Thus the angle of approach to the second barrier is . The compound-angle formula gives
At the second collision, the normal component is multiplied in magnitude by and the parallel component is unchanged. If is the speed between the barriers, then and . Dividing gives , so to three significant figures.