题目
2.
A car of mass tows a trailer of mass up a hill along a straight road that is inclined at angle to the horizontal, where . The trailer is attached to the car by a light inextensible towbar. The resistance to the motion of the car from non-gravitational forces is modelled as a constant force of magnitude . The resistance to the motion of the trailer from non-gravitational forces is modelled as a constant force of magnitude .
When the engine of the car is working at a constant rate of the car and the trailer have a constant speed of
(a) Find the value of .
Later, at the instant when the car and the trailer are travelling up the hill with a speed of , the towbar breaks. When the towbar breaks the trailer is at the point . The trailer continues to travel up the hill before coming to instantaneous rest at the point . The resistance to the motion of the trailer from non-gravitational forces is again modelled as a constant force of magnitude .
(b) Use the work-energy principle to find the distance .
题目中文翻译
质量为 的汽车牵引质量为 的拖车,沿一条与水平面成 角的直路上坡,其中 。拖车通过不可伸长的轻牵引杆与汽车连接。将汽车所受的非重力运动阻力视为大小为 的恒力,将拖车所受的非重力运动阻力视为大小为 的恒力。
当汽车发动机以恒定功率 工作时,汽车与拖车以恒定速率 行驶。
(a) 求 的值。
后来,在汽车与拖车以速率 上坡的瞬间,牵引杆断裂。断裂时拖车位于 点。拖车继续上坡,直至在 点瞬时静止。 仍将拖车所受的非重力运动阻力视为大小为 的恒力。
(b) 利用功—能原理求距离 。
解答
(a)
解法一
思路
展开
把汽车与拖车视为整体可消去牵引杆内力。匀速时牵引力平衡两项阻力及两车的下坡重力分量,最后把瓦换成千瓦。
答题过程
展开
Let the driving force be N. Resolving up the road for the car and trailer together, with zero acceleration,
Hence
The power is , so
Therefore
(b)
解法一
思路
展开
断杆后只研究拖车。它最初以 运动,动能用于克服 牛顿阻力及增加重力势能;本问必须使用功—能原理。
答题过程
展开
Let metres. After the towbar breaks there is no towing force on the trailer. Its loss of kinetic energy equals its gain in gravitational potential energy plus the work done against resistance:
Thus
Therefore