2.8

隐式求导

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$$\rightleftharpoonup{xx}$$ $$\longleftharp{xx}$$, $$\longrightharp{xx}$$,

在经典力学中,运动通常通过空间坐标与时间之间的关系来描述。例如,一辆汽车沿直线公路以恒定加速度行驶时,其速度可以表示为时间的显式函数。该情形可导出线性关系式,从而可以借助基本的求导方法进行较为直接的分析。

与此不同,处于圆形轨道上的卫星,其运动轨迹由隐式函数所刻画。卫星的位置受圆的方程所约束,该方程在…

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