1.6.2 Acceleration

We named the first derivative of a parameterized curve the velocity of the curve (and its length was the speed of the curve). The derivative of the velocity also gets a name - the [color=#ff0000][b]acceleration[/b] [/color]of the path.[br][br]The GeoGebra applet below shows that the acceleration vector always lies in the osculating plane. Experiment with different curves - try a curve with no curvature or one with constant curvature.
In the language of linear algebra, this means the acceleration vector is always a linear combination of the unit normal and unit tangent vectors. Prove it.
It's shown in the text that there are alternate ways to compute the tangential and normal components of acceleration. [br][br][math]a_T=\frac{\vec{a}\cdot\vec{v}}{v}[/math][br][math]a_N=\frac{\left|\left|\vec{a}\times\vec{v}\right|\right|}{v}=\sqrt{\left|\left|\vec{a}\right|\right|^2-\left|a_T\right|^2}[/math]
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Information: 1.6.2 Acceleration