Acceleration of Point in Straight Line
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Theorem
Let $\mathbf a$ be the acceleration of a particle $P$ in space.
Let $P$ be moving along a straight line $\LL$ whose positive direction has been established.
Then the motion of $P$ can be defined by:
- $\mathbf a = \dfrac {\d^2 s} {\d t^2} \mathbf i$
where $\mathbf i$ denotes the unit vector in the positive direction of $\LL$.
Proof
We have by hypothesis that $P$ moves along a straight line $\LL$.
Then the rate of change of displacement perpendicular to $\LL$ is zero.
Let the $\LL$ be embedded in a Cartesian space $\CC$.
From the definition of the components of acceleration vector, we have:
- $\mathbf a = \dfrac {\d \mathbf v} {\d t} = \dfrac {\d^2 \mathbf r} {\d t^2}$
where:
- $\mathbf v$ is the velocity of $P$ at time $t$
- $\mathbf r$ is the displacement of $P$ at time $t$ expressed as a position vector from a given origin.
Thus:
- $\mathbf a = \dfrac {\d^2 x} {\d t^2} \mathbf i + \dfrac {\d^2 x} {\d t^2} \mathbf j + \dfrac {\d^2 x} {\d t^2} \mathbf k$
where:
- $\mathbf r = x \mathbf i + y \mathbf j + z \mathbf k$
Let us define $\CC$ such that $\LL$ is parallel to the $x$-axis of $\CC$.
Then we have:
\(\ds \mathbf v\) | \(=\) | \(\ds \dfrac {\d x} {\d t} \mathbf i + \dfrac {\d y} {\d t} \mathbf j + \dfrac {\d z} {\d t} \mathbf k\) | Definition of Velocity | |||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac {\d x} {\d t} \mathbf i + 0 \mathbf j + 0 \mathbf k\) | as the $y$-axis and $z$-axis are perpendicular to $\LL$ | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \mathbf a\) | \(=\) | \(\ds \dfrac {\d^2 x} {\d t} \mathbf i\) | Definition of Acceleration |
$\blacksquare$
Sources
- 1998: David Nelson: The Penguin Dictionary of Mathematics (2nd ed.) ... (previous) ... (next): acceleration
- 2008: David Nelson: The Penguin Dictionary of Mathematics (4th ed.) ... (previous) ... (next): acceleration