Lecture 02b - Motion in One Dimension (The Equations of Motion)
Four equations for motion under constant acceleration:
Linear Equations | Missing |
---|---|
\(v = v_0 + at \) | \(s\) |
\(s - s_0 = v_0t + \frac{1}{2} a t^2 \) | \(v\) |
\(s - s_0 = \frac{1}{2} (v_0+v)t \) | \(a\) |
\(v^2 = v_0^2 + 2a(s-s_0) \) | \(t\) |
There are six variables overall: \(s_0, v_0 \) (intial variables), and \(s, v, a, t\) (final variables).
Each of the equations is labeled on the right by the final variables that is missing. For example, the first equation has the final variables \(v, a, t\) but is missing \(s\), so we will call it the \(s\)-equation.
The meaning of the variables:
Symbol | Meaning |
---|---|
\(s_0\) | initial displacement |
\( v_0 \) | initial velocity |
\(s\) | final displacement |
\( v \) | final velocity |
\(a\) | acceleration (constant) |
\( t \) | time |
If the acceleration is not a constant (i.e. it changes over time) then the equations are invalid. However, in this course, you can assume \(a\) is constant unless the question stated otherwise.
Gravity pulls everything downward in such a way that the vertical acceleration of an object falling on the surface of the Earth is given by: $$ a = -9.8m/s^2 $$ The negative sign denotes the fact that gravity always ponts downward. The value of \(a\) does not depend on the mass.