Motion in a straight line
Theory
Motion in a straight line is analysed with calculus. Differentiate the displacement \(x(t)\) once for the velocity \(v=\dfrac{dx}{dt}\) and again for the acceleration \(a=\dfrac{dv}{dt}=\dfrac{d^{2}x}{dt^{2}}\). The sign of \(v\) gives the direction, \(v=0\) marks where the particle is momentarily at rest, and the sign of \(v\,a\) tells you whether it is speeding up or slowing down.
For a particle moving on a straight line, its displacement \(x\) (its signed position from a fixed origin \(O\)) is a function of time \(t\). Its motion is described by two derivatives:
Velocity is the rate of change of displacement, \(v=\dfrac{dx}{dt}\). Its sign gives the direction of motion; its size \(|v|\) is the speed.
Acceleration is the rate of change of velocity, \(a=\dfrac{dv}{dt}=\dfrac{d^{2}x}{dt^{2}}\) — the second derivative of displacement.
The particle is momentarily at rest when \(v=0\); it is moving in the positive direction when \(v>0\) and the negative direction when \(v<0\). It is speeding up when \(v\) and \(a\) share a sign and slowing down when they have opposite signs.
Velocity and acceleration from displacement \(x(t)\):
Reading the motion from the signs:
Turning points of the motion (for maxima/minima):
How to analyse straight-line motion
- Differentiate. From \(x(t)\), find \(v=\dfrac{dx}{dt}\) and \(a=\dfrac{dv}{dt}\). Evaluate at a required time by substitution.
- At rest. Solve \(v=0\) for the time(s); substitute back into \(x\) or \(a\) for the position or acceleration then.
- Direction. Read the sign of \(v\): positive means the positive direction, negative means the negative direction.
- Speeding up or slowing down. Compare the signs of \(v\) and \(a\): same sign \(\Rightarrow\) speeding up; opposite signs \(\Rightarrow\) slowing down.
- Maxima/minima. For greatest displacement solve \(v=0\); for greatest/least velocity solve \(a=0\). Confirm with a second-derivative or sign test and check any interval endpoints.
| \(v=\dfrac{dx}{dt}\) | \(=\) | \(6t^{2}-6t\) |
| \(v(2)\) | \(=\) | \(6(2)^{2}-6(2)\) |
| \(=\) | \(24-12\) | |
| \(=\) | \(12\) |
| \(v=\dfrac{dx}{dt}\) | \(=\) | \(3t^{2}-12t+9\) |
| \(3t^{2}-12t+9\) | \(=\) | \(0\) |
| \(3(t-1)(t-3)\) | \(=\) | \(0\) |
| \(t\) | \(=\) | \(1\) or \(3\) s |
| \(v=\dfrac{dx}{dt}\) | \(=\) | \(3t^{2}-6t-9\) |
| \(a=\dfrac{dv}{dt}\) | \(=\) | \(6t-6\) |
| \(v(2)\) | \(=\) | \(3(2)^{2}-6(2)-9\) |
| \(=\) | \(12-12-9=-9\) | |
| \(a(2)\) | \(=\) | \(6(2)-6\) |
| \(=\) | \(6\) |
| \(v\,a\) | \(=\) | \((-9)(6)\) |
| \(=\) | \(-54\) |
| \(v=\dfrac{dx}{dt}\) | \(=\) | \(3t^{2}-12t+9\) |
| \(=\) | \(3(t-1)(t-3)\) | |
| \(v=0\) | \(\Rightarrow\) | \(t=1\) or \(t=3\) |
| \(a(1)\) | \(=\) | \(6(1)-12\) |
| \(=\) | \(-6<0\) (maximum) |
| \(x(1)\) | \(=\) | \((1)^{3}-6(1)^{2}+9(1)\) |
| \(=\) | \(1-6+9\) | |
| \(=\) | \(4\) |
| \(x(0)\) | \(=\) | \(0\) |
| \(x(3)\) | \(=\) | \(27-54+27=0\) |
Common pitfalls
Frequently asked questions
How do you find velocity and acceleration from displacement?
Differentiate: \(v=\dfrac{dx}{dt}\) (once) and \(a=\dfrac{dv}{dt}=\dfrac{d^{2}x}{dt^{2}}\) (twice), then substitute the required time.
When is a particle momentarily at rest?
When \(v=0\). Set the velocity to zero and solve for \(t\); the particle stops there before changing direction.
How do you tell which direction a particle is moving?
By the sign of \(v\): \(v>0\) is the positive direction, \(v<0\) the negative direction, \(v=0\) momentarily at rest.
What is the difference between speeding up and slowing down?
Speeding up: \(v\) and \(a\) have the same sign (\(v\,a>0\)). Slowing down: opposite signs (\(v\,a<0\)).
How do you find the maximum displacement or velocity?
Maximum displacement is where \(v=0\); maximum/minimum velocity is where \(a=0\). Confirm with a second-derivative test and check the interval endpoints.
What is the difference between distance and displacement?
Displacement is the signed change in position; distance is the total path length. When the particle reverses, add the distances between successive rest positions.