Linear motion

The motion in which all the particles of a body move through the same distance in the same time is called translatory motion. There are two types of translatory motions: rectilinear motion; curvilinear motion. Since linear motion is a motion in a single dimension, the distance traveled by an object in particular direction is the same as displacement.[4] The SI unit of displacement is the metre.[5][6] If ${\displaystyle x_{1}}$ is the initial position of an object and ${\displaystyle x_{2}}$ is the final position, then mathematically the displacement is given by:

$${\displaystyle \Delta x=x_{2}-x_{1}}$$

The equivalent of displacement in rotational motion is the angular displacement ${\displaystyle \theta }$ measured in radians. The displacement of an object cannot be greater than the distance because it is also a distance but the shortest one. Consider a person travelling to work daily. Overall displacement when he returns home is zero, since the person ends up back where he started, but the distance travelled is clearly not zero.

Velocity refers to a displacement in one direction with respect to an interval of time. It is defined as the rate of change of displacement over change in time.[7] Velocity is a vector quantity, representing a direction and a magnitude of movement. The magnitude of a velocity is called speed. The SI unit of speed is ${\displaystyle {\text{m}}\cdot {\text{s}}^{-1},}$ that is metre per second.[6]

The average velocity of a moving body is its total displacement divided by the total time needed to reach a body from the initial point to the final point. It is an estimated velocity for a distance to travel. Mathematically, it is given by:[8][9]

$${\displaystyle \mathbf {v} _{\text{avg}}={\frac {\Delta \mathbf {x} }{\Delta t}}={\frac {\mathbf {x} _{2}-\mathbf {x} _{1}}{t_{2}-t_{1}}}}$$

where:

• ${\displaystyle t_{1}}$ is the time at which the object was at position ${\displaystyle \mathbf {x} _{1}}$ and
• ${\displaystyle t_{2}}$ is the time at which the object was at position ${\displaystyle \mathbf {x} _{2}}$

The magnitude of the average velocity ${\displaystyle \left|\mathbf {v} _{\text{avg}}\right|}$ is called an average speed.

In contrast to an average velocity, referring to the overall motion in a finite time interval, the instantaneous velocity of an object describes the state of motion at a specific point in time. It is defined by letting the length of the time interval ${\displaystyle \Delta t}$ tend to zero, that is, the velocity is the time derivative of the displacement as a function of time.

$${\displaystyle \mathbf {v} =\lim _{\Delta t\to 0}{\frac {\Delta \mathbf {x} }{\Delta t}}={\frac {d\mathbf {x} }{dt}}.}$$

The magnitude of the instantaneous velocity ${\displaystyle |\mathbf {v} |}$ is called the instantaneous speed.The instantaneous velocity equation comes from finding the limit as t approaches 0 of the average velocity. The instantaneous velocity shows the position function with respect to time. From the instantaneous velocity the instantaneous speed can be derived by getting the magnitude of the instantaneous velocity.

Acceleration is defined as the rate of change of velocity with respect to time. Acceleration is the second derivative of displacement i.e. acceleration can be found by differentiating position with respect to time twice or differentiating velocity with respect to time once.[10] The SI unit of acceleration is ${\displaystyle \mathrm {m\cdot s^{-2}} }$ or metre per second squared.[6]

If ${\displaystyle \mathbf {a} _{\text{avg}}}$ is the average acceleration and ${\displaystyle \Delta \mathbf {v} =\mathbf {v} _{2}-\mathbf {v} _{1}}$ is the change in velocity over the time interval ${\displaystyle \Delta t}$ then mathematically,

$${\displaystyle \mathbf {a} _{\text{avg}}={\frac {\Delta \mathbf {v} }{\Delta t}}={\frac {\mathbf {v} _{2}-\mathbf {v} _{1}}{t_{2}-t_{1}}}}$$

The instantaneous acceleration is the limit, as ${\displaystyle \Delta t}$ approaches zero, of the ratio ${\displaystyle \Delta \mathbf {v} }$ and ${\displaystyle \Delta t}$, i.e.,

$${\displaystyle \mathbf {a} =\lim _{\Delta t\to 0}{\frac {\Delta \mathbf {v} }{\Delta t}}={\frac {d\mathbf {v} }{dt}}={\frac {d^{2}\mathbf {x} }{dt^{2}}}}$$

The rate of change of acceleration, the third derivative of displacement is known as jerk.[11] The SI unit of jerk is ${\displaystyle \mathrm {m\cdot s^{-3}} }$. In the UK jerk is also referred to as jolt.

The rate of change of jerk, the fourth derivative of displacement is known as jounce.[11] The SI unit of jounce is ${\displaystyle \mathrm {m\cdot s^{-4}} }$ which can be pronounced as metres per quartic second.