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Chapter 2 -1 Dimensional Motion

Reference Frames

When we consider motion we always consider the motion of objects in a reference frame, or coordinate system. An appropriate choice of coordinate system can help enormously in solving a problem.

Unit Vectors

It can be useful to express vector quantities in terms of unit vectors. These are dimensionless vectors of length = 1 that point along the coordinate axes. They are usually denoted with carets (hats), i.e. $(\hat{i},\hat{j},\hat{k})$

For example:

$\vec{v}\,\mathrm{ms^{-1}}=v_{x}\,\mathrm{ms^{-1}}\,\hat{i}+v_{y}\,\mathrm{ms^{-1}}\,\hat{j}+v_{z}\,\mathrm{ms^{-1}}\,\hat{k}$

or

$\vec{r}\,\mathrm{m}=x\,\mathrm{m}\,\hat{i}+y\,\mathrm{m}\,\hat{j}+z\,\mathrm{m}\,\hat{k}$

Displacement

We need a quantity to express the position of an object. The displacement of an object is a vector which points from the origin of the coordinate system to the object. For now we'll deal with 1 dimensional displacement.

We should also consider the relative displacement of one object from another, or of an object from a position it occupied at an earlier time.

Note that the displacement of an object is not necessarily the same as the distance it has traveled!

Average Velocity

If we denote the displacement from a point at time $t_{1}$ as $x_{1}$ and at time $t_{2}$ as $x_{2}$ the change in the displacement in the time interval $\Delta t=t_{2}-t_{1}$ is $\Delta x = x_{2}-x_{1}$.

The average velocity in this time interval is

$\large \bar{v}=\frac{\Delta x}{\Delta t}$

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Instantaneous Velocity

The instantaneous velocity is found by taking the limit as $\Delta t\to 0$

$\large v=^\lim_{\Delta t\to0} \frac{\Delta x}{\Delta t}=\frac{dx}{dt}$

Note that the velocity is the slope of the interval, not the length of the arrow!

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Acceleration

In the same way as velocity is the rate of change of displacement acceleration is the rate of change of velocity

Average acceleration is

$\large \bar{a}=\frac{\Delta v}{\Delta t}$

The instantaneous acceleration is found by taking the limit as $\Delta t\to 0$

$\large a=^\lim_{\Delta t\to0} \frac{\Delta v}{\Delta t}=\frac{dv}{dt}=\frac{d^2x}{dt^2}$

Accelerometers

Most smartphones include accelerometers to be able to detect motion and there are apps available which provide access to their readouts.

We can see that the accelerometer measures the acceleration due to gravity. Many smartphones and tablets now add, in addition to the accelerometer, a gyroscope which can determine which direction is down and compensate for the acceleration due to gravity. You can try loading this link on your device and you will get a plot for the acceleration of the three axes of the phone against time (if your device has the necessary sensors).

Movement in different reference frames

In classical physics we can easily transform the displacement, velocity and acceleration from one reference frame to another, using Galilean transformations (i.e. just subtract the motion of the reference frame from the motion of the object.)

For example, if I am running at 10km/h (relative to a stationary observer), past someone who is running at 9km/h, my relative velocity to the other person, or, my velocity in their reference frame is 10km/h - 9km/h = 1 km/h.

We should be mindful that all these quantities are vectors, we will later learn how to deal with relative motion in more than one dimension.

Relativity, which we will not be covering in this course, results in a different set of transformations, because in this theory light moves at the same speed in all reference frames. At speeds much less than the speed of light the mathematical limits of relativistic transformations are the same as the Galilean transformations.

Equations of motion for constant acceleration

These three equations will be very important in this course. Make sure you know how to use them correctly! They apply only when the acceleration $a$ is a constant that does not change with time $t$. In these equations a variable with a subscript 0 refers to the value of that quantity at time $t=0$.

$\large v= v_{0}+at$

$\large x= x_{0}+v_{0}t+\frac{1}{2}at^2$

$\large v^{2}=v_{0}^2+2a(x-x_{0})$

Equations of motion using calculus

If the acceleration is a constant $a$ which does not change with time then we can say at a time $t$

$\int^{v}_{v_0}\,dv= v(t)-v_0=\int^{t}_0 a\,dt = at$ where $v_{0}$ is the velocity at $t=0$.

so $v= v_{0}+at$

and similarly

$\int^{x}_{x_0}\,dx= x(t)-x_0=\int^{t}_{0} v\,dt = v_{0}t+\frac{1}{2}at^2$

so $x= x_{0}+v_{0}t+\frac{1}{2}at^2$

Equation of motion without time

To find a relation between acceleration and velocity that does not include time

$\large a=\frac{dv}{dt}=\frac{dv}{dx}\frac{dx}{dt}=v\frac{dv}{dx}$

$\large \int^{x}_{x_{0}}a\,dx=\int^{v}_{v_{0}}v\,dv$

$\large a(x-x_{0})=\frac{1}{2}(v^2-v_{0}^2)$

$\large v^{2}=v_{0}^2+2a(x-x_{0})$

Equations of motion

As you can see the equations of motion are simply a result of calculus!

$\large v= v_{0}+at$

$\large x= x_{0}+v_{0}t+\frac{1}{2}at^2$

$\large v^{2}=v_{0}^2+2a(x-x_{0})$

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Objects in free fall

Galileo made a remarkable observation that close to the Earth the acceleration due to gravity is a constant for all objects. Therefore in the absence of air resistance freely falling objects are well described by the equations of motion we just derived.

His observation was especially remarkable given his lack of accurate measurement tools. Today we can do actually do extremely accurate measurements with everyday devices that you may already own!

Video analysis of free fall

By taking a video of a freely falling object and processing it so that we can see the position of the object in each frame (which at 30 frames per second is every 0.033 seconds) we can analysis the motion of the object. The tool to do this is here.

As well as using video frames as we did it is also possible to use sound to measure the time taken for objects to fall. This approach is nicely illustrated at Physclips (Section 2.2)

phy131studiof15/lectures/chapter2.1438026771.txt · Last modified: 2015/07/27 15:52 by mdawber
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