A Physical Trig Identity

Can a basic physics problem give you insight into math?

For example, mathematically

$\cos(x) - \sin(x) = \sqrt{2}\cos(x + \pi/4)$

which is easy to verify using the angle addition formula.

I came across this formula while solving a simple problem in statics.

Imagine the classic “block on an inclined plane”. Gravity ( $F_g$ ) pulls the block down, and you push ( $F_p$ ) on it sideways, like this:

Gravity pulls down on the block and you push on it to the right.

What is the minimum coefficient of static friction to keep the block stationary? In order to calculate this, we need to know the component of force parallel to the plane.

First look at gravity. We want to find the green component $F_{g1}$ .

The force of gravity can be decomposed into two components. One points along the plane and the other is normal to it.

Let’s say the positive direction is to the right. Then gravity is pulling backwards some, so $F_{g1}$ is negative. I know it’s either a sine or cosine of $\theta$ , and in the limit as $\theta \to 0,$ I see that $F_{g1} = 0$ , so

$F_{g1} = -F_g \sin\theta$ .

Then we look at the pushing force.

The force from pushing is likewise decomposed.

A similar procedure gives

$F_{p1} = F_p \cos\theta$ .

So the total force in the direction of the ramp is

$-F_g \sin\theta + F_p \cos\theta$ .

In the special case where $F_g = F_p = 1$ the force is

$\cos\theta - \sin\theta$ .

Now we will find this component of the force another way. We start by tip-to-tail adding the force of gravity and the force of the push. They’re at right angles, and assuming they’re equal in magnitude we get a resultant force with length $\sqrt{2}$ that bisects the angle between the gravity and pushing forces.

We can also find the component of force along the plane by first adding the two vectors...

The angle between this resultant force and the plane is $\pi/4 + \theta$ .

...and then finding a component of the sum.

The component of this force along the plane is then the cosine of $\pi/4 + \theta$ , so the force along the direction of the plane is

$\sqrt{2} \cos(\pi/4 + \theta)$

and since it’s the same quantity we calculated before, we have

$\cos\theta - \sin\theta = \sqrt{2}\cos(\pi/4 + \theta)$ .

There is no physics in this calculation, but if you had simply asked me to write $\cos\theta-\sin\theta$ as a single trig function, I wouldn’t have thought to approach it like this.

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Tags: trigonometry, vectors

This entry was posted on September 6, 2010 at 3:10 pm and is filed under math, physics. You can follow any responses to this entry through the RSS 2.0 feed. You can leave a response, or trackback from your own site.

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