Length of Line between 2 Points on Circle

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The discussion centers on the concept of a chord, which is the shortest distance between two points on a circle's perimeter. Participants explore the relationship between the length of a chord and the arc length it subtends, particularly in the context of calculus and physics. A key point raised is the approximation that the length of the chord approaches the length of the arc as the angle subtended approaches zero, supported by the limit identity involving sine. The conversation also touches on the differentiation of chord length concerning arc length, emphasizing that the relationship holds true primarily for small angles. Overall, the dialogue clarifies the mathematical principles linking chords and arcs in circular motion.
quasar987
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Hi,

I'd like to know the name for the length in a circle that I will describe:

Consider 2 arbitrary points lying on the perimeter of a circle. I'm talking about the shortest distance distance between these those points. (i.e. the straight line joining them.)

Thx
 
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It's called a chord.
 
Yep, a chord.
 
Ok, I have a confusion involving a cord. In physics, we often make the transformation from an infinitesimal cord to an infinitesimal arc: d(cord) = d(arc). And I think it's used in some math proofs too.

For exemple, imagine a position vector \vec{r}(t) of fixed norm, rotating around the z axis (i.e. \vec{\omega} = \omega \hat{z}). Let's say the radius of the circle described by the motion of its tip/head/arrow is R. After a time \Delta t, it has rotated an angle \omega \Delta t and then they (the manuals) say that it can be seen that when \Delta t is small, ||\Delta \vec{r}|| (which is a cord), is very near the length of the arc \Delta s subtended by the angle \omega \Delta t, and thus, poof, ||d\vec{r}|| = ds.

And while this seems to be true intuitively, I have never seen a proof of this statement. And when I try to do it, here's what I get:

I start from a cercle of radius R and a cord \delta subtended by an angle \theta. I find that the length of the cord is given by

\delta = 2Rsin\left(\frac{\theta}{2}\right)

Therefor,

d\delta=Rcos\left(\frac{\theta}{2}\right)d\theta

While

ds=rd\theta

So

d\delta=cos\left(\frac{\theta}{2}\right)ds

A result indicating that even the differential version is just an approximation because only true for a principal angle \theta=0.
 
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it follows from the identity

\lim_{\theta \rightarrow 0} \frac{\sin \theta}{\theta} = 1

Also, the mistake in your derivation is that theta is a function of the chord length.
 
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Thanks for your reply StatusX

StatusX said:
it follows from the identity

\lim_{\theta \rightarrow 0} \frac{\sin \theta}{\theta} = 1
At which point does that identity fit in?


StatusX said:
Also, the mistake in your derivation is that theta is a function of the chord length.

Could you elaborate?
 
Sure,if "y" is a function of "x",then "x" is a function of "y",right??So he basically didin't say anything new...You were right,though...Your calculations were corrrect.I guess u knew that,but u have my confirmation...

Daniel. :smile:
 
quasar987 said:
At which point does that identity fit in?

A chord of length 2 R sin(theta) is subtended by an angle of 2 theta (in radians) and so has an arclength of 2 R theta. The identity means d(chordlength)/d(arclength) = 1.

Could you elaborate?

I'm sorry, I just glanced at your last step and assumed you had forgotten that if arclength is 0, then theta must be as well. You did forget that, but for a different reason. What you derived is how an chord of finite length changes with an infinitessimal change in arclength. What you wanted was the ratio of a differential chord to the differential arclength it subtends. To get the differential you're looking for, just take theta=0.
 
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