Cusps in the evolution of closed strings

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Homework Help Overview

This discussion revolves around a problem from Zwiebach's book concerning the behavior of closed strings near cusps. The original poster is tasked with demonstrating a relationship between the variables y and x as well as analyzing the period of motion of the closed string.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive the relationship ##y\sim x^{2/3}## and questions the reasoning behind it. Some participants suggest re-evaluating the expressions for y and x without factoring out powers of ##\sigma-\sigma_0##. Others propose solving for ##(\sigma-\sigma_0)## in terms of x and substituting it back into the equation for y.

Discussion Status

The discussion is ongoing, with participants providing feedback on the original poster's attempts. There is a recognition of the need to clarify the expressions involved and explore the implications of periodic functions in part (d). No consensus has been reached yet.

Contextual Notes

Participants are working under the constraints of the problem as stated in the homework, which includes specific equations and relationships that must be adhered to. There is an acknowledgment of potential missing information regarding the derivation of the period of the closed string's motion.

rbwang1225
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Homework Statement


This is problem 7.7 in Zwiebach's book, 2ed ed.
In (b) he want us to show that near the cusp, ##y\sim x^{2/3}.##
In (d), Check that the period of the motion of the closed string is ##\sigma_1/4c##. How many cusps are formed during a period?

Homework Equations


(b) ##\overrightarrow X(t_0,\sigma) = \overrightarrow X_0+\frac{1}{2}(\sigma-\sigma_0)^2\overrightarrow T+\frac{1}{3!}(\sigma-\sigma_0)^3\overrightarrow R
\\=\frac{1}{2}(\sigma-\sigma_0)^2 T\hat y+\frac{1}{3!}(\sigma-\sigma_0)^3 R(\cos\theta\hat x+\sin\theta \hat y)##, where ##|\overrightarrow T|=T \mbox{ and } |\overrightarrow R|=R##.
(d)##\overrightarrow X(t,\sigma)
=\frac{1}{2}[\overrightarrow F(u)+\overrightarrow G(v)]
=\frac{\sigma_1}{4\pi}(\sin \frac{2\pi u}{\sigma_1}+\frac{1}{2}\sin\frac{4\pi v}{\sigma_1},-\cos\frac{2\pi u}{\sigma_1},-\frac{1}{2}\cos\frac{4\pi u}{\sigma_1})
=\overrightarrow X(t+T,\sigma)##

The Attempt at a Solution


(b) ##y=\frac{1}{2}(\sigma-\sigma_0)^2[T+\frac{1}{3}(\sigma-\sigma_0)R\sin\theta]##
##x=\frac{1}{3!}(\sigma-\sigma_0)^3R\cos\theta##
But, I don't see very clearly why ##y\sim x^{2/3}##.
(d) I observe that ##\overrightarrow F(u) \mbox{ and } \overrightarrow G(v)## has periods ##\sigma_1/c \mbox{ and }\sigma_1/2c##, respectively. But I don't know why the period of ##\overrightarrow X## is smaller.

Any advice would be very appreciated.
 
Last edited:
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rbwang1225 said:
##y=\frac{1}{2}(\sigma-\sigma_0)[T+\frac{1}{3}(\sigma-\sigma_0)^2R\sin\theta]##
##x=\frac{1}{3!}R\cos\theta##
But, I don't see very clearly why ##y\sim x^{2/3}##.

These aren't quite correct. Try finding them again. Don't factor out any powers of ##\sigma-\sigma_0##.
 
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George Jones said:
These aren't quite correct. Try finding them again. Don't factor out any powers of ##\sigma-\sigma_0##.
I corrected it.
Or, I still have something lost?
Thanks a lot!
 
It looks like you're still missing something in the expression for y.
 
Oh, sorry for the mistake!
Now, can I conclude that since ##y\sim (\sigma-\sigma_0)^2 \mbox{ and } x\sim (\sigma-\sigma_0)^3## so ##y\sim x^{2/3}##?
I think it's yes, because the factors, T, and x-component of R are just numbers, they don't affect the main feature of the line.
Thank you very much!
 
Roughly, yes.

Maybe better is to solve the ##x## equation for ##(\sigma-\sigma_0)##, and substitute this into the ##y## equation, so as to obtain ##y## as a function of ##x##. The expression for ##y## should contain two terms that involve ##x##. Argue that, near a cusp, one of these terms dominates.
 
OK, then I know how to get the answer.
But now I have a question in (d). I don't know how to derive the period of the function of the sum of 2 periodic functions. I thought it was the smaller one between the two, but it seems like something was missing.
 

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