Solving Zwiebach 6.1: Stretched String & Nonrelativistic Limit

  • Thread starter ehrenfest
  • Start date
In summary: It is a little confusing. It's not clear if he wants \vec v_\perp to be a d-dimensional vector (as seems to be the case when he writes above |\vec v_\perp|<<|c|, since here its the entire perpendicular velocity vector that's relevant), or a d-1 dimensional projection of this vector, as would be necessary for the equation you're asked to show.
  • #1
ehrenfest
2,020
1

Homework Statement


http://books.google.com/books?id=Xm...42EpgKaxsi5Dw&sig=6cUrZKqmPMoe0QBRTSYNnipNRw4
In problem 6.1, I am trying to show "why the following relations hold"

for the first one, that would just be the definition of ds^2 if you had (cdt)^2 in there but I cannot figure out what happened to it

for the the second one, I am confused about how that can possible be write because the expression for v_perp on 110 implies that it is a vector with the same number of components as X^mu but the y has two fewer components than X. What gives?


Homework Equations





The Attempt at a Solution

 
Physics news on Phys.org
  • #2
Is this even the same ds that is used in the equation ds^2 = cdt^2 +dx^2 + dy^2 + ...?

Or is this just an infinitesimal length of the string? Are we holding time constant in this problem?
 
Last edited:
  • #3
This is a non-relativistic problem, so by ds they probably mean the ordinary distance measure in Euclidean space. For the second part, it seems they are breaking up all the (n dimensional) vectors into the form [itex](x_1, \vec x_T)[/itex] (where [itex]\vec x_T[/itex] is n-1 dimensional). So by [itex]\vec v_\perp[/itex], they probably mean the last n-1 components of the n dimensional perpendicular velocity (the first component being zero to first approximation).
 
  • #4
StatusX said:
This is a non-relativistic problem, so by ds they probably mean the ordinary distance measure in Euclidean space.

If this is so, then isn't the first part true by definition?

StatusX said:
For the second part, it seems they are breaking up all the (n dimensional) vectors into the form [itex](x_1, \vec x_T)[/itex] (where [itex]\vec x_T[/itex] is n-1 dimensional). So by [itex]\vec v_\perp[/itex], they probably mean the last n-1 components of the n dimensional perpendicular velocity (the first component being zero to first approximation).
Yes. Maybe this is just a really minor issue but y is a d-1 dimensional vector (where d is the number of spatial dimensions) and v_T is a dimensional vector and Zwiebach sets the two equal.
 
  • #5
Does my question make sense to people?
 
  • #6
Sorry, didn't see your reply.

ehrenfest said:
If this is so, then isn't the first part true by definition?

Pretty much. I think the reason they're asking you about it is because you'll need the arclength in constructing the lagrangian.

Yes. Maybe this is just a really minor issue but y is a d-1 dimensional vector (where d is the number of spatial dimensions) and v_T is a dimensional vector and Zwiebach sets the two equal.

It is a little confusing. It's not clear if he wants [itex]\vec v_\perp[/itex] to be a d-dimensional vector (as seems to be the case when he writes above [itex]|\vec v_\perp|<<|c|[/itex], since here its the entire perpendicular velocity vector that's relevant), or a d-1 dimensional projection of this vector, as would be necessary for the equation you're asked to show. He probably means to ask you to show that it is only these d-1 coordinates that are non-zero, but there's not an easy way to express this with his notation.
 
Last edited:
  • #7
A related thing that is confusing me is Figure 6.9. X-vector is defined on page 106 as containing only the spatial string coordinates, but in this figure its time-partial clearly has a time-component.
 
Last edited:
  • #8
Does this make sense to anyone else?
 

Related to Solving Zwiebach 6.1: Stretched String & Nonrelativistic Limit

1. What is Zwiebach 6.1 and why is it important to solve?

Zwiebach 6.1 is a problem from the textbook "A First Course in String Theory" that involves analyzing the behavior of a stretched string in the nonrelativistic limit. It is important to solve because it is a fundamental concept in string theory and understanding it can lead to a deeper understanding of the theory as a whole.

2. What is the nonrelativistic limit and how does it relate to Zwiebach 6.1?

The nonrelativistic limit is when the speed of an object is much smaller than the speed of light. In Zwiebach 6.1, this limit is applied to the behavior of a stretched string, which allows for simpler calculations and a clearer understanding of the underlying principles.

3. How can the stretched string be modeled and solved in the nonrelativistic limit?

The stretched string can be modeled using the wave equation, which describes the propagation of waves through a medium. In the nonrelativistic limit, the wave equation can be simplified to the classical string equation, which can then be solved using techniques from classical mechanics and calculus.

4. Are there any real-world applications of solving Zwiebach 6.1?

Yes, the principles and techniques used to solve Zwiebach 6.1 can be applied to various systems involving strings and waves, such as musical instruments, bridges, and even gravitational waves. It also has implications for understanding the behavior of fundamental particles in string theory.

5. What are some common challenges when solving Zwiebach 6.1?

Some common challenges when solving Zwiebach 6.1 include understanding the underlying concepts of string theory, applying the nonrelativistic limit correctly, and using the appropriate mathematical techniques to solve the problem. It may also require a strong understanding of classical mechanics and calculus.

Similar threads

  • Advanced Physics Homework Help
Replies
2
Views
2K
  • Advanced Physics Homework Help
Replies
5
Views
3K
Replies
1
Views
2K
  • Advanced Physics Homework Help
Replies
1
Views
2K
  • Advanced Physics Homework Help
Replies
1
Views
2K
  • Advanced Physics Homework Help
Replies
3
Views
2K
  • Advanced Physics Homework Help
Replies
2
Views
2K
  • Advanced Physics Homework Help
Replies
9
Views
2K
  • Advanced Physics Homework Help
Replies
1
Views
1K
  • Advanced Physics Homework Help
Replies
4
Views
2K
Back
Top