Infinitely long molecular zipper

  • Thread starter Thread starter subzero0137
  • Start date Start date
  • Tags Tags
    Molecular
Click For Summary

Homework Help Overview

The problem involves a "molecular zipper" consisting of two rows of molecules, where each row contains a large number of monomers linked by bonds that can be broken sequentially. The task is to derive expressions for various thermodynamic properties of the zipper, treating it as infinitely long and considering the energy required to break bonds.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to find the partition function Z, suggesting that the energy levels correspond to multiples of ε. There is uncertainty about whether the series for Z should be finite or infinite, given the context of broken bonds.

Discussion Status

Some participants provide clarification regarding the interpretation of n as corresponding to microstates, indicating that each molecule can have its own value of n. This suggests an exploration of the distribution of n values in the sample, while confirming that the limit of n is indeed infinite.

Contextual Notes

There is a hint provided in the original problem regarding the summation of a geometric series, which may influence the approach to finding the partition function. The discussion reflects a focus on the assumptions regarding the nature of the bonds and the states of the zipper.

subzero0137
Messages
91
Reaction score
4

Homework Statement


[/B]
A "molecular zipper" has two rows of molecules, and each row has a large number of monomers. A monomer from one row is weakly linked to a monomer in the other row. The zipper can unzip from one end by breaking the bond between pairs of monomers. A bond can be broken only if the bond to its left is already broken. It requires energy ε to break each bond, i.e. for every broken bond, the zipper absorbs energy ε. Thus, for every extra bond that is broken, the zipper can be regarded as moving up on the energy ladder by ε.

Treating the zipper as infinitely long, find expressions for the energy, the Helmholtz free energy, heat capacity and entropy of such a zipper at temperature T. [Hint: A zipper can have n broken bonds at T. Each value of n corresponds to one microstate. You need to find the partition function Z at temperature T. You may assume $$a + ar + ar^2 + ... = a \sum_{0}^\infty r^n = \frac {a}{1 - r}$$

Homework Equations


[/B]
$$Z = \sum e^{- \frac {ε_{i}}{kT}}$$

The Attempt at a Solution



I'm trying to find the partition function Z. I think ##ε_i = iε## here, so

$$Z = e^{ \frac {-0ε}{kT}} + e^{ \frac {-1ε}{kT}} + e^{ \frac {-2ε}{kT}}... = \frac {1}{1 - e^{ \frac {-ε}{kT}}}$$

but I'm not sure if it's right because if it can only have n broken bonds at T, should it not be a finite series?
 
Physics news on Phys.org
Read the question again. "Each value of n corresponds to one microstate". Each molecule has its own value of n, and there is a distribution of n values in the sample. (n corresponds to the index i in your equation for Z. It is not the limit of i. The limit of i (or n) is infinity.)
 
mjc123 said:
Read the question again. "Each value of n corresponds to one microstate". Each molecule has its own value of n, and there is a distribution of n values in the sample. (n corresponds to the index i in your equation for Z. It is not the limit of i. The limit of i (or n) is infinity.)

Thanks for the reply. So I'm on the right track with my partition function?
 
Looks like it.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
5
Views
2K
  • · Replies 20 ·
Replies
20
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K