Statistical mechanics problem of spin

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Homework Help Overview

The problem involves a statistical mechanics scenario with two subsystems, A and A', containing spins with specified magnetic moments. The original poster is tasked with calculating the probability of various total magnetic moment values after the systems are placed in thermal contact.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to determine the probabilities of different total magnetic moment configurations based on initial conditions and configurations of spins. Participants question the correctness of the configurations counted and their contributions to the total magnetic moment.

Discussion Status

Participants are actively discussing the implications of the original configuration on the possible outcomes. Some guidance has been offered regarding the conservation of energy and the correct interpretation of the total magnetic moment in the configurations considered.

Contextual Notes

There appears to be confusion regarding the initial total magnetic moment and how it affects the counting of configurations. The original poster's calculations do not align with expected results, prompting further exploration of assumptions and definitions.

athrun200
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Homework Statement


Consider a system consists of two subsystem A and A' in which A contains 3 spins and A' contains 2 spins. Suppose that, when the systems A and A' are initially separated from each other, measurements show the total magnetic moment of A to be - 3{\mu _0} and the total magnetic moment of A' to be + 4{\mu _0}. The systems are now placed in thermal contact with each other and are allowed to exchange energy until the final equilibrium situation has been reached. Under these conditions calculate:
(a) The probability P(M) that the total magnetic moment of A assumes anyone of its possible values M.

Homework Equations


Basic statistic and probability tools.

The Attempt at a Solution


The question implies that each of the spin in A has magnetic moment {\mu _0} while A' has 2{\mu _0}.
Originally, the system has the spin arrangement like this:
--- ++
where - means spin down and vice versa.

After they are in contact, they can have the following possibility.
--- ++ - 3{\mu _0}
--+ -+ - {\mu _0}
-+- -+ - {\mu _0}
+-- -+ - {\mu _0}
+-- +- - {\mu _0}
+-+ -- {\mu _0}
++- -- {\mu _0}
--+ +- - {\mu _0}
-++ -- {\mu _0}
-+- +- - {\mu _0}

So P( - 3{\mu _0}) = \frac{1}{{10}}, P( - {\mu _0}) = \frac{6}{{10}}, P({\mu _0}) = \frac{3}{{10}}.

But the answer is P({\mu _0}) = \frac{6}{7}, P( - 3{\mu _0}) = \frac{1}{7}.

What's wrong?
 
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Hi athrun200!

--+ -+ would have total moment -\mu_0, not +\mu_0, as is required by conservation of energy.
 
I know --+ -+ produces total moment - {\mu _0}
But how does it affect the answer?
 
The original configuration --- ++ had total moment +\mu_0, yes?

So all the possible configurations that you're counting should have total moment +\mu_0, not -\mu_0.
 
Oxvillian said:
The original configuration --- ++ had total moment +\mu_0, yes?

So all the possible configurations that you're counting should have total moment +\mu_0, not -\mu_0.

Oh! Now I get it, thanks a lot!
 
np :smile:
 

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