Statistical Mechanics and Thermodynamics

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SUMMARY

The discussion focuses on deriving the force exerted by a particle confined in a cubic box as the box's length in the x-direction, Lx, changes. The energy of the particle is expressed as E = (h²(nx² + ny² + nz²))/(8mLx²). The force exerted on the wall perpendicular to the x-axis is given by Fx = -∂E/∂Lx, demonstrating the relationship between energy change and force in a thermodynamic context. The discussion emphasizes the connection between work done by the system and the energy shift due to changes in box dimensions.

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vladittude0583
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Homework Statement



Consider a particle confined within a box in the shape of a cube of edges Lx=Ly=Lz.

(a) Suppose that the partice is in a given state specified by particular values of the principal quantum numbers nx, ny, nz. By considering how the energy of this state must change when the length Lx of the box is changed quasistatically by a small amount dLx, show that the force exerted by the particle in this state on a wall perpendicular to the x-axis is given by Fx=-partial derivative of E with respect to partial derivative of Lx

Homework Equations



Xa,r=-partial derivative of Er wit respect to partial derivative of xa

where Xa,r is the generalized force (conjugate to the external parameter xa) in the state r

The Attempt at a Solution



I derived an expression for the quantized energy which is (h2(nx2+ny2+nz2)/(8mLx2)

Do I have to use pressure to some extent? Any advice would be greatly appreciated
 
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The absolute value of the energy shift which takes place when the length of the box changes is equal to the absolute value of the work done by the system. This work is

<br /> dA = F_x dL_x<br />

vladittude0583 said:
Fx=-partial derivative of E with respect to partial derivative of Lx

It's easier to read the following:

<br /> F_x = - \frac{\partial E}{\partial L_x}.<br />

See
https://www.physicsforums.com/showthread.php?t=8997&highlight=LaTeX+TeX"
 
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