Thermal equilibrium of A and B, microstates and quanta

In summary, to find the number of quanta in systems A and B and the temperature at thermal equilibrium, you can use the formulas Q = U/hw and U = Nhwf(T). By equating these formulas and solving for the unknown variables, we can determine that the number of quanta in A and B will be 3x10^23 and 6x10^23 respectively, and the temperature will be 3x10^3 K.
  • #1
karnten07
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Homework Statement



System A consisting of 10^23 oscillators for which hw=10^-20 J, is in thermal contact with system B, consisting of 2x10^23 similar oscillators. The joint system has internal energy 3x10^3 J. Calculate the number of quanta in A and B, and the temperature, when A and B are in thermal equilibrium.

Homework Equations





The Attempt at a Solution



So i have this: W(N,Q) = (N+Q-1)!/[(N-1)!Q!] N is number of oscillators and Q is number of quanta.

For a generic system and W(total) for the system A and B = [tex]\Sigma[/tex]W1(E1)W2(U-E1)

Where W is the number of microstates.

How do i find the number of quanta in A and B?
 
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  • #2


To find the number of quanta in A and B, you can use the formula Q = U/hw, where Q is the number of quanta, U is the internal energy, and hw is the energy of each quantum. From the given information, we know that U = 3x10^3 J and hw = 10^-20 J. Therefore, for system A, we have Q = (3x10^3 J)/(10^-20 J) = 3x10^23 quanta. Similarly, for system B, we have Q = (3x10^3 J)/(10^-20 J) = 6x10^23 quanta.

To find the temperature, we can use the formula U = Nhwf(T), where U is the internal energy, N is the number of oscillators, hw is the energy of each quantum, and f(T) is the average number of quanta per oscillator at temperature T. Since the systems are in thermal equilibrium, the temperature for both systems will be the same. Therefore, we can equate the two equations for U and solve for T.

U(A) = N(A)hwf(T) = (10^23)(10^-20 J)(f(T))

U(B) = N(B)hwf(T) = (2x10^23)(10^-20 J)(f(T))

Equating the two equations, we get:

(10^23)(10^-20 J)(f(T)) = (2x10^23)(10^-20 J)(f(T))

Solving for f(T), we get f(T) = 1/2. This means that at thermal equilibrium, each oscillator will have an average of 1/2 quantum. Substituting this value for f(T) in the equation for U, we get:

U = (10^23)(10^-20 J)(1/2) = 3x10^3 J

Solving for T, we get T = U/(Nhw) = (3x10^3 J)/[(10^23)(10^-20 J)] = 3x10^3 K.

Therefore, at thermal equilibrium, the number of quanta in A and B will be 3x10^23 and 6x10^23 respectively, and the temperature will be 3x10^3 K.
 

FAQ: Thermal equilibrium of A and B, microstates and quanta

1. What is thermal equilibrium?

Thermal equilibrium refers to the state in which two or more objects or systems have reached the same temperature and there is no net heat transfer between them.

2. How is thermal equilibrium achieved?

Thermal equilibrium is achieved when the rate of heat transfer between two objects or systems is equal and there is no temperature gradient between them. This can occur naturally through conduction, convection, or radiation.

3. What are microstates in relation to thermal equilibrium?

Microstates refer to the specific arrangement of particles within a system. In the context of thermal equilibrium, microstates play a role in determining the probability of a certain state occurring and the overall entropy of the system.

4. What is the concept of quanta in thermal equilibrium?

Quanta, or discrete packets of energy, play a crucial role in understanding thermal equilibrium. In a system in thermal equilibrium, energy can only be exchanged in discrete quanta, leading to the concept of quantized energy levels.

5. How do A and B reach thermal equilibrium?

A and B can reach thermal equilibrium through the process of energy exchange, where A and B transfer energy to each other until their temperatures are equal. This process is governed by the laws of thermodynamics and is essential for maintaining balance in many natural systems.

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