How to understand the zeroth law through these specific equations?

In summary, the zeroth law of thermodynamics establishes thermal equilibrium among systems, allowing the definition of temperature. Understanding this law through specific equations involves analyzing the relationships and interactions between systems in equilibrium, demonstrating how temperature serves as a measurable property that correlates to energy transfer. Key equations illustrate these concepts by quantifying heat exchange and establishing criteria for equilibrium, ultimately reinforcing the foundational principles of thermodynamics.
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Homework Statement
I've studied the zeroth law in other books and am just reviewing it in a new book.
Relevant Equations
This new book shows some math to explain the zeroth law.
I've seen this math also in a lecture once. It seems very vague to me.

Here is the relevant part of the book

1726349972748.png


##F_1## and ##F_2## are introduced as seen above. There is, as far as I can tell, no previous mention of them.

Why does ##F_1(P_A,V_A,P_B,V_B)=0## signify thermal equilibrium?

##P_A## and ##V_A## determine ##T_A## and the same for the ##B## thermodynamic variables.

Thus, it seems that this equation indicates that given, say, ##P_A## and ##V_A##, ie ##T_A##, then there are specific pairs of ##P_B## and ##V_B## that make the equation true.

The book where this equation appears does not define thermal equilibrium.

In Zemansky and Dittman we have the following definition

Thermal Equilibrium: state achieved by two (or more) systems, characterized by restricted values of the coordinates of the systems, after they have been in communication with each other through a diathermic wall.

This means that systems ##A## and ##B## can exchange energy (I think this means just heat).

Again in Zemansky and Dittman
Experiment shows that there exists a whole set of states of a system A, any one of which is in thermal equilibrium with some specific state of system B, and all of which are in equilibrium with each other.

All such states lie on a curve in $xy$-plane called an **isotherm:** locus of all points representing states in which a system is in thermal equilibrium with one state of another system.

The specific state of system B is also on an isotherm, and the isotherm of system A and the isotherm of system B in question are called corresponding isotherms.

Suppose we keep ##V_B## constant and vary ##P_B## and ##T_B##. Then we are moving among different isotherms.

In the equation for ##F_1## in the screenshot above, it seems that this type of change in ##B## should not be allowed.

But I cannot see what it is that prevents it from being allowed with just that equation.

Next, the book isolates ##P_B## in the two initial equations and reaches

$$f_1(P_A,V_A,V_B)=f_2(P_C,V_C,V_B)$$

and says this means ##A## and ##C## are in equilibrium. Why?
 
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The wikipedia article on the Zeroth Law seems pretty good and might give you clues on how to understand the text above:

https://en.wikipedia.org/wiki/Zeroth_law_of_thermodynamics

They have a section on ideal gases and the PV/n=RT formula where P is the pressure, V is the volume, and n is the number of moles. R represents a constant, and T represents the temperature.

So, using a thermometer to measure the temperature of one system A, getting a reading of 100 Celsius when system A and the thermometer reach thermal equilibrium, and then measuring a second system B with the same thermometer and getting 100 Celsius, one can conclude that system A and system B are in thermal equilibrium by the Zeroth Law.

The thermometer is the means to determine the thermal equilibrium.
 
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  • #3
From the book „A History of Thermodynamics – The Doctrine of Energy and Entropy“ by Ingo Müller (Springer-Verlag Berlin Heidelberg 2007); in chapter 1 “Temperature” one reads:

For the early researchers there was no need to define temperature. They knew, or thought they knew, what temperature was when they stuck their thermometer into well-water, or into the armpit of a healthy man. They were unaware of the implicit assumption, – or considered it unimportant, or self-evident – that the temperature of the thermometric substance, gas or mercury, or alcohol, was equal to the temperature of the measured object.

This in fact is the defining property of temperature: That the temperature field is continuous at the surface of the thermometer; hence temperature is measurable. Axiomatists call this the zeroth law of thermodynamics because, by the time when they recognized the need for a definition of temperature, the first and second laws were already firmly labelled.
 
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I understand the zeroth law, I just don't understand how these specific mathematical equations are expressing it.
 

FAQ: How to understand the zeroth law through these specific equations?

What is the Zeroth Law of Thermodynamics?

The Zeroth Law of Thermodynamics states that if two systems are in thermal equilibrium with a third system, then they are in thermal equilibrium with each other. This principle establishes a foundation for the concept of temperature and allows us to use thermometers to measure temperature consistently.

How do the equations relate to thermal equilibrium?

The equations associated with the Zeroth Law typically express the condition of thermal equilibrium mathematically. For example, if system A is in equilibrium with system C, and system B is also in equilibrium with system C, then we can express this as T(A) = T(C) and T(B) = T(C), leading to T(A) = T(B). This shows that systems A and B must also be in thermal equilibrium.

What role do temperature scales play in understanding the Zeroth Law?

Temperature scales, such as Celsius, Fahrenheit, and Kelvin, are essential for quantifying thermal equilibrium. The Zeroth Law implies that temperature is a measurable property that can be used to compare the thermal states of different systems. The equivalence of temperatures across different scales is crucial for establishing a common understanding of thermal equilibrium.

Can you provide an example of the Zeroth Law in action?

An everyday example of the Zeroth Law is using a thermometer. If you place a thermometer (system C) in a cup of coffee (system A) and allow it to reach thermal equilibrium, the thermometer will indicate the coffee's temperature. If you then place the thermometer in a glass of water (system B) and it reaches equilibrium again, you can conclude that the coffee and water are at the same temperature if they both read the same value on the thermometer.

How does the Zeroth Law connect to the first and second laws of thermodynamics?

The Zeroth Law lays the groundwork for the first and second laws of thermodynamics by defining temperature and thermal equilibrium. The first law, which deals with the conservation of energy, relies on the concept of temperature to describe energy transfer as heat. The second law introduces the concept of entropy and the direction of spontaneous processes, which also depend on temperature differences. Together, these laws create a comprehensive framework for understanding thermodynamic systems.

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