A Suggestion to Make Thermodynamic Theory More Easily Understandable

The conceptual difficulties encountered in thermodynamics are well known and are certainly the reasons that have led the great physicist Arnold Sommerfeld, a long time ago, to say that understanding thermodynamics is not easy. The situation remains nearly the same today and is due to the fact that the tools used in thermodynamics, i.e. the equations, are not in good accordance with the laws of thermodynamics. Since the efficiency of the tools cannot be contested, it is probably the formulation of the laws that needs to be revised. On the basis of arguments already evoked in previous papers, the suggestion presented below is a contribution going in this sense and inserting the Einstein’s relation E = mc in the thermodynamic reasoning.


Introduction
The scientific reputation of Arnold Sommerfeld seems to rest in two main reasons. The first one is that he has been the scientist the most often nominated for the Nobel Prize in Physics (81 times according to Wikipedia) although he never won it. The second is that his judgment on thermodynamics remained famous because of the next shape he gave it: "Thermodynamics is a funny subject. The first time you go through it, you don't understand it at all. The second time you go through it, you think you understand it, except for one or two points. The third time you go through it, you know you don't understand it, but by that time you are so used to the subject, it doesn't bother you anymore". Confronting both reasons, it cannot be excluded that some members of the Nobel Prize Committee have not appreciated the judgment given by Arnold Sommerfeld about thermo-

A Brief Reminder on the First Law of Thermodynamics
Let us imagine that the system we are considering ( Figure 1) is a given mass of gas placed in a glass cylinder, equipped with a mobile frictionless piston. In the initial state, the piston is in equilibrium at height A and the first equation we write takes the form: 1 1 i e P P = (1) whose meaning is: Internal pressure at time 1 = External pressure at time 1.
More precisely, this is a way to say that the pressure exerted on the gas (i.e. the atmospheric pressure augmented by the pressure due to the mass of the piston) is equal to the pressure exerted by the gas on the inderside of the piston.
If a determined mass M of sand is deposited on the piston, this last one goes downward until it reaches a new equilibrium state at height B, where the new equation of equilibrium becomes: Depending on whether the mass of sand is deposited all at once or in successive small batches, the time required by the piston to go down from A to B is not the same.
In the first case, the external pressure P e and the internal pressure P i are constantly different during the moving of the piston and become equal only when the piston stops. This condition is called irreversibilty with regard to the pressure and the work done on the gas by the piston is defined at each moment by  where dV is the volume change of the gas. In the second case, the external pressure P e and the internal pressure P i tend to be constantly equal during the moving of the piston. This condition is called reversibilty with regard to the pressure and the work done on the gas by the piston is defined at each moment by the relation: For a given value of dV, the difference between dW irr and dW rev is therefore: that can also be written: The condition (P i − P e ) > 0 leading to dV > 0 and the condition (P i − P e ) < 0 to dV < 0, we have always ( ) 0 i e dV P P − > , and therefore the relation between dW irr and dW rev is always: Having in mind the representation given above (Figure 1), we easily conceive that when P i and P e are rigorously equal, the piston does not move, so that we get dV = 0. The evidence of this situation is well known and has inspired to Arnold Sommerfeld the following comment: Reversible processes are not, in fact, processes at all, they are sequences of states of equilibrium. The processes which we encounter in real life are always irreversible processes. This is a way to recall that the condition of reversibility is a limited case, whose usefulness is mainly theoretical. From the practical point of view, the information to keep in mind is that when a system passes from a state A to a state B, depending on whether the process is highly irreversible or slightly irreversible (with regard to the pressure), the physical significance of Equation (7) is: irr highly irr slightly dW dW > (8) In conditions of irreversibility, it has been observed for a long time that when the piston moves down (case represented by the left arrow), the temperature of the gas tends to increase temporarily, before returning to its initial value. This is the sign that a part of the work done on the gas is transformed in heat, classically noted dQ. But this heat is finally eliminated towards the surroundings so that its writing takes the negative form: Conversely, if the sand initially deposited is removed, the piston will moves up (case represented by the right arrow) and it has been observed that the temperature of the gas decreases temporarily, before returning to its initial value. This is the sign that a given amount of heat has transited from the surroundings (the atmosphere) to the gas. Being received by the system, this heat is counted posi- In the process just examined, the energy given or removed by the experimentor is exclusively under the form of work (by deposit or evacuation of sand). As a consequence, the appearance or disappearance of heat is a natural reaction entirely due to the system itself. In many other contexts, the experimentor plays directly a role on both work and heat (or only on heat as will be the case in section 3 and 4).
The numerous studies done on this subject have led to the first law of thermodynamics. With reference to the simple experimental context considered here, it consists in admitting as a general postulate that the concept of internal energy variation called dU and defined by the relation: is independent of the level of irreversibility of the process by which the system passes from an initial state A to a final state B. (The fact that, in Equation (11), dQ is placed before dW and not after is just due to the respect of a thermodynamic writing convention).
In other words, this is a way to say that the term dU always obeys the relation: Having got for dW the general proposal dW irr > dW rev given by Equation (7), the logic of the thermodynamic reasoning would be that the proposal obtained for dQ should take the form: The next section is devoted to this question.

A Brief Reminder of the Second Law of Thermodynamics
In the same manner as Equations (3) and (4) show the link existing between the terms dW, P and dV, a thermodynamic link has been established between dQ, T and the term dS, called the change in entropy.
This last concept being less familiar than that of change in volume (dV) it is important to begin the discussion with a reminder of the definition given to dS in thermodynamics.
In condition of reversibility (i.e. when we have constantly T i = T e ), the term dS is linked to dQ and T (the absolute temperature) by the relation: In conditions of irreversibility (i.e. when we have T i ≠ T e ), the term dS is linked to dQ and T (the absolute temperature) by the relation: This last relation is often written: In contrast, the term dQ/T is called the external component of entropy and noted dS e , so that Equation (16) takes the significance: This equation illustrates the fact that, in conditions of irreversibility, a part of the entropy, noted dS e , is due to the exchange of heat between the system and its surroundings, while another part, noted dS i , is created inside the system. Having in mind that the result dQ irr < dQ rev given by Equation (13) was presented as the logical consequence of the first law of thermodynamics, we may be tempted to think that the term dQ of Equation (14) represents dQ rev , while the term dQ of relation 15 and Equation (16) represents dQ irr . In such conditions, the coherency of the theory would seem reached.
The problem is that this impression is not the adequate one and there are two reasons to this situation: The first is that the precise meaning of Equation (14) is: The second is that the precise meaning of relation (15) is: Consequently, the precise meaning of Equation (16) Combining Equations (18) and (20), we can see that for a given value of dS, the corresponding value of dS i is given by equation: The positive value of dS i (evoked in the comment following Equation (16)) is classically confirmed by Equation (21) through the fact its right end term is always positive.
Indeed, when we have T i < T e , the term in parentheses is positive and dQ rev too.
When we have T i > T e , the term in parentheses is negative and dQ rev too.
Therefore the general result that needs to be retained takes the form: It constitutes a simple expression of the second law of thermodynamics as well as Equation (11)

The Divergence between Theory and Practice in Thermodynamics
At this point of the discussion, the attention is called on the fact that: • we are reasoning on systems as simple as possible • we have in mind the judgment beared by Arnold Sommerfeld on thermodynamics • we are trying to test the coherency of the theory, which means that, according to the usual understanding of the first law, we want to see if the proposal dQ irr < dQ rev suggested by Equation (13), is confirmed.
Observing that we can deduce from Equation (18) the relation: our remaining objective is the search of the corresponding relation concerning dQ irr .
In the list of 23 equations already written, the term dQ irr is present nowhere, excepted in Equation (13) which is not an answer, but just a question.
Confronted to this situation, it seems that the only possible solution to get dQ irr consists in multiplying both sides of relation 20, which is an entropy equation, by T e , and we obtain the energy equation: whose thermodynamic meaning is: Knowing from Equation (21) that we have dS i > 0 and having also T e > 0 since T e is an absolute temperature, the obtained conclusion takes the form: Obviously, this result is not compliant with the one usually predicted by the first law of thermodynamics and therefore requires an explanation. Before discussing this interesting question in section 5, let us examine a very simple example of calculus leading to a confirmation of Equation (26).
The system we are considering is 1 liter of water (=1000 g) placed in a transparent graduate cylinder. In the initial state A, the temperature of the water is 25˚C (=298 K) and by heating the water passes to a final state B where its temperature is 80˚C (=353 K). Our objective is the determination of the various terms evoked above: ΔQ irr , ΔQ rev , ΔS, ΔS e and ΔS i .
A first important remark is that inside the transparent cylinder, the water level did not change by heating. This seems the sign that the water volume does not change either so that we don't have to consider the existence of a term ΔW.
As a consequence we can deduce from Equation (11) that the change in internal energy of the water is limited to the expression: Then, remembering that the first law postulates the equality: As will be seen below, the terms ΔQ irr and ΔQ rev are not equal and therefore are not in accordance with the usual interpretation of the first law.
For the calculation of ΔQ rev the equation classically used is: If, in a second experiment, the cylinder containing the water at 298 K is itself immersed in a larger water tank whose temperature is 353 K, this temperature becomes the term T e (the external temperature) evoked in Equation (24). This is a way to say that, according to the relation linking together Equations (24) and (25) (ΔQ irr = T e ΔS), the value of the term ΔQ irr is: This last result corresponds effectively to the condition dQ irr > dQ rev and not to the condition dQ irr = dQ rev evoked by Equation (29) and presented as the logical prediction of the first law.
In this conception, the difference between ΔQ irr and ΔQ rev appears as an additional energy that can be called ΔQ add and whose definition is: Its numerical value, in the present case, is: The other expected results are as follows:

Discussion
The main difference between the conventional interpretation of the first law of and the new suggested one can be summarized as follows: In the conventional interpretation, the entropy Equation (20) whose expression is: is not converted into the energy Equation (24) whose expression is: Comparing both definitions, the conclusion dQ irr > dQ rev can be deduced by the same kind of simple reasoning as the conclusion dW irr > dW rev obtained above from Equation (7).
Transposed in the context of change in internal energy, the term dQ add of Equation (38) becomes a contribution to the term dU add of the energy equation: explaining that the formulation of the first law would imply the inequality: instead of the equality dU irr = dU rev usually admitted.
Concerning this question, the attention is called on the two following points. • An irreversibility of pressure generates a heat that is really detected before being ejected from the system (context examined above in section 2); • An irreversibility of temperature generates an energy which seems implicitly evident but is not really detected (context examined above in section 3 and 4).
It is certainly for this second reason that, when the thermodynamic theory was The situation is different today because in the meantime, the mass-energy relation E = mc 2 has been discovered by Einstein, whose differential form is: explaining that a mass can be transformed in energy and conversely. The term c 2 being enormous, we easily conceive that when an energy is transformed in mass, the change in mass is generally too small to be physically detectable. In present physico-chemical textbooks, when a change in mass linked to Equation (42) is described as detectable, it takes place in the context of a radioactive reaction, not in the context of a ordinary chemical reaction and even less in the context of a simple heating of water as the one examined above. In relation with this situation, it can be imagined that the additional energy ΔQ add evoked in section 4, whose reality has not been physically detected, but whose numerical value has A correlative important question is the choice of the sign + or -in Equation (42). The first idea that would come in mind is that the additional energy ΔQ add being transformed in mass, the mass of the water would increase. The second is that the additional energy ΔQ add could take the form of a potential gravitational energy created by a decrease in mass of the water.

Conclusions
After a mention concerning Arnold Sommerfeld [1], the section References that will follow these conclusions is divided in two parts. The first one (Ref.
[2] to [5]) is devoted to a series of thermodynamics textbooks, generally written for geologists (since geology was my specialty that is a combination of the first and second laws and becomes the chosen hypothesis to go farther in the study of the problem.
An interesting detail is that applying the concept of Gibbs's free energy, noted G, to the process of heating water evoked above in section 4, we get dG dH TdS = − whose precise meaning is rev irr dG dQ dQ = − . The obtained result is dG < 0, which takes a particular interest, because dQ being here the only component of dU, the result dG < 0 means dU rev < dU irr .
The fact that such arguments are simple is a possible handicap for their acceptation since in contrast to its remarkable ability to understand and solve complicated problems, the scientific community sometimes tends to be wary of hypothesis that seems simple. Geology has known an example of this situation with the concept of continental drift suggested by Alfred Wegener. Considered today as evident, this idea has long been rejected, because the hypothesis that continents can move was perceived as unimaginable.
In the field of physics, Arnold Sommerfeld's description of thermodynamics would have been seen as an innocuous joke if he had only been an amateur, but since he was a great physicist, there is no doubt that it deserves to be seen as a