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Physics and Economics. Gnoseological difference and its manifestation in IT

I came to the world of IT from theoretical physics. He was mainly engaged in economic tasks. Engaged - this: analysis, TK, statement, design, programming. Naturally, all the time I compared the physical and economic approaches to understanding the laws of nature and economics, respectively. A certain point of view has ripened on this subject. About her and will be discussed.


1. About cognition in general


There are two approaches to cognition:


Aristotle's approach . This is a holistic approach and treats the object as a black box. The phenomenon, the object is studied in all reality as a whole. And reality says, for example, that heavy bodies fall to the ground faster than light ones; that left to itself a moving body gradually stops. Aristotle's approach deals with the phenomenon as an integral reality, and therefore can be called phenomenological.


Galileo's approach . This is an analytical, systems approach. This is the divide and conquer approach. The phenomenon, the object are decomposed into its constituent parts and each of them is studied separately, abstracting from the rest (analysis). Then, the resulting pictures can be combined into one, taking into account the interaction of the components (synthesis). For example, the fall of bodies is considered as the fall of bodies in the void. And there they turn out to fall with the same acceleration. But in reality, friction against air prevents them from falling equally. Having studied this force separately, we can explain the result of Aristotle. Similarly, if we disengage from the forces of friction, then the moving body will move without stopping. And if we take into account the friction force, we get the result of Aristotle. Galileo's approach immediately leads to the need to study forces. This, in the end, translates into a coherent system of classical physics.


Once again, for clarity.


Aristotle's approach . There is a phenomenon under study, “The fall of a body in the air to the ground” - the F. phenomenon. We take different bodies and find that heavier bodies fall to the ground faster than light ones.


Galileo's approach . When studying the phenomenon of F, one must take into account not only weight. We study the fall in the air. And let's change not only weight, but also air. Let's try to reduce its density, so that, in the end, there is no air. Then we find that all bodies fall in the void with the same acceleration. We find the parameters of the effect on the phenomenon and try to create conditions under which only one parameter is significant. This is not in nature. Therefore, a physicist needs a laboratory where he could vary the parameters. Having studied the influence of one parameter, we can proceed to study the influence of another parameter. We are trying to reduce the complexity of the whole approach to the composition of simpler approaches. Varying the shape of the falling body, we can study the dependence of the friction force on air depending on the shape of the body. By varying the rate of fall, we can detect the dependence of the friction force on speed. By varying the height of the fall, we can detect the dependence of acceleration on height. By varying the geographical location on earth, we find the dependence of the acceleration of fall on geography.


Roughly speaking, in the approach of Aristotle they study reality, and in the approach of Galileo they study abstractions, and from them, through synthesis, they go to reality.


2. The model of physical knowledge


Physics is an ideal theory for many sciences, including economics. In physical experiments, discrete series of values ​​are obtained. But they are considered an approximation to continuous functions, which in reality are physical indicators. And physicists are trying to guess these functions. So Galileo guessed the parabola for the trajectory of a stone thrown at an angle to the horizon; Kepler guessed the trajectories of the planets - ellipses, etc. Having guessed the trajectory, we get a predictive apparatus - the ability to calculate the value for unexplored coordinates of the trajectory. To test, they put an experiment - create the conditions for experimental obtaining the value of interest. Then, having verified the predicted value and the experimental one, we get a confirmation or refutation of the theory. Here sometimes the error of the experimental error plays an important role. Physical knowledge comes down to the identification of determinism - the law of obtaining a state from an initial state:


S(t)=D(Q,S(0))


S(0) -   D –  – ,  S(t)  S(0) Q –       . ,  ,      . 

So, for a thrown stone from a point (0,0) with a speed v0at an angle αto the horizon we have


$$ display $$ x (t) = v_0 t cos⁡ (α), y (t) = v_0 t sin⁡ (α) - (gt ^ 2) / 2 $$ display $$


The initial state S (0) is set by three parameters: departure point (0,0), initial speed v0angle α.
The impact of the environment Q is given by the acceleration of gravity g. When expanding the scope of the problem (high initial velocity), g is no longer constant.
The determinism D is given by the above formula.


For a more realistic task, you need to take into account friction against the air. This complicates the math of the problem, but the principle remains the same. Instead of stone, you can consider a plane. Then the thrust force of the aircraft comes into play, and its regulation by the pilot. A non-physical factor also appears - the will of the pilot. We cannot take it into account. But we know that it is not unlimited: traction cannot be infinite, acceleration cannot be infinite. This introduces an element of certainty into the movement. They use it, for example, to build the trajectory of an air defense missile.


Let's go back to the flying stone. It is characterized by an infinite number of physical parameters. For example, only its shape can be arbitrarily complex. But we are sure that in some useful area we can consider the stone as a material point. This is the main abstraction of classical mechanics. All systems are represented as sets of interacting material points. This makes the main cognitive reduction - the reduction of the behavior of a complex system to the behavior of its elementary components.


In connection with the mentioned cognitive reduction, two epistemological approaches can be distinguished - reductionism and holism.


3. Reductionism and holism


Reductionism is the principle of reducing the characteristics of a system from the characteristics of subsystems and the characteristics of the interaction of subsystems. Successfully works in physics.
Consider, for example, gas. Without decomposing it into subsystems, we can operate with experimental, phenomenological concepts: pressure P, temperature T, volume V. Empirically, we find the relation connecting these parameters - the equation of state of the gas:


PV=constT


This is the so-called phenomenological level - work with phenomena (phenomena) without going into their structure. This is Aristotle's approach.


Now apply the approach of Galileo. We decompose the “gas" system: imagine it as a collection of colliding molecules. Then we define P and T through the mechanical parameters of the molecule. This is done in molecular physics. Thus, we reduce the gas system to subsystems of molecules. This will clarify the equation of state or deduce it for new systems.


Accordingly, in business we have an analogy: macroeconomics are decomposed into enterprises and households. But here the reduction is not yet perfect. Alas, there is no economic Newton. The problem is the complexity and availability of a subjective factor that is not in physics (though there is a debate about the role of the subject in quantum mechanics).


And now about holism.


Holism is the principle that there can be non-reducible properties in a system. So in biology, the doctrine of vitalism is based on the concept of entelechy, the life force inherent in the body as a whole and irreducible.


Physics so far dispenses with the concept of holism.


4. Formula and algorithmic models


A formula model is a model defined by a formula. The concept of “formula” will be considered known.


Examples in physics: Newton equations, Lagrange equations, Maxwell equations, Navier-Stokes equations, Heisenberg-Schrödinger equations, Einstein equations.


Examples from the economy: Black-Scholes formula for the option price, money supply formula, linear programming model for optimizing the financial portfolio, interest calculation formulas, risk calculation formulas.


With a formulaic model, a person can work without a computer. Such is almost all pure mathematics. But here, algorithmic plays an increasingly important role. So the solution to the problem of four colors was not reduced to any formula, but required a brute-force solution for many special cases. This bust was done by computers.


Algorithmic model - a model defined by an algorithm, possibly not reducible to a formula. Of course, it is possible to classify the algorithm as formulas, but these are not the same classical formulas. The algorithmic model is initially realistic only using a computer
A formal model can always be reduced to an algorithmic one.


An example of the first algorithmic model is the Fermi-Pasta-Ulam problem. Here is a quote from Ulam’s book, The Adventures of Mathematics.


Quote

As soon as the machines were completed, Fermi, with his intuition and great common sense, immediately realized all their importance in the study of problems of theoretical physics, astrophysics and classical physics. We discussed this issue in the most detailed way and decided to try to formulate some problem that would be simple in its formulation, but would have a solution requiring very long calculations, impossible with the help of a pen and paper or existing mechanical computing devices. Having discussed a number of possible problems, we settled on one typical problem associated with the long-term behavior of a dynamical system and requiring a long-term prediction. It considered an elastic string with two fixed ends, which is affected not only by the usual elastic deformation force proportional to deformation, but also by a small physical nonlinear force. It was necessary to find out how, after a very large number of periods of oscillations, this nonlinearity will gradually affect the known periodic behavior of oscillations in one key, how other key keys will acquire their amplitudes, and how, we reasoned, the movement will be thermalized, imitating, perhaps, the behavior liquids, which, being initially laminar, become more and more turbulent, until, finally, their macroscopic motion is converted into heat.

John Pasta, a physicist who recently arrived in Los Alamos, helped us with creating flowcharts, programming, and processing tasks at MANIAC. Fermi decided to learn how to program a machine. In those days, it was more difficult to do than now, when ready-made programs and established rules already exist, and this procedure itself is automated. Then it was necessary to learn various tricks. Fermi mastered them very quickly, and taught me something, although I already knew enough to be able to evaluate what kind of tasks can be solved in this way, determine their duration in the number of calculation steps and understand the principles of their implementation.


As it turned out, we very successfully selected the task. The results obtained in qualitative terms completely differed even from those that Fermi expected with his deepest knowledge of wave motions. The original goal was to see at what speed the string energy, originally embedded in a simple sinusoidal wave (a note was taken as one tone), would gradually create higher harmonics, and how the system would come to a final chaotic state, describing how the shape of the string , so the nature of the distribution of energy among higher and higher keys. But nothing of the kind happened. To our surprise, the string began to play only on a few deaf notes and, which is probably even more striking, after several hundreds of ordinary reciprocating vibrations, it again took almost the same sinusoidal shape as at the beginning.


I know that Fermi considered this a “minor discovery,” as he himself said. But he was going to tell about him a year later, when he was invited to give a lecture by Gibbs (a very honorable event at the annual meeting of the American Mathematical Society). He fell ill before the meeting, and this lecture never took place. However, a report on this work, written by Fermi, Pasta and me, was nevertheless published - as a report on work in Los Alamos.


I must explain that the motion of a continuous medium, such as a string, for example, can be investigated using a computer if we imagine that a string consists of a finite number of particles - in our case, sixty-four or one hundred and twenty-eight. (The number of elements is better represented as some power of two, since this facilitates processing on a computer.) These particles are interconnected by forces that, in addition to distance-linear terms, also contain small nonlinear quadratic terms. Then the machine quickly calculates the movement of each of these points in short time steps. Having calculated one position, she goes to another time stage and calculates a new position, and so it repeats itself many times. There is absolutely no way to do this calculation manually, it would take literally thousands of years. The solution in an analytical form using mathematical methods of classical analysis of the nineteenth and twentieth centuries is completely unacceptable here.


The results were truly astounding. Many attempts have been made to elucidate the causes of such periodic and regular behavior, which has become a source for the voluminous literature on nonlinear oscillations existing today. Work on them was written by Martin Kruskal, a physicist from Princeton, and Norman Zabuski, a mathematician who worked in the Bell Telephone Laboratory. Later, Peter Lake made a brilliant contribution to this theory. All of them conducted an interesting analysis of problems of this kind. The mathematician knows that the so-called returning Poincare dynamical system, which includes so many particles, has a gigantic length - in fact, on an astronomical scale - and that it quickly returns to its original position is most surprising.


Another physicist from Los Alamos, James So, decided to see if the period following this very close return to the initial position begins again from the same state, and what will happen after this second “period”. Together with Pasta and Metropolis, he repeated the whole procedure, and, surprisingly, the return occurred again, but with an accuracy less than about one percent. This picture was repeated further, but after six or twelve such periods, the accuracy began to increase again, which indicated the appearance of a kind of “super period”. So, one strangeness was followed by another, no less.



And here is an article on Habré, telling about the current state of the Fermi-Pasta-Ulam problem:
Mathematicians solved the Fermi-Pasta-Ulam problem


5. Coordination


By system coordination, I understand the definition of basic parameters, which in principle determine the evolution of the system. For example, in the mechanics of a material point, the coordination is defined by:



The evolution of the system is given by Newton's equation


(d2r(t))/(dt2)=(F(t))/m


What is the coordination of the economic entity? I once worked on a business intelligence system. Its main term is indicator. The basis of the system is a scorecard. Hundreds of indicators. But I searched in vain on the Internet for a description of the basis of indicators - a set of indicators that cannot be reduced to others and which, in principle, completely determine the evolution of an economic entity. That is, as I understand it, no coordination has been made in the economy. And, therefore, talking about some basic dynamic law is not yet possible. It is only possible, based on the connection of indicators, to conduct a scenario analysis - to answer the question “What will happen to the derived indicators if the underlying indicators will change according to the given scenario?”


6. Abstract example. Time Series Forecasting Like Physics


You can ask the forecasting problem based on the actual time series: having a number of real values, you need to get the predicted value of the indicator - the value in the future. This suggests a kind of hidden determinism of the time series. There were many scientific and pseudo-scientific speculations on this subject. I myself dealt with doctors of sciences who claimed that their methodology would allow them to obtain an exchange rate forecast and showed the corresponding dissertations with all sorts of confidence intervals and other attributes of distribution laws. But, when confronted with reality, the techniques were blown away.


Sometimes to get a forecast do this:


  1. Take the real time series {V (ti)}. Schedule - step broken line.
  2. Take a continuous function W (t) such that W (ti) = V (ti). The graph is a continuous curve.
  3. A polynomial P (t) is selected that approximates W (t) with a sufficient degree of accuracy. A polynomial can be considered for all t.
  4. Then we have a forecast for future time T: V (T) = P (T)
    All this gives the impression of science, but only at first glance. Yes, the existence of an approximating polynomial for W (t) is guaranteed by the Weierstrass theorem from matanalysis. We can polynomize W (t) arbitrarily precisely. But it cannot be used for predictions.

The approximative value for the real series is 100%, and the predictive value is zero. Polynomials can be invented arbitrarily, but they will all give different forecasts.


When day T arrives and we find out the real V (T), then for the series {{V (ti)}, V (T)} we can construct a new polynomial Q (t) which approximates this series arbitrarily exactly, but the time T is no longer in the future and Q (T) is no longer a forecast, but a reality. The polynomials P (t) and Q (t) absolutely do not have to coincide, and for the new forecast time T '> T they will show different results. That is, there is no forecast. There seems to be science, but no forecast. This is like the medieval theory of angels. She can explain everything, but she cannot predict anything.


The difference between physical interpolation and extrapolation from economic:



7. Economics and physics


In economics, real trajectories — essentially discontinuous — are piecewise constant functions. For example, the “Currency rate” indicator can make a jump at any time. Continuous economic functions - approximations for the sake of matanalysis (if you have a hammer in your hands, then you want to consider any object as a nail ...). Each accounting transaction causes jumps in the values ​​of indicators of derivatives from accounts. And they are the majority of indicators. Further, each change in the number of workers is discrete, etc. The continuity of economic trajectories contrasts with the continuity of most physical trajectories. Therefore, the apparatus of matanalysis is not directly applicable to economic trajectories.


Picture for physical cognition. The trajectory of a stone thrown at an angle to the horizon


Picture for economic knowledge. The exchange rate at the central bank.



This is a real experimental exact function. It is discontinuous at points in time when the exchange rate changes.


In physics:



In economics:



Economic knowledge has not reached a level similar to classical mechanics:


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Summary


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Source: https://habr.com/ru/post/460833/


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