STATIONARY QUANTUM STATES IN THE CARDIO- PULMONARY SYSTEM

Similar documents
PROCESSES WITH QUANTUM JUMPS IN THE CARDIO-PULMONARY SYSTEM

Stoian PETRESCU 1, Bogdan BORCILA 1, *Monica COSTEA 1, Romi BOLOHAN 2, Valeria PETRESCU 1, Michel FEIDT 3, Georgeta BOTEZ 4

CIRCADIAN CYCLES OF THE CARDIO-PULMONARY SYSTEM STUDIED IN QUANTUM BIOLOGICAL THERMODYNAMICS WITH FINITE SPEED

WHAT IS QUANTUM BIOLOGICAL THERMODYNAMICS WITH FINITE SPEED OF THE CARDIO-PULMONARY SYSTEM: A DISCOVERY OR AN INVENTION?

GRAPHO-ANALYTICAL METHOD FOR CALCULLATING IRREVERSIBILITY PROCESSES WITH FINITE SPEED

, an adiabatic expansion machine, an isothermal compression machine at T L

Concepts and fundamental equations in Thermodynamics with Finite Speed

THE COEFFICIENT OF REGENERATIVE LOSSES IN STIRLING MACHINES

ENTROPY GENERATION ANALYSIS AND COP EVALUATION FOR A REVERSED QUASI-CARNOT CYCLE

THEORETIC AND EXPERIMENTAL RESEARCH ON THE CHARACTERISTIC DIAGRAMS OF A NEW TYPE OF ROTATING MACHINE WITH PROFILED ROTORS

CARNOT CYCLE WITH EXTERNAL AND INTERNAL IRREVERSIBILITIES ANALYZED IN THERMODYNAMICS WITH FINITE SPEED WITH THE DIRECT METHOD

COMPARISON BETWEEN THERMAL MACHINES AND FUEL CELL TREATMENT IN THE FRAMEWORK OF THERMODYNAMICS WITH FINITE SPEED

Chapter 16 Thermodynamics

(prev) (top) (next) (Throughout, we will assume the processes involve an ideal gas with constant n.)

REFRIGERATION CYCLES WITH VAPOR TREATED WITH THE DIRECT METHOD FROM FINITE SPEED THERMODYNAMICS (TFS)

Spring_#7. Thermodynamics. Youngsuk Nam.

Engineering Thermodynamics. Chapter 5. The Second Law of Thermodynamics

ME 200 Final Exam December 12, :00 a.m. to 10:00 a.m.

THERMODYNAMICS b) If the temperatures of two bodies are equal then they are said to be in thermal equilibrium.

Downloaded from

Irreversible Processes

CHAPTER - 12 THERMODYNAMICS

Chapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

A METHOD FOR DETERMINING THE PERFORMANCES OF STIRLING MACHINES BASED ON THE FIRST LAW FOR PROCESSES WITH FINITE SPEED AND USING A PV/PX DIAGRAM

Lecture 44: Review Thermodynamics I

Heat What is heat? Work = 2. PdV 1

Thermodynamics: The Laws

Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Existing Resources: Supplemental/reference for students with thermodynamics background and interests:

THERMODYNAMICS. Chapter Twelve MCQ I

Handout 12: Thermodynamics. Zeroth law of thermodynamics

(1)5. Which of the following equations is always valid for a fixed mass system undergoing an irreversible or reversible process:

Chapter 11 Heat Engines and The Second Law of Thermodynamics

University of Washington Department of Chemistry Chemistry 452 Summer Quarter 2014

IMPROVING ELECTRIC ARC FURNACE (EAF) OPERATION THROUGH MATHEMATICAL MODELLING

Heat engines and the second law of thermodynamics

A Numerical Model of Regenerator Based on Lagrange Description

Classical thermodynamics

October 18, 2011 Carnot cycle - 1

Distinguish between an isothermal process and an adiabatic process as applied to an ideal gas (2)

Handout 12: Thermodynamics. Zeroth law of thermodynamics

MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING Thermal-Fluids Engineering I

TWO BOUNDARY ELEMENT APPROACHES FOR THE COMPRESSIBLE FLUID FLOW AROUND A NON-LIFTING BODY

STUDY OF FLOW AT THE AIR WATER INTERFACE

Compression Losses In Cryocoolers

ME Thermodynamics I. Lecture Notes and Example Problems

Thermodynamics of Fluid Phase Equilibria Dr. Jayant K. Singh Department of Chemical Engineering Indian Institute of Technology, Kanpur

MULTIPHYSICS FINITE ELEMENT MODEL OF A CONTINUOUS THIN METALLIC SHEETS HEATER WITH ROTATING PERMANENT MAGNETS SYSTEM

Nonlinear Thermodynamic Analysis and Optimization of a Carnot Engine Cycle

Chapter 1 Introduction and Basic Concepts

Lecture 7, 8 and 9 : Thermodynamic process by: Asst. lect. Karrar Al-Mansoori CONTENTS. 7) Thermodynamic process, path and cycle 2

Optimization and entropy production: application to Carnot-like refrigeration machines

ASPECTS REGARDING NUMERICAL MODELING OF INDUCTIVE HEATING PROCESS FOR LOW VOLTAGE ELECTRICAL CABLES

Thermodynamic Systems, States, and Processes

Chapter 12. The Laws of Thermodynamics

The Kelvin-Planck statement of the second law

Physics 207 Lecture 27. Lecture 26. Chapters 18, entropy and second law of thermodynamics Chapter 19, heat engines and refrigerators

ME 200 Thermodynamics I, Spring 2015, Exam 3, 8 p.m. to 9 p.m. on April 14, 2015

Chapter 12. The Laws of Thermodynamics. First Law of Thermodynamics

Lecture 26. Second law of thermodynamics. Heat engines and refrigerators.

Chapter 4 ENERGY ANALYSIS OF CLOSED SYSTEMS

DEZVOLTAREA REGIONALĂ PRIN TURISM

An introduction to thermodynamics applied to Organic Rankine Cycles

Modeling and Analysis of Dynamic Systems

The Second Law of Thermodynamics. (Second Law of Thermodynamics)

Minimum Bias Events at ATLAS

DETERMINISTIC AND PROBABILISTIC SEISMIC PERFORMANCE ASSESSMENT OF A LOW-CODE RC FRAME BUILDING

Introduction to Aerospace Propulsion. Prof. Bhaskar Roy. Prof. A. M. Pradeep. Department of Aerospace Engineering

Irreversible Processes

Mechanical Analysis of Genoa 03 Stirling Engine

Electrical Analogy of Liquid Piston Stirling Engines

5/6/ :41 PM. Chapter 6. Using Entropy. Dr. Mohammad Abuhaiba, PE

BME-A PREVIOUS YEAR QUESTIONS

Thermodynamics 1 Lecture Note 2

The First Law of Thermodynamics

w = -nrt hot ln(v 2 /V 1 ) nrt cold ln(v 1 /V 2 )[sincev/v 4 3 = V 1 /V 2 ]

Chapter 19 The First Law of Thermodynamics

OBSERVABILITY AND SINGULARITY IN THE CONTEXT OF RÖSSLER MAP

A GENERALIZATION OF A CLASSICAL MONTE CARLO ALGORITHM TO ESTIMATE π

THERMODYNAMICS CONCEPTUAL PROBLEMS

Chapter 19. Heat Engines

THE CURRENT INDUCED CALCULATION IN CLAW POLE OF AN ALTERNATOR BY FINITE ITE ELEMENT METHOD

NEW HORIZON PRE UNIVERSITY COLLEGE LESSON PLAN FOR THE ACADEMIC YEAR Department of PHYSICS ( I PUC)


ME 200 Final Exam December 14, :00 a.m. to 10:00 a.m.

THERMODYNAMICS NOTES. These notes give a brief overview of engineering thermodynamics. They are based on the thermodynamics text by Black & Hartley.

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 32: Heat and Work II. Slide 32-1

8.21 The Physics of Energy Fall 2009

ME2320 Thermodynamics I. Summer I Instructor: Dr. William W. Liou

Classification following properties of the system in Intensive and Extensive

SECOND LAW OF THERMODYNAMICS

Chapter One Reviews of Thermodynamics Update on 2013/9/13

Reversibility, Irreversibility and Carnot cycle. Irreversible Processes. Reversible Processes. Carnot Cycle

University of Engineering & Technology Lahore. (KSK Campus)

UBMCC11 - THERMODYNAMICS. B.E (Marine Engineering) B 16 BASIC CONCEPTS AND FIRST LAW PART- A

THE OPTICAL STARK EFFECT IN PARABOLIC QUANTUM WELL WIRES UNDER HYDROSTATIC PRESSURE

The first law of thermodynamics. U = internal energy. Q = amount of heat energy transfer

STUDIES ON THE MESOMORPHIC STATE OF THE STEARIC ACID

Chapter 12 Thermodynamics

Chapter 7. Entropy: A Measure of Disorder

Transcription:

STATIONARY QUANTUM STATES IN THE CARDIO- PULMONARY SYSTEM Stoian Petrescu 1, Monica Costea 1, Valeria Petrescu 1, Radu Bolohan 3, Nicolae Boriaru 1, Adrian S. Petrescu 2, B. Borcila 1 1 University Politehnica of Bucharest 2 Bellevue University, Greater Omaha, Nebraska, USA 3 Clinical Centre of Emergency Medicine in Cardiovascular Disease Dr. Constantin Zamfir Bucharest, Clinic of Cardiology, Arrhythmology and Electrophysiology ABSTRACT: The proposed paper presents the results of systematic theoretical and experimental research with the goal of applying and extending Thermodynamics with Finite Speed to the human Cardio-Pulmonary System. Using experimental methods we discovered Stationary Quantum States correlating the working frequency of the heart with that of the lungs through a Quantified Equation built around an integer number dependent on the characteristics of the person and on the effective position of the body. Diagrams illustrating these States for persons of different age categories lead to the conclusion that the same pattern holds for all healthy ones. Keywords: Quantum Biological Thermodynamics with Finite Speed, Stationary Quantum States, Cardio-Pulmonary Quantum interaction, Quantum Numbers in Heart-Lung interaction, Heart Disease, Lung Disease. STARI CUANTICE STATIONARE ALE SISTEMULUI CARDIO-PULMONAR - REZUMAT: Lucrarea propusă prezintă rezultatele unei cercetări sistematice teoretice şi experimentale cu scopul de a aplica şi extinde Termodinamica cu Viteză Finită la sistemul cardiopulmonar uman. Utilizând metode experimentale am descoperit stări staționare cuantice care corelează frecvența bătăilor inimii cu cea a respirației printr-o relație cuantificată construită în jurul unui număr întreg dependent de caracteristicile persoanei şi de poziția efectivă a corpului ei. Diagramele ilustrând aceste stări ale persoanelor de diferite categorii de vârstă conduc la concluzia că modelul este acelaşi pentru toţi cei sănătoşi. Cuvinte cheie: Termodinamică Biologică Cuantică cu Viteză Finită, Stări staționare cuantice, Interacțiune cardio-pulmonară cuantică, Numere cuantice în interacțiunea inimă-plămâni, boli de inimă, boli de plămâni. 1. INTRODUCTION This might be the beginning of a new branch of Thermodynamics of irreversible processes that we called Biological Quantum Thermodynamics with Finite Speed for Cardio-Pulmonary Systems (CPS). This is in fact an extension of the Thermodynamics with Finite Speed (TFS) already validated for Thermal Machines that began by the seminal papers of Lazăr Stoicescu, Stoian Petrescu and Valeria Petrescu (1964) when a new expression of the First Law of Thermodynamics for Irreversible Processes with Finite Speed was discovered/invented (Stoicescu and Petrescu, 1964a): du aw δqirr pm, i 1 (1) dv c This new equation has been applied to all five irreversible processes (isothermal, isochoric, isobaric, adiabatic and polytropic) (Stoicescu and Petrescu, 1964b, 1965a) and to Irreversible Thermodynamic Cycles (Stoicescu and Petrescu, 1965b).

STATIONARY QUANTUM STATES IN THE CARDIO-PULMONARY SYSTEM 197 Case of R f = 2 (N=0) R f = F H/ F L = / = 2/1 = 2 Case of R f = 3 (N=4) R f = F H/ F L = / = 3/1 =3 Case of R f = 4 (N=8) R f = F H/ F L = / = 4/1 =4 Fig.1. Explaining Diagrams for Frequency Ratios R f = 2; 3; 4 and corresponding Integer Quantum Numbers N=0; 4; 8. Case of R f = 2.5 (N=2) R f = F H/ F L = / = 5/2 = 2.5 Case of R f = 3.5 (N=6) R f = F H/ F L = / = 7/2 =3.5 Fig.2. Explaining Diagrams for Frequency Ratios: R f =2.5 and 3.5 corresponding to Interactional Quantum Numbers: N= 2 and 6. In 1992 (1) was extended to processes with friction and throttling (Petrescu et al., 1992; Petrescu and Harman, 1994): aw p p f du δq p thr f (2) irr m,i 1 dv c pm,i p m,i A lot of papers were dedicated since to the study of several Thermal Machines operating with irreversible cycles with finite speed (Petrescu and Harman, 1994, 2001; Costea, 1997; Dobre, 2012; Enache and Petrescu, 2012a, b; Petrescu et al., 2014a, b; Enache et al., 2015b; Petrescu and Enache 2013c), culminating with some extremely important (Petrescu et al., 1992, 2002, 2010; Petrescu and Harman 1994). In 1993, based on research by V. Petrescu on Fuel Cells (Petrescu, 1969; Petrescu and Petrescu, 1971; Petrescu et al., 1993, 2013a, b), we extended TFS to

198 Lucrările celei de-a X-a ediţii a Conferinţei anuale a ASTR, 2015 Electrochemical Devices (Petrescu et al., 1993). A few years ago, in 2012, we opened a new domain of research on Biological Systems (Petrescu and Harman, 2001; Costea, 1997; Dobre, 2012; Enache and Petrescu, 2012a, b; Petrescu and Enache 2013c; Petrescu et al., 2014a, b, c, d; Enache et al., 2015a). 2. ELECTROCHEMICAL-MECHANICAL MODEL OF THE CARDIO- RESPIRATORY SYSTEM Considering the skeletal muscles as well as the myocardium (heart) and pulmonary muscles as electrochemical - mechanical machines in motion, we started to work at TFS extension to Biological Systems. We began by regarding the Heart as a blood (liquid) pump and the Lungs as two parallel air compressors. In our first attempt to treat human CPS we considered the processes taking place inside it as continuous (Enache and Petrescu, 2012a, b; Petrescu and Enache 2013c; Petrescu et al., 2014b, c; Enache et al., 2015). Experimental researches aiming to validate the findings from these papers allowed us to discover the quantifying of the interaction between Heart and Lungs as oscillating Thermal Machines (a pump in interaction with two air compressors). The very successful validation for Stirling Machines (13 engines - Petrescu et al., 2002, 4 Solar Stirling Engines - Dobre, 2012) and also for Refrigerating Machines and Compressors (Dobre, 2012) justified our confidence that we could do something similar for the human CPS too. With the goal of applying the First Law for irreversible Processes with Finite Sped, friction and throttling (2) to the human CPS, we invented a new diagram PV/px similar to that for two pistons Stirling Machines (Petrescu et al., 2002, 2014a, 2015a). 3. STATIONARY QUANTUM STATES The two previously mentioned frequencies may be constant (for minutes, tens of minutes or even hours) in what we called stationary quantum states (SQS), while sleeping, sitting on a chair, walking, doing repetitive physical work etc. As by applying statistical methods to the experimental data (Petrescu et al., 2014a, 2015a), a correlation between the speeds of the pump and that of the compressors could not be obtained, in a completely new approach suggested by our previous results (Petrescu et al., 2014a), the big surprise was the discovery (Petrescu et al., 2015a) of the following formula: F H = F L. (2+ N/4) (3) where F H is the Frequency of the Heart beat (Pulse) and F L the Frequency of the Lungs (the Respiratory Rhythm) [oscillations / minute]. Their ratio R f = F H /F L (Petrescu et al., 2014a, 2015a) represents a new parameter of state characterizing a stationary state of interaction between the two subsystems Heart-Lungs. The most amazing discovery was the fact that this correlation (3) is valid for all healthy persons, despite of the fact that the domain of values of N depends on the person (Fig. 3). 4. EXPLANATION OF FREQUENCY RATIO VALUES FOR STATIONARY QUANTUM STATES A phenomenological explanation of formula (3), for integer and non integer values of the Frequency Ratio R f in all SQS results from Figure 1and 2. The corresponding integer values of the Quantum Number N which characterize an interaction state between Heart and Lungs, as oscillatory sub-systems of the CPS resulted from (3). In Fig. 3 are presented processes with quantum jump, observed at 5 kids (aged between 9 and 13 years), by the change of their position between 3 stationary states, from horizontal, to sitting and finally to vertical. They conducted these experiments by themselves following the research protocol, and without my (S.P.) intervention, in order to be certain of their objective observations and measurements. It is interesting to see how, as different as they are, (3) still holds for all of them. Similar results were experimentally obtained for 50 mature persons (master students - Advanced Thermodynamics Course at UPB, in 2013 and 2014). From these results comes our belief that (3) could be valid for any healthy person. In Figure 4, we present another diagram illustrating processes with quantum jump for the same person (S.P.), between SQS, from one stationary state to another, during one day. In all stationary states (3) was validated. Very interesting is also the fact, recently discovered by L. Timofan et al. (Petrescu et al., 2014a), that in the case of Bowen Therapy, the Relaxation can be achieved also by the patient himself, passing his CPS, step by step, through a succession of SQS. We have already observed, in fact, that in many other Relaxation Techniques (as: Reflexo-therapy, Reiky, Massage, Yoga, Silva, etc.) the same behavior of the healthy CPS appears, by improving the ratio R f. 5. CONCLUSIONS AND PERSPECTIVES In this paper we gave a phenomenological explanation for two extremely important experimental discoveries, namely:

STATIONARY QUANTUM STATES IN THE CARDIO-PULMONARY SYSTEM 199 1. The quantification of parameters of state F H, F L and N in what we introduced as a new concept: Stationary Quantum States in the Heart Lungs Interactional System (CPS). Fig. 3. Quantum jump processes for 5 kids, while changing their posture: 1-2 horizontal position states; 2-3 process with changing position; 3-4 sitting on a chair states; 4-5 process with changing position; 5-6 vertical position states. Fig. 4. Change of R f and N during processes with quantum jump (for SP). To each value of R f, an integer value of the quantum number N, from (3) corresponds.

200 Lucrările celei de-a X-a ediţii a Conferinţei anuale a ASTR, 2015 2. The correlation between these 3 parameters of state, expressed by a quantum formula (3) was validated, based on thousands of experiments on 50 persons. These discoveries are the basis (fundamentals) of the Development of what we called: Quantum Biological Thermodynamics with Finite Speed for CPS. Combining (3) with the concept of quantum jump processes, in another paper we developed the description of these processes in 5 diagrams (Petrescu et al., 2015b). Using these new concepts, formula (3) and diagrams combined with the new equation of the First Law for Processes with Finite Speed (1 and 2) these irreversible processes can be described quantitatively, in a way similar with how we did already for Thermal Machines in the Thermodynamics with Finite Speed (Petrescu et al., 2014c). Last but not least, we would like to thank very much to the five children-students: Ana, Emma, Bianca, Crista and Vlad for their very important help in this experimental research. They did it with great enthusiasm and very seriously. REFERENCES Costea, M., (Advisers: S. Petrescu and M. Feidt), Improvement of heat exchangers performance in view of the thermodynamic optimization of Stirling Machine; Unsteady-state heat transfer in porous media, Ph.D. Thesis, UPB & U.H.P. Nancy 1, 1997. Dobre, C., (Advisers: S. Petrescu, P. Rochelle), Contribution to the Development of Some Methods of Irreversible Engineering Thermodynamics Applied to the Analytical and Experimental Study of Stirling and cvasi-carnot Machines, Ph.D. Thesis, U. P. Bucureşti U. Paris X, 2012. Enache V., Petrescu S., Algoritm local pentru optimizarea costului rețelelor arborescente de conducte, Proceedings of the VIIth Edition of the Int. Conf. ACADEMIC DAYS of The Academy of Technical Science in Romania, Bucharest, pp. 236, Editura AGIR, Bucureşti, România, 2012a. Enache, V., Petrescu S., Optimizarea costului instalațiilor arborescente de transport, Rev. Termotehnica, XVI, 2/2012, p. 4, Ed. AGIR, Bucureşti, 2012b. Enache, V., Petrescu, S., Bolohan, R., Condiții de optim în sistemul Cardio-Vascular-Pulmonar obținute în cadrul Termodinamicii Ireversibile cu Viteză Finită. II. Optimizarea puterii utile furnizate de organism, Rev. Chim., 2015 (in press). Petrescu, S., (Adviser: L. Stoicescu), Contribution to the study of thermodynamically non-equilibrium interactions and processes in thermal machines, Ph.D. Thesis, I.P.B., Bucharest, Romania, 1969. Petrescu, V., Petrescu, S., A Treatment of the Concentration Overpotential Using the Thermodynamics of Irreversible Processes, Revue Roumaine de Chimie, Romanian Academy, 16, 9, 1291-1296, 1971. Petrescu, V., (Adviser: S. Sternberg), Electrode Processes and Transport Phenomenon at the interface of Chlorine-Carbon Electrode-Molten Salt, PhD Thesis, I. P. Bucureşti, 1974. Petrescu, S., Lectures on New Sources of Energy, Helsinki University of Technology, Otaniemi, Finland, p.320, Lectures in October 1991. Petrescu, S., Stanescu, G., Iordache, R., Dobrovicescu, A., The First Law of Thermodynamics for Closed Systems, Considerring the Irreversibilities Generated by the Friction Piston-Cylinder, the Throttling of the Working Medium and Finite Speed of the Mechanical Interaction, Proc. of ECOS'92, Zaragoza, Spain, Ed. A. Valero, G. Tsatsaronis, ASME, 33-39, 1992. Petrescu, S., Petrescu, V., Stanescu, G., Costea, M., A Comparison between Optimization of Thermal Machines and Fuel Cells based on New Expression of the First Law of Thermodynamics for Processes with Finite Speed, Proc. First International Thermal Energy Congress, ITEC - 93, Marrakech, Morocco, 1993. Petrescu, S., Harman, C., The Connection Between the First Law and Second Law of Thermodynamics for Processes with Finite Speed - A Direct Method for Approaching and Optimization of Irreversible Processes, Journal of The Heat Transfer Society of Japan, 33, 128, 60-67, 1994. Petrescu, S., Zaiser, J., Petrescu, V., Lectures on Advanced Energy Conversion, Bucknell University, Lewisburg, PA, USA, 1996. Petrescu, S., Harman, C., The Jump of an Electron in a Hydrogen Atom using a Semi-classical Model, Rev Chim., Bucharest, English Edition, 2, 1-2, 3-10, 2001. Petrescu, S., Costea, M., Harman, C., Florea, T., Application of the Direct Method to Irreversible Stirling Cycles with Finite Speed, Int. Journal of Energy Research, 26, 589-609, 2002. Petrescu, S., Zaiser, J., Harman, C., Petrescu, V., Costea, M., Florea, T., Petre, C., Florea, T.V., Florea, E., Advanced Energy Conversion - Vol II, Bucknell University, Lewisburg, PA, USA, 2006a. Petrescu, S., Harman, C., Costea, M., Florea, T., Petre, C., Advanced Energy Conversion- Vol I, Bucknell University, Lewisburg, PA-17837, USA, 2006b. Petrescu, S., Petre, C., Costea, M., Boriaru, N., Dobrovicescu, A., Feidt, M., Harman C., A Methodology of Computation, Design and

STATIONARY QUANTUM STATES IN THE CARDIO-PULMONARY SYSTEM 201 Optimization of Solar Stirling Power Plant using Hydrogen/Oxygen Fuel Cells, Energy, 35, 729 739. 2010. Petrescu, S., Costea, M., et al., Development of Thermodynamics with Finite Speed and Direct Method, Editura AGIR, Bucureşti, România, 2011. Petrescu, S., Maris, V., Costea, M., Boriaru, N., Stanciu, C., Dura, I., Comparison between Fuel Cells and Heat Engines. I. A Similar Approach in the Framework of Thermodynamics with Finite Speed, Revista de Chimie, 64, 7, 739-7461, 2013a. Petrescu, S., Maris, V., Costea, M., Boriaru, N., Stanciu, C., Dura, I., Comparison between Fuel Cells and Heat Engines. II. Operation and Performances, Revista de Chimie, 64, 10, 1187-1193, 2013b. Petrescu, S., Enache, V., Applying the Finite Speed Thermodynamics (FST) to the Human Cardiovascular System, National Conf. of Thermodynamics. (NACOT), Constanta, 2013c. Petrescu, S., Costea, M., Timofan, L., Petrescu, V., Means for qualitative and quantitative description of the Cardio-Pulmonary System Operation within Irreversible Thermodynamics with Finite Speed, ASTR Conference, Sibiu, 2014a. Petrescu S., Feidt M., Costea M., Enache V., Petre C., Boriaru N., Perspective d unification de la Thermodynamique en Dimensions Physiques Finies avec la Thermodynamique à Vitesse Finie, COFRET'14, Paris, CNAM, 2014b. Petrescu, S., Petrescu, V, Costea, M., Timofan, L., Danes, S., Botez, G., Discovery of Quantum Numbers In the Cardio-Pulmonary Interaction. studied In Thermodynamics with Finite Speed, ASTR Conference, Sibiu, 6-7 November, 2014c. Petrescu, S., Costea, M, Petrescu, A.S., Petrescu, V., From Thermodynamics with Finite Speed toward Quantum Biological Thermodynamics with Finite Speed, NACOT Conference, Iasi, 2015a. Petrescu, S., Costea, M., Petrescu, V., Bolohan, R., Petrescu, A.S., Boriaru, N. Stationary Quantum States in the Cardio-Pulmonary System. Conferinta ASTR-Galati, 9-10 Octombrie, 2015b. Petrescu S., Enache V, Bolohan R., Condiții de optim în sistemul Cardio-Vascular-Pulmonar obținute în cadrul Termodinamicii Ireversibile cu Viteză Finită, I. Debitul de oxigen în funcție de viteza sângelui, Rev.Chim., București. 2015c, (In Press). Stoicescu, L., Petrescu, S., The First Law of Thermodynamics for Processes with Finite Speed, in Closed Systems, Bulletin I.P.B., Bucharest, Romania, XXVI, 5, 87-108, 1964a. Stoicescu, L., Petrescu, S., Thermodynamic Processes Developing with Constant Finite Speed, Bull. I.P.B. Romania, XXVI, 6, 79-119, 1964b. Stoicescu, L., Petrescu, S. Thermodynamic Processes with Variable Finite Speed, Buletin I.P.B., Romania, XXVII, 1, 65-96, 1965a. Stoicescu, L., Petrescu, S., Thermodynamic Cycles with Finite Speed, Bulletin I.P.B., Bucharest, Romania, XXVII, 2, 82-95, 1965b. Stoicescu, L., Petrescu, S., The Experimental Verification of The New Expression of the First Law for Thermodynamic Processes with Finite Speed, Bull. I.P.B., Bucharest, XXVII, 2, 97-106, 1965c.