Rodolfo Sergio González Castro. HAL Id: hal v2

Size: px
Start display at page:

Download "Rodolfo Sergio González Castro. HAL Id: hal https://hal.archives-ouvertes.fr/hal v2"

Transcription

1 Equation of the force of gravity resulting from the Planck Energy/Area and wavelength of De-Broglie without using the Universal Gravitation Constant Newton. Rodolfo Sergio González Castro To cite this version: Rodolfo Sergio González Castro. Equation of the force of gravity resulting from the Planck Energy/Area and wavelength of De-Broglie without using the Universal Gravitation Constant Newton <hal v2> HAL Id: hal Submitted on 19 Feb 2014 (v2), last revised 25 Mar 2014 (v8) HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

2 Equation of the force of gravity resulting from the Planck Energy/Area and wavelength of De-Broglie without using the Universal Gravitation Constant of Newton. Rodolfo Sergio González Castro Research Institute, University of Tijuana CUT, Av. Lucrecia Borja 1010, Col. Altamira, Tijuana, Baja California, Mexico. CP BA in Psychology, MSc. Administration General (MBA), MSc. Education, PhD candidate in Education, Theoretical Physicist Autodidact. Abstract In this paper I show that it is possible to calculate the force of gravity deriving an equation of the Planck Energy/Area and wavelength of De-Broglie associated with particles or massive objects in gravitational interaction without use the universal gravitational constant of Newton (G). OAI: hal.archives-ouvertes.fr:hal PACS: Kd Newton Keywords: physics, particles, gravity, gravitation constant, 1. INTRODUCTION The mathematical physicist Sir Isaac Newton in 1687 published his book "Philosophiae Naturalis Principia Mathematica" where he presented the law of universal gravitation empirically derived to describe and calculate quantitatively the mutual attraction of each particle and massive objects in the universe. In that document, Newton concluded that the attraction together two bodies is proportional to product of their masses and inversely proportional to the square of the distance that separates them. However, these must be adjusted proportionalities by introducing a constant called Universal Gravitation (G) with an approximate value of N m2 kg-2 units in the International System. Without the introduction of this constant, the equation, lose their rationality and is impractical to calculate the force of gravity without it. For Newton, gravity is considered a force exerted on a remote Instant. Moreover, when the gravity force is exerted by two or more bodies extremely mass, Newton's law has serious limitations and then must resort to the Theory of Relativity General stated by Albert Einstein in 1915, who says that gravity is not a force exerted to distance but a contraction of Space-Time produced by the presence of matter (1). However in the final formulation of the equations of the universe, to make it compatible with the law of conservation of energy and principles of general covariance and minimal coupling, Einstein included mathematical concepts such as the Ricci Tensor and scalar, but mainly the energymomentum tensor, but fails to integrate into

3 said Energy-Momentum Tensor the constant Universal Gravitation Newton, as this is finally out in the second member of the equation. While Einstein equation establishes the relationship between gravity, energy and geometry distortions spacetime, it does not define the origin of the relationship. Subsequently in 1995 Jacobson linked the laws of thermodynamics to the Einstein equation and the equation of state correlates with entropy the energy sector flow (2). Erik Verlinde published on January 6, 2010, his work "On the Origin of Gravity and the Laws of Newton" (3), which proposed that gravity is a reality entropic force emerging space. In its formulation, includes reduced Planck's constant, N as a Screen of information bits of space, adds a new constant called G, which ultimately Accounts found to be equivalent to the Universal Gravitational Constant. On that basis, Verlinde forecast to gravity as a fundamental force. In March 2010, Jae-Weon Lee, Hyeong-Chan Kim and Lee Jungjai published a paper in which suggest that the Einstein equation can be derived from the principle of Landauers on the Elimination of information causal horizons, and conclude that gravity has its origin in quantum information (4). From then such work is also supported by Jacobson linking between thermodynamics and the equation Einstein, as well as on the work of Verlinde entropic force. Thus, we already have a strong linkage between energy, heat, laws of thermodynamics, theory general relativity, perturbation of the geometry of space-time, entropy and quantum information, but somehow linking gravity and electrostatic force has been fails to integrate in all this work to finally derive the Einstein equation and the gravitational constant universal. From my point of view, crucial to successfully solve the equations of gravity aspect is the distribution of Plank area, and both invariance in all particles and massive objects in the universe, as discussed in this paper. Derive a gravity equation that eliminates the universal gravitational constant and link strength gravity with the electrostatic force requires on the one hand make Planck area invariant, and include in the equation the length of De Broglie wave. I.-GRAVITATIONAL ENERGY DERIVED FROM PLANCK ENERGY/AREA Newton's equation establishes the relationship between mass and gravity, while the equation Einstein relates the Energy-Momentum Tensor with the modification or distortion of space, which is more proper perspective proposed here, including in the case of particles resting or non-relativistic speeds. For particles at rest, Einstein's equation defines the Energy-Momentum tensor in the coordinate time (t). I mean, you have a single source of tension, so the above equation requires the universal gravitational constant outside the tensor. This work is based on the priori hypothesis that particles resting actually have two sources of tension at different times (t) with different effects in terms of pressure on space. The first source of tension generated electrostatic force, while the second source of tension is the cause of the gravitational force. To explain this I have to consider the existence of a hypothetical particle whose Plank energy

4 distribution in space is the area of a perfect square: Y = = = 1, E-34 m X = = = 1, E-34 m electrostatic effects and Gravity effects are "visible" to outside observers. In other words, the ratio of Planck Area is invariant in all of the particles and objects mass of the universe when they are at rest or non-relativistic speeds. Here graphically proportional representation of an electron according to Planck Energy/Area: Y = = 4, E-57 m Both the axis (X) and the axis (Y) corresponding to the Planck length. Both faces of the square axes exert pressure on space, or in terms of Einstein, Energy-Momentum produce tensor. In the Axis (X) the Energy- Momentum tensor is exactly the same as Einstein or first source of tension, but for axis (Y) still corresponds to second source of tension or gravity source. However, in the case of the hypothetical Plank particle, because both axes or faces have equal length, and in the case of (Y) perpendicular pressure is negative and therefore, the two pressures or two source of tension cancel each other. In terms of the De Broglie wavelength to be exactly equal in length and amplitude but opposite to each other, they cancel each other, so that an external observer can t capture the presence of the Planck particle in electrostatic or gravitational terms. It is then a "Null particle" or "Space Empty". By the law of conservation of the area, or a hypothetical "law of conservation of space, an electron or any other particle in the universe always retain the same area of Plank. if the (X) axis is lengthened, then proportionally axis (Y) will be shortened. But also at the time at which the lengths (X) and the lengths (Y) are different, they stop cancel each other and the X = = = 2, E-12 m Note: The graph of the rectangle is not exactly proportional to the scalar quantities for obvious reasons. As will be seen, in the electron, because (X) is too extension with respect to the length of Planck, then (Y) is proportionally shortened and wavelength being excessively small but sufficient to generate gravitational effects of the electron. In other words, the particles are like strings or threads whose extension in the X axis is much longer compared to the Planck length, but the width, height or thickness (Y axis) is very short. In this sense, the present work of the a priori hypothesis that all the specific objects universe and all clusters of material occupying a particular area of space, whether electrons, protons, atoms, planets, stars and galaxies, all can be considered as "particles" whose distribution of energy per occupied space area, rigorously meet the total Planck energy distributed in the Planck area or area of the particle according to the following equation: = (1.1)

5 Where Ep is Planck's energy and N is the ratio of the rest energy of any particle or object mass and the Planck energy given by the equation: (1.2) Substituting N into Equation (1.1) then the energy distribution in an area Planck is given by: (1.3) In this case (E) corresponds to the rest energy of any known particle or massive object, while (Eg) in equation described below corresponds to the "Gravitational Energy" not known so far (Virtual, dark, pop, entropic or whatever you want to call) existing in the area occupied by a visible particle or massive object, which although is not observable or detectable until now, its possible existence is the source of gravitational attraction. (1.4) Both the rest energy (E) as the gravitational energy (Eg), both have a wavelength according to the associated de Broglie postulates given by the familiar equation: That in the case of the gravitational energy, the corresponding equation is: The product of two wave lengths, corresponding to the wavelength of Planck: ( 1.5) Where h is Planck's constant and c is the speed of light, and where is the wavelength of Broglie energy at rest and is the gravitational wave length. 2. GRAVITATIONAL COUPLING Because the two wavelengths originate almost "simultaneous", the Wavelength gravitational be coupled to the wavelength of the rest energy, Generating a factor of coupling to the gravitational force given by: (2.1) Where is the factor of gravitational coupling. For the electrostatic force, value coupling is considered constant (Fine Structure), but, in the case of gravity, said coupling depends on the ratio of both wavelengths (and thus Energy) as shown in the equation THE EQUATION OF GRAVITY FORCE WITHOUT CONSTANT GRAVITATION Thus if we have defined or calculated the "Gravitational Energy" derived from the Planck Energy/Area, the De-Broglie wavelength associated Gravity and Gravitational coupling factor, we can then stating a priori an equation for the gravitational attraction between two particles or massive objects identical to or have the same amount of mass: = (3.1) And for the case of two different particles or objects mass: (1.6) = (3.2)

6 Then comes to be a general equation for calculating the force of gravity without the use of the gravitational constant of Newton and based on Planck Energy/area, and Wave length De Broglie. Moreover, due to the existence of a constant in this equation, it is possible to reduce it further. In this case the product of the energy (E) for its associated wavelength is constant: E-25 joules per meter (3.3) Which in turn we reduce as in the case of Planck's constant: E-26 joules per meter (3.4) Thus we can write a new equation for calculating the gravitational force between two equal mass particles or objects: = = (3.5) And for the interaction between two particles or different massive objects: = Thereupon (3.6) = (3.7) It is my final general equation for calculation of the force of gravity between two particles or objects mass. 4. DERIVATION OF EQUATION OF CALCULATION OF FORCE ELECTROSTATIC About the same arguments above, the calculation of the electrostatic force between two particles is still simpler due to electrostatic coupling constant or fine structure. In this case, we carried a broad general shall term a priori constant Electrostatic Universal Constant: per meter E-27 joules (4.1) No matter how much rest energy of the particle, the electrostatic force is always the same and will vary only based on the distance. That is, the calculation of the electrostatic force between two identical or different particles is given by the general equation: = = (4.2) Where E is the energy at rest, the wavelength of de Broglie, coupling constant or Fine structure, d is the distance between the two particles. But it is possible to reduce it to eliminate (2 Pi) in the equation: = (4.3) That is my general equation for calculating the electrostatic force between two identical particles or different. This equation is equivalent to Coulomb's law: = For the case of two particles in load electrostatic interaction. = = =

7 Again, I must point out here that the develop equations for calculating the force of gravity are for particles or massive objects at rest or in non relativistic speeds. My next job will be related to cases of relativistic velocities integrated into the Einstein Tensor. 5. CONCLUSION Having proven naturally and clean that gravity is possible to calculate from the Plank energy/area and De Broglie wavelength without using the gravitational constant Newton, paves the way for a unified theory of everything, and in that sense can assert a priori: 1.-That to calculate the electrostatic force of gravity in terms necessarily need to include the concept of "Gravitational Energy" derivative of the Planck energy/area. 2.-That the electrostatic force and the force of gravity can be calculated from the Planck Energy/area. 3.-That because the wavelength of the energy at rest and the wavelength of the "Energy Gravitational" originate form virtually "simultaneously" because this, the wavelength Gravity be coupled to the variable length of electrostatic wave form, which so far had hampered their electrostatically calculation. 4.-Developed here that the equation for the calculation of the force of gravity, is actually an equation electrostatic force, instead of using the fine structure constant, must use the variable gravitational coupling due to the argument of the previous paragraph. 5.-And I can finally conclude a priori, due to the equations presented here that the force of gravity It is also modulated by the variable electrostatic force of gravitational coupling. REFERENCES 1. Wald RM. General Relativity. University of Chicago Press; Available from: ISBN= Jacobson T. Thermodynamics of Spacetime: The Einstein Equation of State. arxiv.org. 1995;Phys. Rev.(qr-qc/ v2): Verlinde E. On the Origin of Gravity and the Laws of Newton. 2010;(arxiv: v1): Lee J, Kim H, Lee J. Gravity from Quantum Information. 2010;(arXiv: v2).

EQUATION OF FORCE OF GRAVITY DERIVED FROM THE AREA OF PLANCK INVARIANCE UNUSED UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON (G).

EQUATION OF FORCE OF GRAVITY DERIVED FROM THE AREA OF PLANCK INVARIANCE UNUSED UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON (G). EQUATION OF FORCE OF GRAVITY DERIVED FROM THE AREA OF PLANCK INVARIANCE UNUSED UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON (G). Rodolfo Sergio González Castro To cite this version: Rodolfo Sergio González

More information

GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON

GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON Rodolfo Sergio González Castro To cite this version: Rodolfo Sergio González

More information

GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON

GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON Rodolfo Sergio González Castro To cite this version: Rodolfo Sergio González

More information

GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON

GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON GRAVITATIONAL ACCELERATION EQUATION WITH WAVELENGTH AND SPEED OF LIGHT WITHOUT USING THE UNIVERSAL GRAVITATIONAL CONSTANT OF NEWTON Rodolfo Sergio González Castro Research Institute, University of Tijuana

More information

THEORY OF GRAVITY ENERGY-WAVE : THE ORIGIN

THEORY OF GRAVITY ENERGY-WAVE : THE ORIGIN THEORY OF GRAVITY ENERGY-WAVE : THE ORIGIN Rodolfo Sergio González Castro To cite this version: Rodolfo Sergio González Castro. THEORY OF GRAVITY ENERGY-WAVE : THE ORIGIN. New version. 2014.

More information

A new simple recursive algorithm for finding prime numbers using Rosser s theorem

A new simple recursive algorithm for finding prime numbers using Rosser s theorem A new simple recursive algorithm for finding prime numbers using Rosser s theorem Rédoane Daoudi To cite this version: Rédoane Daoudi. A new simple recursive algorithm for finding prime numbers using Rosser

More information

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Matthieu Denoual, Gilles Allègre, Patrick Attia, Olivier De Sagazan To cite this version: Matthieu Denoual, Gilles Allègre, Patrick Attia,

More information

Dispersion relation results for VCS at JLab

Dispersion relation results for VCS at JLab Dispersion relation results for VCS at JLab G. Laveissiere To cite this version: G. Laveissiere. Dispersion relation results for VCS at JLab. Compton Scattering from Low to High Momentum Transfer, Mar

More information

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle Nathalie Olivi-Tran, Paul M Gauthier To cite this version:

More information

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma.

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Loïc De Pontual, Delphine Trochet, Franck Bourdeaut, Sophie Thomas, Heather Etchevers, Agnes Chompret, Véronique Minard,

More information

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122,

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, 244902 Juan Olives, Zoubida Hammadi, Roger Morin, Laurent Lapena To cite this version: Juan Olives,

More information

Exact Comparison of Quadratic Irrationals

Exact Comparison of Quadratic Irrationals Exact Comparison of Quadratic Irrationals Phuc Ngo To cite this version: Phuc Ngo. Exact Comparison of Quadratic Irrationals. [Research Report] LIGM. 20. HAL Id: hal-0069762 https://hal.archives-ouvertes.fr/hal-0069762

More information

Easter bracelets for years

Easter bracelets for years Easter bracelets for 5700000 years Denis Roegel To cite this version: Denis Roegel. Easter bracelets for 5700000 years. [Research Report] 2014. HAL Id: hal-01009457 https://hal.inria.fr/hal-01009457

More information

On the longest path in a recursively partitionable graph

On the longest path in a recursively partitionable graph On the longest path in a recursively partitionable graph Julien Bensmail To cite this version: Julien Bensmail. On the longest path in a recursively partitionable graph. 2012. HAL Id:

More information

On size, radius and minimum degree

On size, radius and minimum degree On size, radius and minimum degree Simon Mukwembi To cite this version: Simon Mukwembi. On size, radius and minimum degree. Discrete Mathematics and Theoretical Computer Science, DMTCS, 2014, Vol. 16 no.

More information

Passerelle entre les arts : la sculpture sonore

Passerelle entre les arts : la sculpture sonore Passerelle entre les arts : la sculpture sonore Anaïs Rolez To cite this version: Anaïs Rolez. Passerelle entre les arts : la sculpture sonore. Article destiné à l origine à la Revue de l Institut National

More information

Can we reduce health inequalities? An analysis of the English strategy ( )

Can we reduce health inequalities? An analysis of the English strategy ( ) Can we reduce health inequalities? An analysis of the English strategy (1997-2010) Johan P Mackenbach To cite this version: Johan P Mackenbach. Can we reduce health inequalities? An analysis of the English

More information

Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas

Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas Susumu Kato, Eisuke Miura, Mitsumori Tanimoto, Masahiro Adachi, Kazuyoshi Koyama To cite this

More information

Comment on: Sadi Carnot on Carnot s theorem.

Comment on: Sadi Carnot on Carnot s theorem. Comment on: Sadi Carnot on Carnot s theorem. Jacques Arnaud, Laurent Chusseau, Fabrice Philippe To cite this version: Jacques Arnaud, Laurent Chusseau, Fabrice Philippe. Comment on: Sadi Carnot on Carnot

More information

Completeness of the Tree System for Propositional Classical Logic

Completeness of the Tree System for Propositional Classical Logic Completeness of the Tree System for Propositional Classical Logic Shahid Rahman To cite this version: Shahid Rahman. Completeness of the Tree System for Propositional Classical Logic. Licence. France.

More information

L institution sportive : rêve et illusion

L institution sportive : rêve et illusion L institution sportive : rêve et illusion Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar To cite this version: Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar. L institution sportive : rêve et illusion. Revue

More information

b-chromatic number of cacti

b-chromatic number of cacti b-chromatic number of cacti Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva To cite this version: Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva. b-chromatic number

More information

Analysis of Boyer and Moore s MJRTY algorithm

Analysis of Boyer and Moore s MJRTY algorithm Analysis of Boyer and Moore s MJRTY algorithm Laurent Alonso, Edward M. Reingold To cite this version: Laurent Alonso, Edward M. Reingold. Analysis of Boyer and Moore s MJRTY algorithm. Information Processing

More information

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach Christophe Cruz, Helmi Ben Hmida, Frank Boochs, Christophe Nicolle To cite this version: Christophe Cruz, Helmi Ben Hmida,

More information

On sl3 KZ equations and W3 null-vector equations

On sl3 KZ equations and W3 null-vector equations On sl3 KZ equations and W3 null-vector equations Sylvain Ribault To cite this version: Sylvain Ribault. On sl3 KZ equations and W3 null-vector equations. Conformal Field Theory, Integrable Models, and

More information

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart To cite this version: Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart.

More information

On Symmetric Norm Inequalities And Hermitian Block-Matrices

On Symmetric Norm Inequalities And Hermitian Block-Matrices On Symmetric Norm Inequalities And Hermitian lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna On Symmetric Norm Inequalities And Hermitian lock-matrices 015 HAL Id: hal-0131860

More information

SOLAR RADIATION ESTIMATION AND PREDICTION USING MEASURED AND PREDICTED AEROSOL OPTICAL DEPTH

SOLAR RADIATION ESTIMATION AND PREDICTION USING MEASURED AND PREDICTED AEROSOL OPTICAL DEPTH SOLAR RADIATION ESTIMATION AND PREDICTION USING MEASURED AND PREDICTED AEROSOL OPTICAL DEPTH Carlos M. Fernández-Peruchena, Martín Gastón, Maria V Guisado, Ana Bernardos, Íñigo Pagola, Lourdes Ramírez

More information

Sound intensity as a function of sound insulation partition

Sound intensity as a function of sound insulation partition Sound intensity as a function of sound insulation partition S. Cvetkovic, R. Prascevic To cite this version: S. Cvetkovic, R. Prascevic. Sound intensity as a function of sound insulation partition. Journal

More information

Exogenous input estimation in Electronic Power Steering (EPS) systems

Exogenous input estimation in Electronic Power Steering (EPS) systems Exogenous input estimation in Electronic Power Steering (EPS) systems Valentina Ciarla, Carlos Canudas de Wit, Franck Quaine, Violaine Cahouet To cite this version: Valentina Ciarla, Carlos Canudas de

More information

Question order experimental constraints on quantum-like models of judgement

Question order experimental constraints on quantum-like models of judgement Question order experimental constraints on quantum-like models of judgement Patrick Cassam-Chenaï To cite this version: Patrick Cassam-Chenaï. Question order experimental constraints on quantum-like models

More information

Vibro-acoustic simulation of a car window

Vibro-acoustic simulation of a car window Vibro-acoustic simulation of a car window Christophe Barras To cite this version: Christophe Barras. Vibro-acoustic simulation of a car window. Société Française d Acoustique. Acoustics 12, Apr 12, Nantes,

More information

Entropies and fractal dimensions

Entropies and fractal dimensions Entropies and fractal dimensions Amelia Carolina Sparavigna To cite this version: Amelia Carolina Sparavigna. Entropies and fractal dimensions. Philica, Philica, 2016. HAL Id: hal-01377975

More information

A remark on a theorem of A. E. Ingham.

A remark on a theorem of A. E. Ingham. A remark on a theorem of A. E. Ingham. K G Bhat, K Ramachandra To cite this version: K G Bhat, K Ramachandra. A remark on a theorem of A. E. Ingham.. Hardy-Ramanujan Journal, Hardy-Ramanujan Society, 2006,

More information

A new approach of the concept of prime number

A new approach of the concept of prime number A new approach of the concept of prime number Jamel Ghannouchi To cite this version: Jamel Ghannouchi. A new approach of the concept of prime number. 4 pages. 24. HAL Id: hal-3943 https://hal.archives-ouvertes.fr/hal-3943

More information

A Simple Proof of P versus NP

A Simple Proof of P versus NP A Simple Proof of P versus NP Frank Vega To cite this version: Frank Vega. A Simple Proof of P versus NP. 2016. HAL Id: hal-01281254 https://hal.archives-ouvertes.fr/hal-01281254 Submitted

More information

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Shahid Rahman To cite this version: Shahid Rahman. Soundness of the System of Semantic Trees for Classical Logic

More information

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Marie Duhamel To cite this version: Marie Duhamel. Evolution of the cooperation and consequences

More information

Lorentz force velocimetry using small-size permanent magnet systems and a multi-degree-of-freedom force/torque sensor

Lorentz force velocimetry using small-size permanent magnet systems and a multi-degree-of-freedom force/torque sensor Lorentz force velocimetry using small-size permanent magnet systems and a multi-degree-of-freedom force/torque sensor D Hernández, C Karcher To cite this version: D Hernández, C Karcher. Lorentz force

More information

Multiple sensor fault detection in heat exchanger system

Multiple sensor fault detection in heat exchanger system Multiple sensor fault detection in heat exchanger system Abdel Aïtouche, Didier Maquin, Frédéric Busson To cite this version: Abdel Aïtouche, Didier Maquin, Frédéric Busson. Multiple sensor fault detection

More information

Full-order observers for linear systems with unknown inputs

Full-order observers for linear systems with unknown inputs Full-order observers for linear systems with unknown inputs Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu To cite this version: Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu. Full-order observers

More information

On Politics and Argumentation

On Politics and Argumentation On Politics and Argumentation Maria Boritchev To cite this version: Maria Boritchev. On Politics and Argumentation. MALOTEC, Mar 2017, Nancy, France. 2017. HAL Id: hal-01666416 https://hal.archives-ouvertes.fr/hal-01666416

More information

Thermodynamic form of the equation of motion for perfect fluids of grade n

Thermodynamic form of the equation of motion for perfect fluids of grade n Thermodynamic form of the equation of motion for perfect fluids of grade n Henri Gouin To cite this version: Henri Gouin. Thermodynamic form of the equation of motion for perfect fluids of grade n. Comptes

More information

Determination of absorption characteristic of materials on basis of sound intensity measurement

Determination of absorption characteristic of materials on basis of sound intensity measurement Determination of absorption characteristic of materials on basis of sound intensity measurement R. Prascevic, A. Milosevic, S. Cvetkovic To cite this version: R. Prascevic, A. Milosevic, S. Cvetkovic.

More information

New Basis Points of Geodetic Stations for Landslide Monitoring

New Basis Points of Geodetic Stations for Landslide Monitoring New Basis Points of Geodetic Stations for Landslide Monitoring V Riabchii, M Tregub, Yankin To cite this version: V Riabchii, M Tregub, Yankin. New Basis Points of Geodetic Stations for Landslide Monitoring.

More information

On path partitions of the divisor graph

On path partitions of the divisor graph On path partitions of the divisor graph Paul Melotti, Eric Saias To cite this version: Paul Melotti, Eric Saias On path partitions of the divisor graph 018 HAL Id: hal-0184801 https://halarchives-ouvertesfr/hal-0184801

More information

A note on the computation of the fraction of smallest denominator in between two irreducible fractions

A note on the computation of the fraction of smallest denominator in between two irreducible fractions A note on the computation of the fraction of smallest denominator in between two irreducible fractions Isabelle Sivignon To cite this version: Isabelle Sivignon. A note on the computation of the fraction

More information

Thomas Lugand. To cite this version: HAL Id: tel

Thomas Lugand. To cite this version: HAL Id: tel Contribution à la Modélisation et à l Optimisation de la Machine Asynchrone Double Alimentation pour des Applications Hydrauliques de Pompage Turbinage Thomas Lugand To cite this version: Thomas Lugand.

More information

Numerical Modeling of Eddy Current Nondestructive Evaluation of Ferromagnetic Tubes via an Integral. Equation Approach

Numerical Modeling of Eddy Current Nondestructive Evaluation of Ferromagnetic Tubes via an Integral. Equation Approach Numerical Modeling of Eddy Current Nondestructive Evaluation of Ferromagnetic Tubes via an Integral Equation Approach Anastassios Skarlatos, Grégoire Pichenot, Dominique Lesselier, Marc Lambert, Bernard

More information

The Zenith Passage of the Sun in the Plan of Brasilia

The Zenith Passage of the Sun in the Plan of Brasilia The Zenith Passage of the Sun in the Plan of Brasilia Amelia Carolina Sparavigna To cite this version: Amelia Carolina Sparavigna. The Zenith Passage of the Sun in the Plan of Brasilia. Philica, Philica,

More information

Water Vapour Effects in Mass Measurement

Water Vapour Effects in Mass Measurement Water Vapour Effects in Mass Measurement N.-E. Khélifa To cite this version: N.-E. Khélifa. Water Vapour Effects in Mass Measurement. Measurement. Water Vapour Effects in Mass Measurement, May 2007, Smolenice,

More information

A Study of the Regular Pentagon with a Classic Geometric Approach

A Study of the Regular Pentagon with a Classic Geometric Approach A Study of the Regular Pentagon with a Classic Geometric Approach Amelia Carolina Sparavigna, Mauro Maria Baldi To cite this version: Amelia Carolina Sparavigna, Mauro Maria Baldi. A Study of the Regular

More information

Improving the Jet Reconstruction with the Particle Flow Method; an Introduction

Improving the Jet Reconstruction with the Particle Flow Method; an Introduction Improving the Jet Reconstruction with the Particle Flow Method; an Introduction Jean-Claude Brient To cite this version: Jean-Claude Brient. Improving the Jet Reconstruction with the Particle Flow Method;

More information

Nodal and divergence-conforming boundary-element methods applied to electromagnetic scattering problems

Nodal and divergence-conforming boundary-element methods applied to electromagnetic scattering problems Nodal and divergence-conforming boundary-element methods applied to electromagnetic scattering problems M. Afonso, Joao Vasconcelos, Renato Mesquita, Christian Vollaire, Laurent Nicolas To cite this version:

More information

Solving the neutron slowing down equation

Solving the neutron slowing down equation Solving the neutron slowing down equation Bertrand Mercier, Jinghan Peng To cite this version: Bertrand Mercier, Jinghan Peng. Solving the neutron slowing down equation. 2014. HAL Id: hal-01081772

More information

A Slice Based 3-D Schur-Cohn Stability Criterion

A Slice Based 3-D Schur-Cohn Stability Criterion A Slice Based 3-D Schur-Cohn Stability Criterion Ioana Serban, Mohamed Najim To cite this version: Ioana Serban, Mohamed Najim. A Slice Based 3-D Schur-Cohn Stability Criterion. ICASSP 007, Apr 007, Honolulu,

More information

A Simple Model for Cavitation with Non-condensable Gases

A Simple Model for Cavitation with Non-condensable Gases A Simple Model for Cavitation with Non-condensable Gases Mathieu Bachmann, Siegfried Müller, Philippe Helluy, Hélène Mathis To cite this version: Mathieu Bachmann, Siegfried Müller, Philippe Helluy, Hélène

More information

AC Transport Losses Calculation in a Bi-2223 Current Lead Using Thermal Coupling With an Analytical Formula

AC Transport Losses Calculation in a Bi-2223 Current Lead Using Thermal Coupling With an Analytical Formula AC Transport Losses Calculation in a Bi-2223 Current Lead Using Thermal Coupling With an Analytical Formula Kévin Berger, Jean Lévêque, Denis Netter, Bruno Douine, Abderrezak Rezzoug To cite this version:

More information

Characterization of the local Electrical Properties of Electrical Machine Parts with non-trivial Geometry

Characterization of the local Electrical Properties of Electrical Machine Parts with non-trivial Geometry Characterization of the local Electrical Properties of Electrical Machine Parts with non-trivial Geometry Laure Arbenz, Abdelkader Benabou, Stéphane Clenet, Jean Claude Mipo, Pierre Faverolle To cite this

More information

Hook lengths and shifted parts of partitions

Hook lengths and shifted parts of partitions Hook lengths and shifted parts of partitions Guo-Niu Han To cite this version: Guo-Niu Han Hook lengths and shifted parts of partitions The Ramanujan Journal, 009, 9 p HAL Id: hal-00395690

More information

Theoretical calculation of the power of wind turbine or tidal turbine

Theoretical calculation of the power of wind turbine or tidal turbine Theoretical calculation of the power of wind turbine or tidal turbine Pierre Lecanu, Joel Breard, Dominique Mouazé To cite this version: Pierre Lecanu, Joel Breard, Dominique Mouazé. Theoretical calculation

More information

A numerical analysis of chaos in the double pendulum

A numerical analysis of chaos in the double pendulum A numerical analysis of chaos in the double pendulum Tomasz Stachowiak, Toshio Okada To cite this version: Tomasz Stachowiak, Toshio Okada. A numerical analysis of chaos in the double pendulum. Chaos,

More information

On infinite permutations

On infinite permutations On infinite permutations Dmitri G. Fon-Der-Flaass, Anna E. Frid To cite this version: Dmitri G. Fon-Der-Flaass, Anna E. Frid. On infinite permutations. Stefan Felsner. 2005 European Conference on Combinatorics,

More information

Cutwidth and degeneracy of graphs

Cutwidth and degeneracy of graphs Cutwidth and degeneracy of graphs Benoit Kloeckner To cite this version: Benoit Kloeckner. Cutwidth and degeneracy of graphs. IF_PREPUB. 2009. HAL Id: hal-00408210 https://hal.archives-ouvertes.fr/hal-00408210v1

More information

A Context free language associated with interval maps

A Context free language associated with interval maps A Context free language associated with interval maps M Archana, V Kannan To cite this version: M Archana, V Kannan. A Context free language associated with interval maps. Discrete Mathematics and Theoretical

More information

BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES

BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES Antonin Pottier, Rabia Nessah To cite this version: Antonin Pottier, Rabia Nessah. BERGE VAISMAN AND NASH EQUILIBRIA: TRANS- FORMATION OF GAMES.

More information

Ideal Coulomb plasma approximation in line shape models: problematic issues

Ideal Coulomb plasma approximation in line shape models: problematic issues Ideal Coulomb plasma approximation in line shape models: problematic issues Joël Rosato, Hubert Capes, Roland Stamm To cite this version: Joël Rosato, Hubert Capes, Roland Stamm. Ideal Coulomb plasma approximation

More information

On the Earth s magnetic field and the Hall effect

On the Earth s magnetic field and the Hall effect On the Earth s magnetic field and the Hall effect J. E. Allen To cite this version: J. E. Allen. On the Earth s magnetic field and the Hall effect. Nonlinear rocesses in Geophysics, European Geosciences

More information

The influence of the global atmospheric properties on the detection of UHECR by EUSO on board of the ISS

The influence of the global atmospheric properties on the detection of UHECR by EUSO on board of the ISS The influence of the global atmospheric properties on the detection of UHECR by EUSO on board of the ISS C. Berat, D. Lebrun, A. Stutz, E. Plagnol To cite this version: C. Berat, D. Lebrun, A. Stutz, E.

More information

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 Sibiri Christian Bandre To cite this version: Sibiri Christian Bandre. There are infinitely many twin primes

More information

Stickelberger s congruences for absolute norms of relative discriminants

Stickelberger s congruences for absolute norms of relative discriminants Stickelberger s congruences for absolute norms of relative discriminants Georges Gras To cite this version: Georges Gras. Stickelberger s congruences for absolute norms of relative discriminants. Journal

More information

Linear Quadratic Zero-Sum Two-Person Differential Games

Linear Quadratic Zero-Sum Two-Person Differential Games Linear Quadratic Zero-Sum Two-Person Differential Games Pierre Bernhard To cite this version: Pierre Bernhard. Linear Quadratic Zero-Sum Two-Person Differential Games. Encyclopaedia of Systems and Control,

More information

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications Alexandre Sedoglavic To cite this version: Alexandre Sedoglavic. A non-commutative algorithm for multiplying (7 7) matrices

More information

Eddy-Current Effects in Circuit Breakers During Arc Displacement Phase

Eddy-Current Effects in Circuit Breakers During Arc Displacement Phase Eddy-Current Effects in Circuit Breakers During Arc Displacement Phase Olivier Chadebec, Gerard Meunier, V. Mazauric, Yann Le Floch, Patrice Labie To cite this version: Olivier Chadebec, Gerard Meunier,

More information

Teaching Reitlinger Cycles To Improve Students Knowledge And Comprehension Of Thermodynamics

Teaching Reitlinger Cycles To Improve Students Knowledge And Comprehension Of Thermodynamics Teaching Reitlinger Cycles To Improve Students Knowledge nd Comprehension Of Thermodynamics melia Carolina Sparavigna To cite this version: melia Carolina Sparavigna. Teaching Reitlinger Cycles To Improve

More information

Simulation and measurement of loudspeaker nonlinearity with a broad-band noise excitation

Simulation and measurement of loudspeaker nonlinearity with a broad-band noise excitation Simulation and measurement of loudspeaker nonlinearity with a broad-band noise excitation Andrzej Dobrucki, Rafal Siczek To cite this version: Andrzej Dobrucki, Rafal Siczek. Simulation and measurement

More information

The Windy Postman Problem on Series-Parallel Graphs

The Windy Postman Problem on Series-Parallel Graphs The Windy Postman Problem on Series-Parallel Graphs Francisco Javier Zaragoza Martínez To cite this version: Francisco Javier Zaragoza Martínez. The Windy Postman Problem on Series-Parallel Graphs. Stefan

More information

Towards an active anechoic room

Towards an active anechoic room Towards an active anechoic room Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède To cite this version: Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède. Towards an active

More information

The status of VIRGO. To cite this version: HAL Id: in2p

The status of VIRGO. To cite this version: HAL Id: in2p The status of VIRGO E. Tournefier, F. Acernese, P. Amico, M. Al-Shourbagy, S. Aoudia, S. Avino, D. Babusci, G. Ballardin, R. Barillé, F. Barone, et al. To cite this version: E. Tournefier, F. Acernese,

More information

Some diophantine problems concerning equal sums of integers and their cubes

Some diophantine problems concerning equal sums of integers and their cubes Some diophantine problems concerning equal sums of integers and their cubes Ajai Choudhry To cite this version: Ajai Choudhry. Some diophantine problems concerning equal sums of integers and their cubes.

More information

Widely Linear Estimation with Complex Data

Widely Linear Estimation with Complex Data Widely Linear Estimation with Complex Data Bernard Picinbono, Pascal Chevalier To cite this version: Bernard Picinbono, Pascal Chevalier. Widely Linear Estimation with Complex Data. IEEE Transactions on

More information

Ultra low frequency pressure transducer calibration

Ultra low frequency pressure transducer calibration Ultra low frequency pressure transducer calibration A. Semenov To cite this version: A. Semenov. Ultra low frequency pressure transducer calibration. Journal de Physique IV Colloque, 1994, 04 (C5), pp.c7-251-c7-254.

More information

Modeling of Electromagmetic Processes in Wire Electric Discharge Machining

Modeling of Electromagmetic Processes in Wire Electric Discharge Machining Modeling of Electromagmetic Processes in Wire Electric Discharge Machining V.M. Volgin, V.V. Lyubimov, V.D. Kukhar To cite this version: V.M. Volgin, V.V. Lyubimov, V.D. Kukhar. Modeling of Electromagmetic

More information

Antipodal radiation pattern of a patch antenna combined with superstrate using transformation electromagnetics

Antipodal radiation pattern of a patch antenna combined with superstrate using transformation electromagnetics Antipodal radiation pattern of a patch antenna combined with superstrate using transformation electromagnetics Mark Clemente Arenas, Anne-Claire Lepage, Xavier Begaud To cite this version: Mark Clemente

More information

Nonlocal computational methods applied to composites structures

Nonlocal computational methods applied to composites structures Nonlocal computational methods applied to composites structures Norbert Germain, Frédéric Feyel, Jacques Besson To cite this version: Norbert Germain, Frédéric Feyel, Jacques Besson. Nonlocal computational

More information

Quantum efficiency and metastable lifetime measurements in ruby ( Cr 3+ : Al2O3) via lock-in rate-window photothermal radiometry

Quantum efficiency and metastable lifetime measurements in ruby ( Cr 3+ : Al2O3) via lock-in rate-window photothermal radiometry Quantum efficiency and metastable lifetime measurements in ruby ( Cr 3+ : Al2O3) via lock-in rate-window photothermal radiometry A. Mandelis, Z. Chen, R. Bleiss To cite this version: A. Mandelis, Z. Chen,

More information

Some tight polynomial-exponential lower bounds for an exponential function

Some tight polynomial-exponential lower bounds for an exponential function Some tight polynomial-exponential lower bounds for an exponential function Christophe Chesneau To cite this version: Christophe Chesneau. Some tight polynomial-exponential lower bounds for an exponential

More information

The Riemann Hypothesis Proof And The Quadrivium Theory

The Riemann Hypothesis Proof And The Quadrivium Theory The Riemann Hypothesis Proof And The Quadrivium Theory Thierno M. Sow To cite this version: Thierno M. Sow. The Riemann Hypothesis Proof And The Quadrivium Theory. 2017. HAL Id: hal-01513658 https://hal.archives-ouvertes.fr/hal-01513658

More information

Nel s category theory based differential and integral Calculus, or Did Newton know category theory?

Nel s category theory based differential and integral Calculus, or Did Newton know category theory? Nel s category theory based differential and integral Calculus, or Did Newton know category theory? Elemer Elad Rosinger To cite this version: Elemer Elad Rosinger. Nel s category theory based differential

More information

Computer Visualization of the Riemann Zeta Function

Computer Visualization of the Riemann Zeta Function Computer Visualization of the Riemann Zeta Function Kamal Goudjil To cite this version: Kamal Goudjil. Computer Visualization of the Riemann Zeta Function. 2017. HAL Id: hal-01441140 https://hal.archives-ouvertes.fr/hal-01441140

More information

On the Griesmer bound for nonlinear codes

On the Griesmer bound for nonlinear codes On the Griesmer bound for nonlinear codes Emanuele Bellini, Alessio Meneghetti To cite this version: Emanuele Bellini, Alessio Meneghetti. On the Griesmer bound for nonlinear codes. Pascale Charpin, Nicolas

More information

DEM modeling of penetration test in static and dynamic conditions

DEM modeling of penetration test in static and dynamic conditions DEM modeling of penetration test in static and dynamic conditions Quoc Anh Tran, Bastien Chevalier, Pierre Breul To cite this version: Quoc Anh Tran, Bastien Chevalier, Pierre Breul. DEM modeling of penetration

More information

A non-linear simulator written in C for orbital spacecraft rendezvous applications.

A non-linear simulator written in C for orbital spacecraft rendezvous applications. A non-linear simulator written in C for orbital spacecraft rendezvous applications. Paulo Ricardo Arantes Gilz To cite this version: Paulo Ricardo Arantes Gilz. A non-linear simulator written in C for

More information

Optical component modelling and circuit simulation using SERENADE suite

Optical component modelling and circuit simulation using SERENADE suite Optical component modelling and circuit simulation using SERENADE suite Laurent Guilloton, Smail Tedjini, Tan-Phu Vuong To cite this version: Laurent Guilloton, Smail Tedjini, Tan-Phu Vuong. Optical component

More information

Some approaches to modeling of the effective properties for thermoelastic composites

Some approaches to modeling of the effective properties for thermoelastic composites Some approaches to modeling of the ective properties for thermoelastic composites Anna Nasedkina Andrey Nasedkin Vladimir Remizov To cite this version: Anna Nasedkina Andrey Nasedkin Vladimir Remizov.

More information

Control of an offshore wind turbine modeled as discrete system

Control of an offshore wind turbine modeled as discrete system Control of an offshore wind turbine modeled as discrete system Pedro Guimarães, Suzana Ávila To cite this version: Pedro Guimarães, Suzana Ávila. Control of an offshore wind turbine modeled as discrete

More information

Diurnal variation of tropospheric temperature at a tropical station

Diurnal variation of tropospheric temperature at a tropical station Diurnal variation of tropospheric temperature at a tropical station K. Revathy, S. R. Prabhakaran Nayar, B. V. Krishna Murthy To cite this version: K. Revathy, S. R. Prabhakaran Nayar, B. V. Krishna Murthy.

More information

GENERALIZED OPTICAL BISTABILITY AND CHAOS IN A LASER WITH A SATURABLE ABSORBER

GENERALIZED OPTICAL BISTABILITY AND CHAOS IN A LASER WITH A SATURABLE ABSORBER GENERALIZED OPTICAL BISTABILITY AND CHAOS IN A LASER WITH A SATURABLE ABSORBER E. Arimondo, F. De Tomasi, B. Zambon, F. Papoff, D. Hennequin To cite this version: E. Arimondo, F. De Tomasi, B. Zambon,

More information

The Learner s Dictionary and the Sciences:

The Learner s Dictionary and the Sciences: The Learner s Dictionary and the Sciences: Geoffrey Williams To cite this version: Geoffrey Williams. The Learner s Dictionary and the Sciences:: Mismatch or no match?. Corpora, Language, Teaching, and

More information

RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING

RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING Jean-François Semblat To cite this version: Jean-François Semblat. RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING. Journal of Sound and Vibration, Elsevier,

More information