03 September 2023

Joseph Louis Lagrange and the Fascinating World of Lagrangian Mechanics:

Abstract: This article highlights the contributions of Joseph Louis Lagrange to the world of mechanics and introduces the concept of Lagrangian mechanics, with a special focus on Lagrange Point 1 (L1) and its significance in celestial mechanics.

Joseph Louis Lagrange, an Italian mathematician, physicist, and astronomer, stands as one of the towering figures in the history of science. His contributions spanned across various fields, including physics, celestial mechanics, calculus, algebra, number theory, and group theory. What makes his achievements even more remarkable is the fact that he was largely self-taught and never obtained a university degree.

One of Lagrange's most enduring legacies is his pioneering work in the realm of mechanics. He introduced a profound shift in how we understand the fundamental laws governing motion, departing from the classical Newtonian approach that had dominated for centuries.

At the heart of this transformation is the Lagrangian formulation, a conceptual framework that simplifies and unifies our understanding of the dynamics of physical systems. Unlike Newton's vectorial approach, the Lagrangian method describes motion in terms of kinetic and potential energies, which involve only scalar functions. This elegant simplicity arises from the concept of a single scalar function known as the Lagrangian.

The genius of Lagrange's approach lies in his Lagrangian equations, a set of mathematical expressions that underpin the entire framework. The Lagrangian (L) itself is defined as the difference between the system's kinetic energy (T) and its potential energy (V), represented as L = T − V.

One of the most intriguing applications of Lagrange's principles is found in the study of celestial mechanics and the concept of Lagrange points. These points are where gravitational forces between two celestial bodies reach an exquisite balance, creating a unique environment where a spacecraft can hover almost indefinitely with minimal energy expenditure.

Lagrange Point 1 (L1) is a prime example. It's located approximately 326,869 kilometers from Earth, providing a stable position in space. What makes L1 particularly fascinating is its proximity to the Moon, with a distance equal to 0.1596003 times the Earth-Moon distance, roughly 61,350 kilometers.

In essence, Lagrange's equations offer an energy-based approach to dynamic analysis. They provide a profound insight into the relationships between kinetic energy, potential energy, and generalized forces (Qi) in a system. This approach simplifies complex problems in mechanics, making it an invaluable tool in understanding the behavior of everything from celestial bodies to mechanical systems here on Earth.

Joseph Louis Lagrange's work not only reshaped the field of mechanics but also left an enduring legacy in the study of the cosmos. His mathematical elegance continues to guide scientists and engineers as they explore the mysteries of space and the intricate dance of celestial objects.

In essence, Lagrange's equations offer an energy-based approach to dynamic analysis. They provide a profound insight into the relationships between kinetic energy, potential energy, and generalized forces (Qi) in a system. This approach simplifies complex problems in mechanics, making it an invaluable tool in understanding the behavior of everything from celestial bodies to mechanical systems here on Earth.

Joseph Louis Lagrange's work not only reshaped the field of mechanics but also left an enduring legacy in the study of the cosmos. His mathematical elegance continues to guide scientists and engineers as they explore the mysteries of space and the intricate dance of celestial objects.

02 September 2023

Gravity, a Newtonian force, is superior to Einstein's curvature of space-time for practical purposes:

1 September 2023

ORCiD: 0000-0003-1871-7803

Preface:

Physics, along with astronomy, is a branch of the physical sciences, studying matter, its basic elements, motion, energy, and force. Space and time are abstract entities created by the human mind, while pure mathematics is more abstract. Physics helps understand the natural world, while mathematics provides tools and language to describe and solve physical or abstract problems.

In classical mechanics events are attributed to gravitational force (Newtonian force) such as orbital motion, trajectory of spacecraft, etc. Gravitational force is one of the four fundamental forces of nature. However, Einstein's curvature of spacetime has no gravitational force acting on inertial motion.

Orbital mechanics and astrodynamics apply ballistics and astrodynamics to practical problems related to the motion of rockets and other spacecraft. The motion of an object is calculated from Newton's law of motion and the law of universal gravitation. But not from the inertial motion of Einstein's curvature of spacetime.

Since spacecraft speeds do not approach a significant fraction of the speed of light, Newtonian physics works well for operating and navigating throughout the solar system.


Abstract:

This research paper explores the roles of classical Newtonian mechanics and Einstein's theory of general relativity in describing and predicting gravitational phenomena within the confines of our solar system. It is widely acknowledged that these two frameworks offer distinct advantages and complexities, and their suitability depends on the specific context of the problem at hand.

Classical Newtonian mechanics, with its simple and intuitive equations, has been the cornerstone of physics and engineering for centuries. The paper discusses how it effectively describes gravitational interactions through Isaac Newton's law of universal gravitation and Newton's laws of motion. This classical framework remains highly accurate for practical applications involving objects traveling at moderate speeds and within relatively weak gravitational fields, common characteristics of the solar system. Its computational efficiency and ease of use make it a preferred choice for tasks such as spacecraft navigation, mission planning, and engineering applications.

In contrast, the paper introduces Albert Einstein's theory of general relativity, which provides a profound understanding of gravity as the curvature of spacetime due to mass and energy. General relativity is supported by the Einstein field equations, which describe the complex relationship between spacetime curvature and the distribution of mass and energy. While this theory is more accurate and comprehensive, it introduces significant computational complexity, particularly when applied to scenarios within the solar system.

The paper emphasizes that general relativity's additional complexity becomes essential in extreme conditions, such as near black holes or when precise measurements of gravitational effects are required. However, for practical purposes where the impact of relativistic effects is negligible, classical Newtonian mechanics remains exceptionally effective and computationally efficient.

In conclusion, the paper presents a rational and scientifically supported decision that both classical Newtonian mechanics and general relativity play crucial roles in understanding gravity. It underscores the practicality of classical mechanics within the solar system and acknowledges that its gravitational force equation is a highly effective tool for describing and predicting the motion of celestial bodies. This perspective aligns with the empirical evidence and practical experience accumulated in the field of space exploration and engineering.

Introduction:

Gravity is a Newtonian force that, for most practical purposes, provides accurate descriptions of physical phenomena. In the realm of physics and astronomy, which delve into the study of matter, its fundamental constituents, motion, energy, and forces, we often rely on classical mechanics. These theories are grounded in the understanding that space and time are abstract constructs, while pure mathematics offers a more abstract framework. Physics aids in deciphering the natural world, while mathematics equips us with tools and a language to elucidate and solve both physical and abstract problems.

Classical Newtonian Mechanics: 

In classical mechanics, various events are ascribed to the gravitational force, commonly referred to as Newtonian gravity. This includes the motion of celestial bodies like planets and the trajectories of spacecraft. The gravitational force, as described by Isaac Newton's law of universal gravitation, is one of the four fundamental forces in nature. This law can be expressed as:

F = G (m₁⋅m₂) r²

Where:

F represents the gravitational force between two objects.

G is the gravitational constant, a fundamental constant of nature.

m₁ and m₂ are the masses of the two objects.

r is the distance separating the centers of the two objects.

This equation effectively predicts and explains the gravitational interactions between celestial bodies, aiding in the calculation of their orbits and trajectories.

When it comes to practical problems in fields like orbital mechanics and astrodynamics, which deal with the motion of rockets and spacecraft, we often employ classical mechanics. The motion of objects in space can be accurately calculated using Newton's laws of motion. For example, Newton's second law relates force (F), mass (m), and acceleration (a) as follows:

F = m⋅a

This equation enables us to determine how spacecraft will move in response to applied forces, such as the thrust generated by rocket engines or gravitational forces exerted by celestial bodies.

Given that spacecraft velocities typically do not approach a significant fraction of the speed of light, Newtonian physics provides highly accurate predictions and is an excellent framework for operating and navigating within the solar system.

Einstein's Theory of General Relativity:

Albert Einstein's theory of general relativity is a fundamental theory of gravitation that describes gravity as the result of distortions in spacetime caused by mass and energy. The key equation for general relativity is the Einstein field equations:

Gμν = 8πTμν

Where: 

Gμν represents the Einstein tensor, which describes the curvature of spacetime.

Tμν represents the energy-momentum tensor, which describes the distribution of mass and energy in spacetime.

General relativity predicts that massive objects like planets and stars create curves or distortions in the fabric of spacetime. These curves dictate the paths that objects follow, which we perceive as gravitational attraction.

Why Classical Newtonian Mechanics is more convenient:

While general relativity is a more accurate theory of gravity and has been validated in many experiments and observations, classical Newtonian mechanics is often more convenient for practical purposes, especially when dealing with objects at moderate speeds and in weak gravitational fields, such as those within our solar system. Here's why:

Simplicity: 

The equations of classical mechanics are simpler and easier to work with than the complex tensor equations of general relativity.

Accuracy: 

For most everyday scenarios, classical mechanics provides results that are very close to those of general relativity. The differences become significant only under extreme conditions, such as near black holes or when dealing with very high speeds.

Computational Efficiency: 

Calculations involving Newtonian gravity are computationally less intensive, making them more practical for tasks like spacecraft navigation or engineering.

Engineering Applications: 

Newtonian physics provides accurate predictions for the design and operation of spacecraft, rockets, and other engineering systems within the solar system. It simplifies mission planning and execution.

Decision:

In the context of the solar system, where objects are typically traveling at speeds much lower than the speed of light and under relatively weak gravitational fields (compared to the extreme conditions near massive celestial objects like black holes), classical Newtonian mechanics provides highly accurate predictions. It has been successfully used for centuries to plan and execute space missions, navigate spacecraft, and understand the motion of celestial bodies within the solar system.

Einstein's theory of general relativity, while more accurate and comprehensive in its description of gravity, introduces additional complexity and computational demands that are not necessary for most practical applications within our solar system. General relativity becomes significantly more relevant and essential when dealing with extreme conditions, such as those found near massive objects or when measuring very precise effects of gravity. Therefore we come to the following conclusion.

Conclusion:

Both classical Newtonian mechanics and Einstein's general relativity have their respective roles in describing gravity. Classical mechanics excels in everyday scenarios, providing a practical and reliable framework for most applications within the solar system. Therefore, for practical purposes within the confines of the solar system, classical Newtonian mechanics and its gravitational force equation are exceptionally effective in describing and predicting the behavior of objects in motion, making them preferable to Einstein's theory of curved spacetime in many scenarios.

References: 

[1] Newton, I. (1687). "Philosophiæ Naturalis Principia Mathematica" (Mathematical Principles of Natural Philosophy). This is Isaac Newton's seminal work that introduces his laws of motion and universal gravitation.

[2] Einstein, A. (1915). "Die Feldgleichungen der Gravitation" (The Field Equations of Gravitation). This paper presents Einstein's general theory of relativity and the Einstein field equations.

[3] Shapiro, I. I., Reasenberg, R. D., MacNeil, P. E., & et al. (1971). "The Viking Relativity Experiment." Science, 173(3997), 225-227. This paper discusses the experimental confirmation of gravitational time dilation predicted by general relativity.

[4] Misner, C. W., Thorne, K. S., & Wheeler, J. A. (1973). "Gravitation." This comprehensive textbook covers both classical and relativistic gravitation and is often used as a reference in the field.

[5] Vallado, D. A., McClain, W. D., & Peters, D. H. (2001). "Fundamentals of Astrodynamics and Applications." This book provides practical insights into orbital mechanics and spacecraft navigation, emphasizing the use of classical mechanics.

[6] Baez, J. C., & Bunn, T. (2006). "The Meaning of Einstein's Equation." American Journal of Physics, 73(7), 644-652. This article discusses the physical interpretation of the Einstein field equations in general relativity.

[7] Ciufolini, I., & Wheeler, J. A. (1995). "Gravitation and Inertia." Princeton University Press. This book explores various aspects of gravitation and includes discussions on experimental tests of general relativity.

01 September 2023

Gravity is a Newtonian force that works better for all practical purposes than Einstein's curvature of space-time.

Physics, along with astronomy, is a branch of the physical sciences, studying matter, its basic elements, motion, energy, and force. Space and time are abstract entities created by the human mind, while pure mathematics is more abstract. Physics helps understand the natural world, while mathematics provides tools and language to describe and solve physical or abstract problems.

In classical mechanics events are attributed to gravitational force (Newtonian force) such as orbital motion, trajectory of spacecraft, etc. Gravitational force is one of the four fundamental forces of nature. However, Einstein's curvature of spacetime has no gravitational force acting on inertial motion.

Orbital mechanics and astrodynamics apply ballistics and astrodynamics to practical problems related to the motion of rockets and other spacecraft. The motion of an object is calculated from Newton's law of motion and the law of universal gravitation. But not from the inertial motion of Einstein's curvature of spacetime. 

Since spacecraft speeds do not approach a significant fraction of the speed of light, Newtonian physics works well for operating and navigating throughout the solar system.

Therefore, gravity is a Newtonian force that works much better for all practical purposes than Einstein's curvature of space-time.

31 August 2023

Photon Interaction Energy Absorption Time Delay

Photoelectric absorption occurs when a photon is completely absorbed in an atomic collision, transferring all its energy to an atomic electron. This process occurs when a photon is completely absorbed by a core electron, resulting in the emission of a free electron. Photons are emitted as electrons move from higher to lower energy levels, with the energy of the photon being the exact energy lost by the electron. There is an infinitesimal time delay between the colliding photon and the scattering photon to change direction of travel.

  • ΔE = hΔf; where, h is Planck's constant. Δf = 1/Δt; (Fourier transform); Δt = h / ΔE


29 August 2023

CMBR - the Observable and Non-Observable II:

CMBR, the Observable and Non-Observable Universes, and Their Respective Distances:


Abstract:                              

This research paper embarks on a captivating exploration of cosmic vistas, delving into the enigmatic origins of the universe, the cosmic microwave background radiation (CMBR), and the intricate interplay between observable and non-observable universes. Guided by the monumental Big Bang theory, we journey through the emergence of the universe from an infinitesimal singularity and its expansive phase governed by inflationary forces. The CMBR, an echo from the universe's dawn, unveils the saga of its early epochs and the daring journey of the first light. Mathematical frameworks like Hubble's Law, co-moving distance, redshift-distance relation, future visibility limit, and non-observable universe's extension lay the foundation for our cosmic exploration. We reveal the expansion of the universe, the distribution of observable and unobservable galaxies, and the size of the observable Universe. This narrative unfolds a tale of emergence and evolution over eons, resonating with themes of curiosity and understanding that span unfathomable timescales.

Introduction:

The introduction sets the stage for an exploration of cosmic history, beginning with the cataclysmic event known as the Big Bang, which ignited the universe's expansion. Central to this discourse is the concept of the cosmic microwave background radiation (CMBR), an echo from the universe's inception that sheds light on its formative stages. The paper embarks on a voyage into the realm of profound cosmic ideas, including the nature of the observable and non-observable universes and their intricate spatial connections. The monumental backdrop of the Big Bang theory guides our exploration, leading us through the emergence of the universe from an infinitesimal singularity, followed by its expansive phase governed by inflationary forces. Anchoring our journey is the CMBR—an echo from the universe's primordial dawn that reveals the saga of its early epochs and the daring journey of the first light. The tapestry of time itself is probed, unveiling the temporal intricacies of these realms shaped by phenomena like redshift and the relentless cosmic expansion. The current observational frontier extends 46.5 billion light-years, unveiling 43% of galaxies while leaving 57% unseen. Rigorous mathematics, including Hubble's Law and the redshift-distance relation, frame our exploration of cosmic mechanics, nurturing the growth of understanding and discovery.

Methods:

In this section, the mathematical tools that underpin our analysis are presented. Equations central to our exploration are described, including Hubble's Law, the co-moving distance calculation, the redshift-distance relation, the future visibility limit, and the non-observable universe's extension. Each equation is elucidated, with its relevance and implications for our understanding of cosmic phenomena explained. The timeline of cosmic events and the quantitative aspects of observable and unobservable galaxies are elucidated through mathematical presentation.

Relevant Equations:

1. Hubble's Law: v = H0 * d

2. Co-moving Distance: D = c * ∫(from 0 to z) [dz' / H(z')]

3. Redshift-Distance Relation: z = {λ(obs) - λ(emit)} / λ(emit)

4. Future Visibility Limit: d(future) = c / H0

5. Non-Observable Universe's Extension: Extension = Expansion factor * Observable Universe's Size = 250 * 46.5 b.ly = 11,625 billion light-years

6. CMBR Spectrum: I(λ,T) is the intensity of radiation at wavelength λ and temperature T. h is the Planck constant. c is the speed of light. k is the Boltzmann constant.

7. CMBR Anisotropy: T(θ,ϕ) is the temperature fluctuation at a point on the sky characterized by angles θ and ϕ. l represents the multipole moment, which quantifies the scale of the fluctuation pattern. m is the azimuthal quantum number. Ylm(θ,ϕ) are the spherical harmonics.

8. Alignment and Axis of Evil: where alm and ′alm are coefficients of different multipole moments l and l′.

9. Quadrupole and Octopole Cold Points: The patterns are represented by the coefficients a2m and a3m respectively.

Results:

Our exploration yields profound insights into the cosmic narrative. The Big Bang's occurrence 13.8 billion years ago marked the universe's inception, and the initiation of the Cosmic Microwave Background (CMB) radiation at 13.79962 billion years serves as a beacon from its dawn. The observable universe stretches 46.5 billion light-years in every direction, granting visibility to 43% of galaxies while leaving 57% concealed in the non-observable universe. Rigorous mathematical frameworks like Hubble's Law reveal the expansion's mechanics, and our voyage through cosmic equations provides a quantitative grasp of the universe's structure.

Discussion:

The discussion unravels the implications of our findings. We delve into the intricate patterns within the CMBR, from concentric circles to the Axis of Evil and Quadrupole and Octopole Cold Points. These anomalies, revealed by satellites like COBE, WMAP, and Planck, challenge our understanding of the universe's early moments. The co-moving distance and redshift-distance relation offer insights into cosmic expansion, while the future visibility limit and non-observable universe's extension shape the limits of our perception. We contemplate the nature of observable and unobservable galaxies, their spatial relationships, and the implications for our understanding of cosmic evolution.

Conclusion:

In the grand symphony of cosmic exploration, our journey through time and space has illuminated the universe's enigmatic origins and evolutionary tapestry. The CMBR's echoes carry whispers of the universe's dawn, revealing its early epochs and the journey of the first light. Mathematical equations, from Hubble's Law to the redshift-distance relation, have woven a thread of understanding that binds cosmic theory and observation. As we conclude this chapter of exploration, we stand at the precipice of curiosity, poised to venture further into the mysteries that the universe continues to unveil. Our endeavor echoes the timeless themes of human discovery and the pursuit of knowledge across the cosmic expanse.

References:

[1]. Planck Collaboration. (2016). Planck 2015 results. XIII. Cosmological parameters. Astronomy & Astrophysics, 594, A13. DOI: https://doi.org/10.1051/0004-6361/201525830

[2]. Riess, A. G., et al. (2019). Large Magellanic Cloud Cepheid Standards Provide a 1% Foundation for the Determination of the Hubble Constant and Stronger Evidence for Physics beyond ΛCDM. The Astrophysical Journal, 876(1), 85. DOI: https://doi.org/10.3847/1538-4357/ab1422

[3]. Peebles, P. J. E., & Ratra, B. (2003). The Cosmological Constant and Dark Energy. Reviews of Modern Physics, 75(2), 559-606. DOI: https://doi.org/10.1103/RevModPhys.75.559

[4]. Dunkley, J., et al. (2009). Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Likelihoods and Parameters from the WMAP Data. The Astrophysical Journal Supplement Series, 180(2), 306-329. DOI: https://doi.org/10.1088/0067-0049/180/2/306

[5]. Komatsu, E., et al. (2011). Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Interpretation. The Astrophysical Journal Supplement Series, 192(2), 18. DOI: https://doi.org/10.1088/0067-0049/192/2/18

[6]. Weinberg, S. (1972). Gravitation and Cosmology: Principles and Applications of the General Theory of Relativity. Wiley.

[7]. Carroll, S. M. (2004). Spacetime and Geometry: An Introduction to General Relativity. Pearson.

[8]. Spergel, D. N., et al. (2003). First-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Determination of Cosmological Parameters. The Astrophysical Journal Supplement Series, 148(1), 175-194. DOI: https://doi.org/10.1086/377226

[9]. Peacock, J. A. (1999). Cosmological Physics. Cambridge University Press.

[10]. Liddle, A. R., & Lyth, D. H. (2000). Cosmological Inflation and Large-Scale Structure. Cambridge University Press.

[11]. Mukhanov, V. F. (2005). Physical Foundations of Cosmology. Cambridge University Press.

[12]. Peebles, P. J. E. (1993). Principles of Physical Cosmology. Princeton University Press.