Gravitational and Dark Energy Influences on Light:

Soumendra Nath Thakur

ORCiD: 0000-0003-1871-7803

09-06-2024

Abstract:

The speed of light (c) is governed by the equation c=f⋅λ, where frequency (f) and wavelength (λ) are inversely proportional. This relationship ensures that in the absence of external forces, both frequency and wavelength remain constant. However, photons emitted by gravitationally bound bodies experience a gravitational force, described by Fg = G⋅(m₁⋅m₂)/d², influencing their wavelength and causing redshift. Despite this, the speed of light (c) remains unchanged due to the compensatory relationship between frequency and wavelength. As gravitational redshift reduces the frequency, the energy of the photon decreases according to E=hf. Beyond the gravitational influence, photons encounter the effects of dark energy, which exhibits antigravitational properties and becomes significant in cosmic expansion. This study highlights that while light travels at a constant speed in a vacuum, the increasing distance due to cosmic expansion can be perceived as (c+Δd)>c, though the intrinsic speed of light remains c. These findings underscore the importance of gravitational and dark energy influences on light while affirming the constancy of the speed of light in a vacuum.

Keywords: Gravitational redshift, Cosmic redshift, Dark energy, Cosmic expansion, Photon energy, Frequency-wavelength relationship, Antigravity, Zero-gravity radius,

The speed of light (c) is given by the equation c=f⋅λ, where frequency (f) is inversely proportional to wavelength (λ), i.e., f∝1/λ. This means that in the absence of any external forces acting on a wave or photon, both the frequency and wavelength would remain unchanged. However, the source emitting a photon is a gravitationally bound body. Therefore, a gravitational force acts on the wave or photon from the moment of its emission until it exits the gravitational influence of its source. This force is expressed as:

Fg = G⋅(m₁⋅m₂)/d²

The gravitational force (Fg) influences the wavelength (λ), causing redshift, although c remains constant. This is possible because the frequency (f) of the wave or photon must also change due to their relationship f∝1/λ. As the wavelength increases due to the gravitational force (Fg), the frequency (f) correspondingly decreases, ensuring that c remains constant. A reduction in f leads to a reduction in the energy (E) of the wave, as described by E=hf. Consequently, the energy of the wave or photon decreases due to the gravitational force (F_g) until this force becomes negligible, according to the relationship Fg = G⋅(m₁⋅m₂)/d².

When the wave or photon moves beyond the gravitational influence, it no longer experiences redshift or blueshift due to gravity. Beyond gravitational influence, dark energy, which exhibits antigravitational properties, can become significant. This is discussed in the study "Dark energy and the structure of the Coma cluster of galaxies" by Chernin et al. (2013), where dark energy's repulsive effect influences the structure of the Coma cluster. The effective mass of dark energy is considered negative due to its repulsive nature, impacting the cluster's dynamics.

In the context of cosmic expansion, this means that as the wave or photon travels through regions where dark energy dominates, the increasing distance due to cosmic expansion affects the observed wavelength (λ) and frequency (f). While light always travels at the speed c in a vacuum, the increasing distance (c+Δd) due to cosmic expansion can be interpreted as (c+Δd)>c. However, the intrinsic speed of light remains c.

Thus, gravitational influences and cosmic expansion affect the frequency and wavelength of light but do not alter the constancy of the speed of light (c) in a vacuum.

References:

Chernin, A. D., Bisnovatyi-Kogan, G. S., Teerikorpi, P., Valtonen, M. J., Byrd, G. G., & Merafina, M. (2013). Dark energy and the structure of the Coma cluster of galaxies. Astronomy & Astrophysics, 553, A101. https://doi.org/10.1051/0004-6361/201220781

#gravitationalredshift, #cosmicredshift, #darkenergy, #cosmicexpansion, #photonenergy, #frequencywavelengthrelationship, #antigravity, #Zerogravityradius

Group Velocity and Group Velocity Dispersion:

Group Velocity

Definition:

Group velocity (v𝑔) is the speed at which the envelope of a wave packet or a group of waves travels through a medium. It is defined as the rate at which the overall shape of the waves' amplitudes—known as the modulation or envelope—moves through space.

Mathematical Expression:

If we consider a wave packet consisting of a range of frequencies, the group velocity can be expressed as:

v𝑔 = dω/dk

​where:

ω is the angular frequency of the wave.

k is the wave number.

Physical Significance:

The group velocity represents the velocity at which information or energy is conveyed by the wave packet. For example, in optical fibres, the group velocity determines how quickly a light pulse travels down the fibre.

Group Velocity Dispersion (GVD)

Definition:

Group velocity dispersion (GVD) refers to the phenomenon where the group velocity varies with frequency. This occurs because different frequency components of the wave packet travel at different speeds, leading to the spreading or broadening of the packet as it propagates.

Mathematical Expression:

GVD is often quantified by the second derivative of the angular frequency with respect to the wave number:

D = d²ω/dk² 

Alternatively, it can be expressed in terms of the group delay 

τ𝑔 = dϕ/dω 

​

where ϕ is the phase of the wave. The GVD parameter D can then be related to the group delay by:

D = dτ𝑔/dω

 

Physical Significance:

When GVD is present, the wave packet spreads out over time because different frequency components move at different velocities. This effect is crucial in fibre optics, where it can lead to pulse broadening, affecting the performance of optical communication systems.

Key Concepts and Implications

1. Normal and Anomalous Dispersion:

• In regions of normal dispersion, higher frequency components travel slower than lower frequency components (positive GVD).

• In regions of anomalous dispersion, higher frequency components travel faster than lower frequency components (negative GVD).

2. Pulse Broadening:

• In optical fibres, GVD causes pulses to broaden over long distances, which can limit the bandwidth and the distance over which data can be transmitted without significant distortion.

• Dispersion management techniques are employed to mitigate the effects of GVD in communication systems.

3. Applications:

• In ultrafast optics, controlling GVD is essential for the generation and manipulation of ultrashort laser pulses.

• In seismology, understanding GVD helps in the analysis of seismic waves to infer properties of the Earth's interior.

Example

Consider a Gaussian pulse traveling through an optical fibre. Due to GVD, the pulse broadens as it propagates. If the initial pulse has a temporal width τ₀ and the fibre has a GVD parameter β₂, the pulse width after traveling a distance z becomes:

τ(z) = τ₀√{1+(4β₂z/τ₀²)}²

This equation shows how the initial pulse width τ₀ evolves with distance z under the influence of GVD.

Summary

• Group velocity is the speed at which the envelope of a wave packet moves, important for determining the speed of information transfer.

• Group velocity dispersion describes how different frequency components of a wave packet travel at different speeds, leading to the spreading of the packet over time.

Both concepts are fundamental in understanding and designing systems that rely on wave propagation, such as optical communication networks and signal processing devices.

#groupvelocity #GroupVelocityDispersion

The Dynamics of Gravity and Antigravity:

Soumendra Nath Thakur
ORCiD: 0000-0003-1871-7803

08-06-2024

In a gravitationally bound system, the gravitational field is nearly constant and does not propagate in the usual sense.

However, gravity restricts the speed of objects within its influence. The speed of light is determined by gravity.

In the absence of gravity, there may be no speed limit, as there would be no gravitational force to impose such a restriction.

A negative mass can repel a gravitationally bound body if it comes within the range of antigravity.

The rate at which it repels depends on the respective masses, specifically between the effective mass of the antigravity source and the gravitational mass of the object.

The gravitational field moves with the gravitating object at the same speed as the object itself.

The extent of the gravitational field of a gravitating object is limited to its zero-gravity sphere. Beyond this, dark energy prevails.

The interaction between gravity and antigravity can propel a gravitationally bound object much faster than the speed of light.

The effective mass of dark energy, which causes antigravity, is less than zero (<0), yet antigravity can repel a gravitational mass that is greater than zero (>0).

The negative effective mass of antigravity is greater than the gravitational mass, enabling antigravity to dominate.

Gravitational interactions occur between gravitational fields rather than between the masses themselves, meaning that a massive body does not limit speed—its gravitational field does.

Thus, in a gravitationally bound system, speed is constrained by gravity, specifically the gravitational fields. The speed of light is dictated by gravity, not the gravitating body.

Therefore, gravitational interactions may produce energy-carrying gravitational waves whose speed is governed by gravity. The gravitational field itself does not have an independent speed but moves at the speed of the gravitating object.

Comparative Study: Classical and Relativistic Mechanics - Principles, Examples, and Discrepancies in Length Contraction Predictions:

Soumendra Nath Thakur

ORCiD: 0000-0003-1871-7803

08-06-2024

Abstract:

This study investigates the principles of classical and relativistic mechanics, exploring their applications through examples and analysing the differences in length contraction predictions. Classical mechanics concepts such as Newton's second law and Hooke's Law are discussed, alongside relativistic mechanics principles including the Lorentz factor. The study provides examples of both classical deformation and relativistic length contraction, demonstrating how these phenomena manifest at different velocities. By comparing the predicted length contractions, significant discrepancies are identified, particularly at higher velocities. Factors contributing to these differences, such as acceleration-related length deformation and the limitations of the Lorentz factor, are examined. 

Keywords: classical mechanics, relativistic mechanics, length contraction, Lorentz factor, Newton's second law, Hooke's Law, velocity, acceleration,

Lorentz factor (γ):

The Lorentz factor (γ), introduced by Albert Einstein, quantifies the effects of special relativity on time, length, and relativistic mass for objects moving relative to an observer. It is defined by the equation γ = 1/√(1-v²/c²), where v is the velocity of the moving object and c is the speed of light. At rest (v=0), γ=1, indicating no time dilation or length contraction.

As velocities increase, the Lorentz factor approaches 1, indicating negligible relativistic effects. For example, at v=100 m/s, γ≈1.0000000000000556, and at v=1,000,000 m/s, γ≈1.0000055556. The Lorentz factor becomes significant when it exceeds 1.1, corresponding to velocities approaching 0.413 times the speed of light (41.3% of c), such as v=123,900,000 m/s.

Comparison between classical deformation and relativistic length contraction reveals significant discrepancies in relativistic predictions for length changes under similar conditions. Relativistic length contractions are notably smaller than their classical counterparts, as evidenced by the differences measured.

In classical mechanics:

1. The equation v = u + at relates the initial velocity (u), acceleration (a), time (t), and final velocity (v).

2. Newton's second law states F = ma, where force (F) is directly proportional to acceleration (a) and inversely proportional to mass (m).

3. Hooke's Law expresses the relationship between length deformation (ΔL) and applied force (F): F = k⋅ΔL, where k is the spring constant.

4. The spring constant (k) is calculated as k = F/ΔL, where F is the applied force and ΔL is the displacement.

Given an object with mass m = 10g and a spring constant k = 29979.2458N/m, initial velocity u = 0 m/s:

For velocities v=100m/s, v=1,000,000m/s, and v=123900000m/s, time (t) can be determined from (v−u) = 100m/s, yielding t = 1 second.

Using F = ma, forces (F) are calculated for each velocity. Then, ΔL is determined using ΔL = F/k.

The respective deformations (ΔL) for the given velocities are approximately:

• ΔL ≈ 3.34 × 10⁻⁵ m for v = 100 m/s

• ΔL ≈ 0.333 m for v = 1,000,000 m/s

• ΔL ≈ 41.32 m for v = 123,900,000 m/s

To find the total lengths after deformation, add these values to the original length of 1 meter:

• For v = 100 m/s: Total length ≈ 1 meter + 3.34 × 10⁻⁵ m

• For v = 1,000,000 m/s: Total length ≈ 1 meter + 0.333 m

• For v = 123,900,000 m/s: Total length ≈ 1 meter + 41.32 m

These total lengths represent the final lengths of the object after deformation.

Relativistic Mechanics Examples:

Given an object with a rest length (L⁰) of 1 meter and a rest mass of 10 grams (0.01 kg), initially at rest (v = 0 m/s), the object separates from the reference frame at t = 0 s and achieves velocities of 100 m/s, 1,000,000 m/s, and 123,900,000 m/s respectively.

To calculate the length contraction (ΔL) for each velocity using the Lorentz factor (γ), we employ the formula ΔL = γ⋅L⁰.

Using the speed of light (c ≈ 3 × 10⁸ m/s), we find:

1. For v = 100 m/s:

γ ≈ 1.0000000000000556

ΔL ≈ 1.0000000000000556 m

2. For v = 100,000 m/s:

γ ≈ 1.0000055556

ΔL ≈ 1.0000055556 m

3. For v = 123,900,000 m/s:

γ ≈ 1.1

ΔL ≈ 1.1 m

These values represent the change in length (contraction) relative to the observer due to the object's motion, with the original length L⁰ being 1 meter.

Comparison between Classical deformation and relativistic length contraction:

Comparison between classical deformation and relativistic length contraction reveals significant discrepancies in their predictions for length changes under similar conditions. Relativistic length contractions are notably smaller than their classical counterparts, as evidenced by the following differences:

At v = 100 m/s, the relativistic contraction is 0.000033399999444m smaller.

At v = 1,000,000 m/s, the relativistic contraction is 0.3329944444m smaller.

At v = 123,900,000 m/s, the relativistic contraction is 41.22 m smaller.

These differences arise due to several factors. Firstly, the relativistic Lorentz factor (γ) does not account for acceleration-related length deformation as the moving frame transitions from rest to the desired velocity. Additionally, it does not consider the stiffness of the material or the spring constant (k), leading to unaccounted changes in length.

Moreover, the applicability of the Lorentz factor is limited in everyday scenarios where speeds are well below the speed of light. Furthermore, the traditional application of γ·mc² is not suitable for processes involving speeds equal to or exceeding the speed of light, such as nuclear conversions of mass into energy. Therefore, the relativistic Lorentz factor is flawed and inferior to classical mechanics' interpretations of material deformation (ΔL).

#classicalmechanics, #relativisticmechanics, #lengthcontraction, #lorentzfactor, #NewtonsSecondLaw, #hookeslaw, #velocity, #acceleration,

The products of nuclear processes in brief:

Nuclear reactions like fission and fusion split large nuclei, releasing heat and gamma rays, and merge light nuclei, releasing energy, while radioactive decay loses energy through radiation to unstable nuclei.

Nuclear fission products are atomic fragments left after a large nucleus splits into smaller nuclei, releasing heat energy and gamma rays. Nuclear fusion involves merging two light nuclei to form a single heavier nucleus, releasing energy as the resulting mass is less than the original nuclei's. Radioactive decay is the process by which an unstable atomic nucleus loses energy through radiation.

Nuclear Fission:

• In nuclear fission, large nuclei split into smaller fragments, releasing heat energy and gamma rays.

• The products of nuclear fission are atomic fragments (such as isotopes of different elements) resulting from the splitting process.

Nuclear Fusion:

• Nuclear fusion involves merging two light nuclei to form a single, heavier nucleus.

• This process releases energy because the resulting mass is slightly less than the sum of the original nuclei’s masses.

Radioactive Decay:

• Radioactive decay occurs when an unstable atomic nucleus spontaneously emits radiation.

• During decay, the unstable nucleus loses energy, leading to the transformation of the nucleus into a more stable state.

The nuclear reactions encompass both fission and fusion, each with distinct outcomes.

Keywords: nuclear reactions,  fission, fusion, radioactive decay,

#NuclearReactions #fission #fusion #RadioactiveDecay