CERN: Accelerating Particles to 99.99% Speed of Light

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Discussion Overview

The discussion revolves around the implications of particle acceleration to speeds approaching the speed of light, specifically in the context of the Large Hadron Collider (LHC) and the principles of special and general relativity. Participants explore the nuances of velocity addition in relativistic physics and the effects of gravitational fields on speed limits.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether the speed of a particle accelerated to 99.99% of the speed of light, when combined with the solar system's velocity, would exceed the speed of light, indicating a potential misunderstanding of relativistic velocity addition.
  • Another participant introduces the relativistic formula for velocity addition, asserting that it ensures the resultant speed remains below the speed of light.
  • A participant explains that in special relativity, velocities are not simply additive, contrasting it with everyday experiences and emphasizing the need for Lorentz transformations.
  • One post discusses the concept of head-on collisions of particles at high speeds, arguing that the kinetic energy and collision dynamics are more complex than simple additive speeds, and highlights the role of electromagnetic guidance in the LHC.
  • Another participant challenges the notion of "net 2c" in collisions, questioning the validity of adding speeds in the context of relativity and referencing previous posts for clarification.
  • A participant introduces concepts from general relativity, suggesting that the ultimate speed may not be limited to the speed of light in the presence of gravitational fields, and discusses the implications of the metric tensor on speed limits.
  • Another post reiterates the points about general relativity and the conditions under which speed limits may vary, emphasizing the distinction between coordinate speed and measurable speed.

Areas of Agreement / Disagreement

Participants express differing views on the implications of relativistic speed addition and the effects of gravitational fields on speed limits. There is no consensus on the interpretation of these concepts, and the discussion remains unresolved.

Contextual Notes

Participants highlight limitations in understanding velocity addition under relativity and the conditions under which general relativity applies, including gravitational fields and non-inertial frames. These factors contribute to the complexity of the discussion without reaching definitive conclusions.

Rikendogenz
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Please correct me where I'm wrong,
Our solar system is moving around our galaxy at 250km/s and CERN can accelerate a particle to 99.99% the speed of light. If you are observing a particle going 99.99% of c from outside our galaxy and it happens to be moving the same direction of our solar system, the total speed would be greater than c... Am I looking at this the wrong way?
 
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You have to use the Relativistic formula for the addtion of velocities:

[tex]w = \frac{u+v}{1+\frac{uv}{c^2}}[/tex]

This will always give an answer of less than c.

BTW, this is the correct formula to use when adding any velocites, But when u and v are small compared to c, the answer comes out to be so close to the answer you get when you just use [itex]w=u+v[/itex], you can use the simpler formula as long as your answer doesn't have to be too exact.
 
Hi Rikendogenz and welcome to PF,

In special relativity speed is not an additive quantity. For example in Euclidean relativity (every day relativity), if your running left at 5 m/s and I am running right at 5 m/s, then my speed relative to you is 5 + 5 = 10 m/s. However, in special relativity this isn't the case one must use Lorentz transformations to determine the relatvie velocity of two moving bodies.

Edit: I see Janus has snook in before me :rolleyes:
 
Head on photon 'collissions' have net 2C as observed from Stationary

From a stationary reference frame (Earth is close to a stationary frame... read special relativity, Einstein talks of the either and preferred reference frames as Isaac Newton did before him, other reference frames are primarily for time dilation...)

the following was a response I made to a similar question...

nbiggershaft said:
You can spot out various fallacies in his arguments though. For example, the statement "particles colliding at double light speed" clearly ignores relativity.
The Large Hadron Collider will collide proton to proton (and sometimes proton to anti-proton) in head on collisions with each set of particles traveling at 99.9999991% of the speed of light. The net collision speed is additive (same calculation as head-on car collisions). The kinetic energy per particle is determined by how close to the speed of light each particle travels. (That is why cosmic rays can have more energy even when the collision is moving to stationary rather than head on at same speed. The difference is how the energy is focused. Head-on collisions of same mass, same speed, exact opposite vector and center mass impact will focus the energy to a single point).

The particles will be guided around the tunnel by more than 1,600 superpowerful, cylinder-shaped ELECTROMAGNETS, some of which weigh more than 30 tons. The protons will zoom around the ring up to 11,245 times per second, reaching 99.9999991% of the speed of light.

At four points in the ring, magnets will push the beams together, causing up to 600 million PROTON COLLISIONS per second. If all goes as planned, these high-speed, high-energy crashes will create bursts of rare forces and particles that haven’t been seen since the big bang 13.7 billion years ago.

Four huge PARTICLE DETECTORS — the biggest, ATLAS, is 150 feet long, 82 feet high, and has more than 100 million sensors — will track and measure the particles at each collision. Filters will discard all but the 100 most interesting crashes per second. This will still produce enough data to fill a 12-mile-high stack of CDs per year.

JTankers
 
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JTankers said:
"Head on photon 'collissions' have net 2C as observed from Stationary" ...

The Large Hadron Collider will collide proton to proton (and sometimes proton to anti-proton) in head on collisions with each set of particles traveling at 99.9999991% of the speed of light. The net collision speed is additive (same calculation as head-on car collisions). The kinetic energy per particle is determined by how close to the speed of light each particle travels. ...
So where is the "net 2c" speed of anything?
Are you really going to add 99% + 99% for a speed faster than 100% of light "c"!
Did you even read post #4 by Janus on how to add speeds.

OR are your posts more about driving traffic to the sites listed in your posts?
You are new here; you need to actually read what is expected of you in the must read first sticky posts.
 
Strictly speaking, SR applies only in the absence of a gravitational field. In GR “c” is not the ultimate speed of either light or material objects, when a gravitational field is present.

In GR, the ultimate speed is determined only by the metric tensor. Following Max Born, if for simplicity we imagine a 2-D subset (x,t) of the 4-D spacetime continuum, and assume the off-diagonal elements of the metric tensor vanish, then the light lines are given by:

ds^2 = g11*dx^2 + g44*dt^2 = 0 --> ultimate speed = dx/dt = SQRT(-g44/g11).

In the flat Minkowski spacetime of SR, g11 = 1 & g44 = -c^2, so we have:

ultimate speed = SQRT[-(-c^2)/1] = c, as expected.

But in the curved Riemannian spacetime that exists when a gravitational field is present (or if you are using a non-inertial frame of reference?), the values of g11 & g44 could in principle be any real numbers, thus placing no theoretical upper limit on the ultimate speed in GR.
 
Prof Niemand said:
Strictly speaking, SR applies only in the absence of a gravitational field. In GR “c” is not the ultimate speed of either light or material objects, when a gravitational field is present.

In GR, the ultimate speed is determined only by the metric tensor. Following Max Born, if for simplicity we imagine a 2-D subset (x,t) of the 4-D spacetime continuum, and assume the off-diagonal elements of the metric tensor vanish, then the light lines are given by:

ds^2 = g11*dx^2 + g44*dt^2 = 0 --> ultimate speed = dx/dt = SQRT(-g44/g11).

In the flat Minkowski spacetime of SR, g11 = 1 & g44 = -c^2, so we have:

ultimate speed = SQRT[-(-c^2)/1] = c, as expected.

But in the curved Riemannian spacetime that exists when a gravitational field is present (or if you are using a non-inertial frame of reference?), the values of g11 & g44 could in principle be any real numbers, thus placing no theoretical upper limit on the ultimate speed in GR.

But that's strictly coordinate speed, not what anyone would measure. If you take the tangent vector of a null path expressed in the orthonormal basis at a point on timelike world line, you always get c exactly. This is the mathematical expression of 'local vacuum speed of light is always c'. It is also required by the fact that semi-Riemannian geometry has flat Minkowski space as a tangent space at every point.
 

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