Relativity and the universal speed limit

In summary, Relativity has shown that ANY acceleration still produces diminishing additional velocity as you approach c asymptotically.
  • #1
helpimagenius
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0
Hey guys, this is a question that has been bothering me since I finished my special relativity course last year.

I was told that nothing can travel faster than the speed of light. Thinking relativistically, I take this to mean no one thing in the universe can travel faster than any other thing in the universe by a difference 'c'. This seems like a difficult condition to satisfy-- with so many objects moving around in different directions, some of them spinning really fast, like neutron stars, they would have to be configured just so... I guess it's just hard for me to imagine why, if I am in a space ship, I can't just keep accelerating in one direction. Will my constant thrust start producing diminishing acceleration after a while? Put another way, if some object is hurtling towards me at c/2, will it be easier for me to accelerate away from the object than towards it?
 
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  • #2
helpimagenius said:
Hey guys, this is a question that has been bothering me since I finished my special relativity course last year.

I was told that nothing can travel faster than the speed of light. Thinking relativistically, I take this to mean no one thing in the universe can travel faster than any other thing in the universe by a difference 'c'. This seems like a difficult condition to satisfy-- with so many objects moving around in different directions, some of them spinning really fast, like neutron stars, they would have to be configured just so... I guess it's just hard for me to imagine why, if I am in a space ship, I can't just keep accelerating in one direction. Will my constant thrust start producing diminishing acceleration after a while? Put another way, if some object is hurtling towards me at c/2, will it be easier for me to accelerate away from the object than towards it?

Yes, Relativity has shown that ANY acceleration still produces diminishing additional velocity as you approach c asymptotically.
 
  • #3
Another form of this question that sometimes throws people: I have a gun that fires a bullet with a muzzle velocity of .5c, point it in one direction and shoot, then point it in the other direction and shoot. Don't I end up with two bullets moving at speed ##c## relative to one another? Or suppose I mount this gun on a vehicle traveling at .75c and then fire it straight ahead? Don't I end up with a bullet moving at ##1.25c##?

I don't, and the reason is to be found in the rule for "relativistic addition of velocity" which google will find for you pretty quickly. The diminishing acceleration effect that you suspected might exist and phinds confirmed can be derived from this rule.
 
  • #4
The reason why "ANY acceleration still produces diminishing additional velocity" is that as the spacecraft 's speed increases (relative to some reference frame) so does its mass. The closer the speed of the spacecraft gets to the speed of light, the greater the mass gets. that's why "constant thrust" will "start producing diminishing acceleration"- a= f/m.
 
  • #5
HallsofIvy said:
The reason why "ANY acceleration still produces diminishing additional velocity" is that as the spacecraft 's speed increases (relative to some reference frame) so does its mass. The closer the speed of the spacecraft gets to the speed of light, the greater the mass gets. that's why "constant thrust" will "start producing diminishing acceleration"- a= f/m.

Using relativistic mass? A little outdated?

The explanation in terms of 4-velocity and 4-acceleration, translated to English description, suggests that time dilation is the key concept not change of mass. Thus any finite acceleration experienced in the momentarily comoving frame of the accelerating body, when translated back to a frame where the object is moving near c, causes the experienced acceleration (proper acceleration) to be divided by gamma (due to dt versus d tau). As a result, any finite acceleration pattern experienced by a body, when referred to a give inertial frame, always has speed < c, and coordinate acceleration decreasing as speed approaches c.
 
  • #6
PAllen said:
Thus any finite acceleration experienced in the momentarily comoving frame of the accelerating body, when translated back to a frame where the object is moving near c, causes the experienced acceleration (proper acceleration) to be divided by gamma (due to dt versus d tau).
Actually, there's a bit more to the calculation than this, and the factor is [itex]\gamma^3[/itex], not [itex]\gamma[/itex].
 
  • #7
DrGreg said:
Actually, there's a bit more to the calculation than this, and the factor is [itex]\gamma^3[/itex], not [itex]\gamma[/itex].

... and it actually depends on direction of acceleration in relation to current current velocity in the inertial frame (γ3 is only for collinear). I thought of this right after posting, but didn't want to complicate my main point that the better (IMO) way to look at the barrier is the transformation of acceleration (mass not involved).
 
  • #8
To really think relativistically, it might be good to look at the spacetime viewpoint.
A nonzero-mass particle has a unit 4-velocity, whose tip _always_ lies on the future-timelike unbounded unit-hyperboloid that is asymptotic to the light-cone [in the tangent space].

Since the 4-acceleration is orthogonal to the unit-4-velocity, the 4-acceleration is tangent to the hyperboloid. Thus, the 4-acceleration effectively moves the tip of the unit-4-velocity to another point on the hyperboloid, possibly parametrized by angles [rapidities="arc-lengths on the unit-hyperboloid"]. No matter what is done, the unit-4-velocity is always inside the future-light-cone. The relative-speed (regarded as the ratio of the spacelike and timelike components of the unit-4-velocity wrt the lab-frame's 4-velocity) is bounded by 1 and won't change very much when the relative-rapidity is large (as it rides up near the light-cone in the lab-frame).

In the Galilean case [hindsighted from Minkowski spacetime], the unit-4-velocity would have its tips on the unbounded spacelike-plane where its timelike-component is always 1. In this case, the relative-speed is unbounded (and is proportional to the Galilean analogue of the rapidity). Since our everyday intuition is Galilean, we find it hard to see the SR-case, especially if we rely too heavily on purely Galilean methods.
 
  • #9
Quantum and relativity are so confusing to me. I need help.
 
  • #10
We can help you, but you have to pick one or the other. You can not possibly understand both at once because they are incompatible ;)
 
  • #11
QM and special relativity are compatible. And QM is even compatible with curved spacetime, so I wouldn't say they are incompatible without some qualifications.
 
  • #12
helpimagenius said:
I was told that nothing can travel faster than the speed of light.

This is true.

helpimagenius said:
I was told that nothing can travel faster than the speed of light. Thinking relativistically, I take this to mean no one thing in the universe can travel faster than any other thing in the universe by a difference 'c'.

This is true. However if I observe one object traveling away from me at 0.75c and another object traveling away from me in the opposite direction at 0.75c, I measure their relative velocity as 1.5c.

helpimagenius said:
Put another way, if some object is hurtling towards me at c/2, will it be easier for me to accelerate away from the object than towards it?

Yes, in the sense that the rate of change of your relative velocity as measured by you will be higher if you accelerate away from the object. The rate of change of your velocity measured by an independent observer will be the same either way.

Nugatory said:
Another form of this question that sometimes throws people: I have a gun that fires a bullet with a muzzle velocity of .5c, point it in one direction and shoot, then point it in the other direction and shoot. Don't I end up with two bullets moving at speed ##c## relative to one another?

As measured by you, yes.
 
  • #13
Nugatory said:
Another form of this question that sometimes throws people: I have a gun that fires a bullet with a muzzle velocity of .5c, point it in one direction and shoot, then point it in the other direction and shoot. Don't I end up with two bullets moving at speed ##c## relative to one another?

MrAnchovy said:
As measured by you, yes.

The separation speed of the two bullets, as measured by you in your reference frame, is c. That is, the distance between the two bullets increases at the rate c in your reference frame.

The relative speed of the two bullets is 0.8c, as per the "relativistic velocity addition" formula. This is the speed of one bullet in the reference frame in which the other one is stationary, i.e. the speed of one bullet as "observed" by the other one.

http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/einvel2.html#c2

(be careful of + and - signs for the different directions)
 
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What is relativity?

Relativity is a theory developed by Albert Einstein in the early 20th century that describes how the laws of physics apply to objects moving at different speeds. It includes the principle of the universal speed limit, which states that the speed of light is the maximum speed at which all matter and information in the universe can travel.

What is the universal speed limit?

The universal speed limit, also known as the speed of light, is the maximum speed at which all objects and information in the universe can travel. It is approximately 299,792,458 meters per second, or about 670 million miles per hour. According to the theory of relativity, nothing can travel faster than the speed of light.

How does the theory of relativity impact our understanding of the universe?

The theory of relativity has had a significant impact on our understanding of the universe. It explains the relationship between space and time, and has led to advancements in technology such as GPS. It also predicts phenomena such as gravitational lensing and time dilation, which have been observed and confirmed through experiments.

What are the two types of relativity?

The two types of relativity are special relativity and general relativity. Special relativity deals with the laws of physics in inertial (non-accelerating) frames of reference, while general relativity extends these laws to include accelerated frames of reference and the effects of gravity on space and time.

Is the theory of relativity proven?

The theory of relativity has been extensively tested and confirmed through experiments and observations. However, like all scientific theories, it is always subject to further investigation and refinement. So far, it has been able to explain and predict a wide range of phenomena, making it one of the most successful and widely accepted theories in physics.

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