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# Relativity Challenge ľ part 2

### Dealing with acceleration and gravity In the previous chapter we looked at a number of situations in which clocks moved at different constant velocities but without experiencing gravity or acceleration.  There it argued it was possible to construct scenarios where one could not favour one clock over another, in terms of having one experience more time dilation.  It ended up applying these scenarios to the traditional ĹTwins Paradoxĺ story and concluded that they should have the same age upon return.

In this chapter weĺll do the same but this time include the effects of gravity and acceleration.  It will make reference so something called the Principle of Equivalence.  The details of this thought experiment may seem overdone but they are required to counter the many possible objections that might arise from Special and General Relativity (SR and GR) supporters.

#### The Situation

In the first preliminary step we take Earth and relocate it far into intergalactic space.  It will be far enough out such that gravity from the nearest galaxy is a trillion times less than Earthĺs surface gravity.  The reason for doing this is firstly so that we donĺt need to consider the gravity of surrounding stellar bodies, and secondly to remove the motion of the Earth around the Sun and Milky Way from consideration.

Next we prevent the Earth from rotating.  Likewise we do this to avoid having to consider the SR/GR effects of the rotation speed and the small amount of centrifugal force it provides.

Now to begin the story.

A rocket sits on the Earthĺs surface with a large supply of fuel.  Inside it is a room with living facilities and enough food and oxygen to support an occupant for many months.  It also contains an accurate atomic clock.  Beside the launch pad is an identically-fitted room.  It contains a similar clock that has been synchronised with the one aboard the rocket.  There is also a third clock on the opposite side of the Earth that is synchronised with the other two.

Two identical twins agree to take part in the experiment.  Each will spend the next several months either in the rocket or the Earth room, but neither will know which.  Prior to launch, they are both given a sedative and put to sleep.  Each twin is then randomly assigned to be moved into either the rocket or the stationary room.

The rocket lifts off.  At first, very slowly so as not to apply much acceleration.  Then as it moves further from Earth and gravity decreases, the rocket increases its acceleration to Ĺfill inĺ what is missing from Earthĺs gravity.  This acceleration will be steadily increased so that the gravity felt at all times will be exactly equal to 1G.  That is, the gravity measured by an on-board accelerometer (as the sum of real plus artificial gravity) will measure the same as on Earth.  Assume that the rocket engine is silent and acceleration is smooth.

Shortly after launch, when the acceleration has steadied to 1G, the twins wake up.  Neither of them know which room they are in.  The rooms are identical in layout and both experience what appears to be gravity.  If they drop something it will accelerate toward the floor at 9.81m/s2, i.e. at 1G.

Now according to the Principle of Equivalence (also called the strong equivalence principle), as proposed by Einstein and frequently described in terms of falling elevators and rising rockets, the situation inside the two rooms is essentially identical.  That is, there is no experiment you could devise that would allow either of the twins to determine which room they are in.  We will also assume the rooms are not very tall.  This is to prevent an occupant in the Earth-room from measuring slightly less gravity near the ceiling.

Question:  According to the combined rules of SR and GR, will one of the clocks be ahead of the other, and if so, what is the reason for selecting that clock instead of the other?

The fact that the clocks are moving away from each other means they must somehow have different velocities, otherwise they would remain a fixed distance apart.  Therefore according to SR, time dilation should be occurring and the faster-moving clock should be running more slowly.  But since the relative speed between the Earth and rocket is at all times exactly equal from both viewpoints, there appears to be no way of determining which is Ĺfasterĺ.  As for GR, since the acceleration-slash-gravity situation of both rooms is exactly equal at all times (other than the brief lift-off), according to the Equivalence Principle it would appear we are also unable to favour one clock over the other.

So we are left with a conundrum: either we find a way of favouring one clock over the other or we agree that no time difference accumulates between then.

Now an objection might be that we have no way of comparing the clocks without one of them stopping and reversing, which would destroy the symmetry of the situation.  And so the question of which of them runs faster up until that point is somehow hypothetical or meaningless.  But this avoids the issue because the question here is about which clock according to the theory of SR and GR, runs slower.  Unlike the ĹCopenhagen Interpretationĺ of quantum mechanics, relativity does not depend on observers to determine the reality of a situation.  So the answer to this question wonĺt depend on the clocks ever being compared or not.

Still, this objection can be overcome and will be addressed in the remainder of this essay.

After travelling for 10 months, and using a simple classical mechanics calculation, we could determine that the rocket is moving at 87% the speed of light (relative to Earth, which is now relocated outside our galaxy).  At this speed we get a Lorentz factor of 2.  This might mean that either the rocket or Earth clock is running half the speed of the other.  These numbers however are not so important because we mainly care about which clock is ahead of the other, and not by how much (although we are also interested in that!).  So letĺs just pick 10 months as an arbitrary duration and assume a rough Lorentz factor of 2 at that point.  This factor will be sufficient to override minor clock-drift errors, measurement errors, and brief periods where the acceleration of the rocket is not 1G, such as the launch and rotation (as described later).  It should also cause noticeable differences in what the twins remember about the duration of their journey, assuming that one is Ĺrunningĺ half the speed of the other.

So after travelling for 10 months (according to the local clock) the occupant aboard the rocket will take a sedative.  The same will occur at the Earth-room (according to their clock).  Both twins will then sleep for a while.  The rocket engine will then be stopped, allowing the craft to drift freely in space with no acceleration.  It will then be gently rotated 180 degrees to face the opposite direction ľ now pointing at Earth.  The engine will then be started again, applying an acceleration force of exactly 1G.  Both twins will then wake up.

When the rocket-twin awakes, he notices no difference.  Just as before, he experiences what feels like a gravitational force of 1G toward the floor.  The Earth-twin experiences the same.  The rocket is facing the opposite direction and is now decelerating, but by all accounts everything according to the Equivalence Principle is the same.  There is still no experiment either twin could perform to determine which is experiencing gravity.

Therefore it would seem that according to GR, both clocks should still be running at the same rate.  And since the relative velocity is still identical ľ that aspect never changes ľ the clocksĺ situation is still symmetrical according to SR.

An objection here might be that there is a difference because the clocks are experiencing Ĺgravityĺ in opposite directions.  And therefore the clock on the rocket will now be faster or slower (pick one!) than the one on the Earth.  For those who raise this objection, refer instead to that third clock placed on the other side of the Earth.  It is still in-synch with the first Earth clock and now experiencing gravity in exactly the same direction as the rocket.

To continue the story, the deceleration process continues for the same time as the original acceleration process (10 months), at which point the rocket comes to rest relative to Earth.  However the engine doesnĺt stop.  Instead it continues to apply exactly the same amount of force.  Deceleration becomes acceleration and the occupant notices nothing unusual.

The acceleration continues for the next 10 months (according to the local clock) until the rocket reaches (presumably) the original rotation point.  At this point (according to their own clocks), both twins are put to sleep, the rocket is rotated 180 degrees, and then starts to decelerate while pointed away from Earth.  Both twins awake and notice nothing unusual in their Ĺgravityĺ situation.

The rocket continues its deceleration in a perfect reverse of its original departure, steadily coming to a stop relative to Earth, and all the while carefully adjusting its acceleration to give an on-board experience of 1G.  Just prior to landing, both twins are put to sleep and then awoken after landing.

The rocket has now landed beside the replica Earth room.  Neither twin has yet to emerge, and neither still has any idea which one of them was aboard the rocket.

Not that it matters.  This story was never about the twins, it was about the atomic clocks.  The twins were just there to make it interesting and to bring it in line with the historical thought experiments such as falling elevators and the ĹTwins Paradoxĺ.

So to state the obvious question: allowing for minor clock-drift errors and the brief periods of launch, landing, and rotation, when the clocks are compared side-by-side, which of them will have recorded more time?  And why not the other way around?

And while weĺre at it, which of the twins will be older?

#### Discussion

Now that the story has been told, itĺs worth anticipating with what objections might arise.  Several things can be predicted about how relativity supporters will handle this:

1.    They wonĺt accept the twins could be of the same age.
2.    They will have difficulty agreeing on which twin will be older.
3.    For those who do agree, they wonĺt agree on the reasons for it.
4.    They will have different calculations for the age difference.

Understandably itĺs complicated and ends up something like the Ehrenfest Paradox, where everyone agrees relativity should somehow apply but are not sure how to do it.  Still, letĺs see what can be done.

Usually to analyse situations involving both aspects of relativity we need to separately determine the contributions from SR and GR then add them together.  At least thatĺs how itĺs done when calculating the GPS 38-microsecond-per-day time difference.

Calculating the contribution from SR should be easy because we know the velocity at all stages.  Presumably we would plug it into the Lorentz transform and predict the amount of time dilation rate at any point along the way.  That is, we can determine how much slower time will be running aboard the moving rocket.

Except that we have an obvious problem in that the Earth is moving away from the rocket at the exact same velocity.  And so Earth should also be running slower than the rocket and by the same rate.

At this stage of the argument, relativists would typically resort to a number of fall-backs:

1. Start discussing other aspects of SR such as length contraction, simultaneity, and additive velocities.
2. Claim that both are running slower than each other, and/or that the calculated amounts of time dilation refer only to perceived rates of slow down, not actual slow down.
3. Claim that the brief turnarounds are all that is needed to break symmetry and cause one twin to be several months older than the other.
4. Claim that the small amount of acceleration at lift-off is all that is needed to break symmetry and cause one twin to be several months older than the other.
5. Ignore the thought experiment and discuss various real-world experiments.
6. Claim that only the rocket slows down because the Earth is somehow a special/universal reference frame that all velocities need to be compared to.
7. Claim that SR only applies to the rocket because it experiences acceleration.

These are popular claims, and itĺs worth addressing each of them before covering the final point (7) in detail:

1.   Start discussing other aspects of SR such as length contraction, simultaneity, and additive velocities.

This isnĺt going to help because the situation is symmetrical.  Whatever you apply to one clock you must also apply to the other, affecting both clocks by the same degree.  So the situation remains symmetrical and there is still no way of selecting one clock over the other.

2.   Claim that both are running slower than each other, and/or that the calculated amounts of time dilation refer only to perceived rates of slow down, not actual slow down

This claim is nullified because the story involves the clocks coming back together and compared side-by-side.  If time dilation was only perceived/illusionary on the first quarter of the journey, then it would have to be perceived/illusionary on all quarters since they all involve the same amount of acceleration.  This is particularly true of the transition from the second to third stage because acceleration stayed perfectly constant during that time.

3.   Claim that the brief turnarounds are all that is needed to break symmetry and cause one twin to be several months older than the other.

Note that the turnarounds represent at most 100 seconds out of 40 months and the challenge question asked you to ignore any time differences arising from these moments.  For someone to claim this could cause one twin being several months older than the other must be desperate.  Astronauts experience strong accelerations and long periods of weightlessness without becoming noticeably younger.  Aside from that, the person claiming this is also saying none of these months of difference would have accumulated prior to the first turnaround.

4.   Claim that the small amount of acceleration at lift-off is all that is needed to break symmetry and cause one twin to be several months older than the other.

This is another desperate claim.  The rocket lifts off at very slow constant velocity, e.g. at a snailĺs pace.  Now it is true that to get this initial velocity requires a small amount of acceleration.  And perhaps that tiny amount somehow shifts the rocket into a different Ĺreference frameĺ that allows a time difference to steadily accumulate.  Fortunately this can also be overcome by modifying the experiment to say that after lift-off, the rocket will delay applying its own acceleration to make up the difference.  That is, the rocket clock will experience a brief period of <1G to compensate for the brief period of >1G.

5.   Ignore the thought experiment and discuss various real-world experiments.

This is a popular debating technique that allows opponents to avoid the question.  While such experiments are interesting, they canĺt be used to answer it because any number of explanations can be proposed to fit the observations.  Also, we canĺt be sure if specific experiments were properly conducted, making them uncertain.  Since this a thought experiment, all the information required to answer it should be contained in the SR and GR theory ľ there is no need to refer to actual experiments.  Respondents need to explain how the theory answers the question.  If it canĺt be answered by the theory then the theory is deficient.

6.   Claim that only the rocket slows down because the Earth is somehow a special/universal reference frame that all velocities need to be compared to.

Relativists never say this outright but they often end up stating it indirectly.  Seeing that the Earth is now located in intergalactic space, this is going to be very difficult to justify, if it were not difficult enough already.  We have known since the time of Galileo that the Earth has no special position in space.  And in fact Galilean Relativity is contained in the first postulate of SR.  So SR followers have no excuse to be ignorant of it!

7.   Claim that SR only applies to the rocket because it experiences acceleration.

This is often what gets brought up when discussing the traditional Twins Paradox story.  But seeing as the Earth twin experiences the same amount of Ĺaccelerationĺ as the rocket, this would also appear to be an invalid objection in this case.

#### The Principle of Equivalence

This brings us to the focal point of the story.  Namely that the gravity/acceleration was the same for both clocks/twins, and therefore according the to the Equivalence Principle, there should be no way of selecting one clock over the other.

This principle can be stated a number of ways.  Hyperphysics does it like so:

ôExperiments performed in a uniformly accelerating reference frame with acceleration a are indistinguishable from the same experiments performed in a non-accelerating reference frame which is situated in a gravitational field where the acceleration of gravity = g = -a = intensity of gravity field.ö 

Einstein used a number of similar statements before settling on:

ôWhenever an observer detects the local presence of a force that acts on all objects in direct proportion to the inertial mass of each object, that observer is in an accelerated frame of reference.ö

Normally such experiments would involve dropping objects and watching them accelerate Ĺdownwardĺ at a fixed rate independent of the objectĺs mass.  They could also involve watching a horizontal light beam curve toward the floor (which will certainly happen if the floor is accelerating upward, but is also said to happen in the presence of gravity).

The experiment performed in this story involved atomic clocks and finding how much faster/slower they ran in gravitational versus accelerated situations.  There is no falling involved but nonetheless this is still an experiment by definition.   So presumably a clock in constant 1G gravity should run at the same rate as a clock in constant 1G acceleration.  The fact that the clocks cannot be compared while the experiment is in progress should not be an issue because when the comparison eventually takes place, both clocks will have been experiencing 1G at all times, other than the brief moments of turn-around and lift-off/landing (whose microscopic contributions we allow for in the comparison ľ we are looking for large time differences in the order of months).

#### Time dilation due to gravity

Letĺs now look at GR theory and see what it says about gravity, in terms of predicting time dilation.  Since time dilation is often attributed to gravity, one might assume there must be an equation that can tell you how much dilation will be caused by a given amount of gravity.  But thatĺs not the case.  GR describes time dilation not according to gravitational acceleration but gravitational potential.  These two things are very different.

Here is what the equation looks like : ----   (1)

Where γ (gamma) is the rate of dilation (the rate time slows down) and Φ (phi) is the potential.

Gravitational potential refers to the amount of energy required to lift a unit mass (i.e. 1kg in SI units) from its present height, all the way to an infinite height.

We know that gravitational acceleration can be measured by dropping an object and observing how it falls.  We can also measure it in terms of a static force, e.g. by placing a unit mass on some scales.

But gravitational potential is impossible to detect, let alone measure.  The only way to determine it is to measure the acceleration function of gravity all the way to a height of infinity, which obviously canĺt be done.

In theory you could also determine it by multiplying the surface gravity by the radius of the planet you are on.  But this would only work if the planet was: (a) spherical, (b) non-rotating, (c) of uniform density, or the density was Ĺradially symmetricĺ i.e. identical at any given radius.

So how is it possible for clocks to time-dilate according to something that can never be detected?  Not just detect from where they are located, but not detect no matter how they move about, assuming they were allowed to.

Or are GR proponents saying that clocks are somehow aware of the shape of the planet they are on, their density distribution, and their distance from the mid-point?  Do clocks have Ĺremote viewingĺ abilities?  If so youĺd think some relativity expert would have bought that exciting fact to our attention!

Either of these claims should be seen as impossible.  And this alone is sufficient to demolish the GR gravitational time dilation equation as a possibility.  It also demolishes the Equivalence Principle because it admits the time dilation Ĺequivalenceĺ is not due to acceleration but potential.

At this stage, there doesnĺt seem much point in going further because all the claims relating to SR and GR have been shown as unworkable.  Unless that is, you are a geocentrist and believe clocks have psychic powers.

Still, there is another aspect that should be addressed: acceleration.

#### Time dilation due to acceleration

A final aspect to consider is the amount of time dilation due to acceleration.

Relativity supporters often talk about how acceleration affects time dilation.  This is especially so when discussing the Twins Paradox, because it allows them to describe non-symmetry and point to that as the reason for one twin aging faster than the other (and without having to explain why).

Therefore it will probably come as a surprise to learn that there is no equation that allows you to determine time dilation in terms of acceleration.

The reason you canĺt make such an equation is that you first need to Ĺneutralizeĺ the acceleration term and make it dimensionless.

To make such an equation for velocity is easy.  Velocity has the units ĹL/Tĺ, which is Ĺlength divided by timeĺ.  So divide that by c (the speed of light), which has the same units, and you are left with a dimensionless quantity: v/c.

This quantity can then be manipulated in certain ways.  In the case of the Lorentz Transform, the quantity is squared, subtracted from one, then square-rooted and inverted.  This gives the familiar: ----   (2)

But doing this with acceleration is a problem.  Acceleration (a) has the units L/T2.  (length divided by time-squared).  You can multiply and divide that by c all you like and it will never become dimensionless.

One way around it is to introduce a length (L) or time (T) into the equation.  E.g.:

a*L/c2

or

a*T/c

Both the above are dimensionless.  But what length and what time do we plug in?  There are no special universal constants available (other than Plank Units but they are too small).

This is also the reason why time dilation for gravity is in terms of potential rather than acceleration.  By multiplying acceleration by a planetĺs radius (a length), we get an expression for potential which has the units L2/T2.  And this can be divided by c2 to Ĺneutralizeĺ the units as shown in equation (1).

The closest SR comes to doing that when calculating time dilation due to acceleration in a centrifuge.  In this case they can multiply the acceleration by the radius of the centrifuge, divide by c2, and then insert it into something similar to gravitational time dilation equation.  Other than convenience, there is really no justification for using the centrifugeĺs radius.

But for linear acceleration there is no convenient distance to refer to.  At least not one that makes logical sense to include in a time dilation equation.

In response to this, some might object and say that we do indeed have such an equation for acceleration.  It is of the form: ----   (3)

Two important points about this.  First, itĺs not an expression for a rate of time dilation but for an overall time difference.  Second, itĺs not in terms of acceleration but velocity.

What this is is an expression for total elapsed time T experienced by a clock that starts at velocity zero, and accelerates at a constant rate of a for a duration of t.  The full derivation can be seen on Wiki 

What is happening is that the acceleration is being used to calculate velocity at a particular point, which is being plugged into the regular Lorentz transform.  This gives a rate of time dilation expressed in terms of acceleration and elapsed time, although it is really based on velocity.

Except the aim of the exercise is to determine the overall amount of time dilation.  So it integrates this rate of time dilation over a duration from 0 to t, giving the final equation (3) as a total elapsed time experienced by the moving object.

By not including v into the equation it looks like the equation is based on acceleration, when in reality it is entirely based on v, and a and t are just shown in place of v.

In essence, this equation doesnĺt justify why the experience of acceleration should cause one clock to run slower than another.  It just allows us to calculate their relative velocity.  As such the equation should be applied equally to both clocks.

Very deceptive.  But then, what else would you expect from relativists?

Acknowledgments:

Credit goes to Tom Hollings for the original story idea.  Tomĺs website discussing various problems with Relativity is here:
http://problemswithrelativity.com

The original scenario was first put on this forum (see halfway down at post #125):

Itĺs worth reading the various excuses from the relativity supporters as they try to Ĺsolveĺ it.  Their creativity is amazing!

  http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/grel.html
  http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/gratim.html  Although most references use G*M/R in place of Φ (potential), or they use g*R.  When calculating the time dilation at the centre of a planet, you need to use Φ = (3/2)G*M/R
  http://en.wikipedia.org/wiki/Time_dilation#Time_dilation_at_constant_acceleration

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