Does Gravity Exist or Is It Just a Bend in Space-Time?

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Discussion Overview

The discussion revolves around the nature of gravity, questioning whether it is a fundamental force or a result of the curvature of space-time. Participants explore various analogies and conceptual frameworks, including elastic bands and rubber sheets, to understand gravity's effects on mass and motion. The conversation touches on theoretical implications, interpretations of general relativity, and the challenges of grasping these concepts.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that gravity acts like an elastic band, with stronger mass resulting in a stronger pull, while others argue that gravity may not exist as a force but rather as a consequence of space-time curvature.
  • A participant suggests that both views (gravity as a force vs. gravity as curvature) yield similar results in terms of motion, using the snowflake analogy to illustrate this point.
  • Another participant emphasizes that Einstein's theory of relativity describes gravity as the curvature of space-time, where objects follow the shortest path in this curved geometry.
  • There is a discussion about the limitations of analogies, such as the rubber sheet model, and how they may not fully capture the complexities of general relativity.
  • Some participants express confusion about the implications of mass movement and acceleration in relation to gravity, questioning how the Earth and other masses interact in this framework.
  • One participant mentions that not all objects follow straight lines in curved space-time, highlighting the distinction between free-falling objects and others.
  • There are references to the challenges of understanding gravity, with some participants acknowledging the difficulty of the topic and the need for further study.
  • Several participants critique the use of certain analogies, suggesting that they may misrepresent the nature of gravitational interactions.

Areas of Agreement / Disagreement

Participants express a range of views on the nature of gravity, with no consensus reached. Some agree on the conceptual framework of space-time curvature, while others maintain differing perspectives on the existence of gravity as a force.

Contextual Notes

Limitations in understanding arise from the complexity of general relativity and the inadequacy of certain analogies to fully explain gravitational phenomena. Participants highlight the need for a deeper mathematical understanding to grasp these concepts.

Who May Find This Useful

This discussion may be of interest to individuals exploring the foundational concepts of gravity, general relativity, and the philosophical implications of physical theories in the context of physics and mathematics.

AlisonArulia
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Another dumb question, sorry.

I am trying to get my head around if there is some force (Gravity) that acts like an elastic band, pulling everything towards everything else – the more mass a thing has the stronger the elastic band.
Or is it
Gravity doesn’t exist. What happens is that everything bends space/time around it causing everything else to follow the bends formed around. The more mass something the stronger the bends.

Eg. (even though the results are basically the same)
Gravity exists – A snowflake is pulled down downs the Earth and the Earth is pull up toward the snowflake. As the Earth has more mass than the flake, the flake moves more than the Earth does.
Gravity doesn’t exist – Both the Earth and a snowflake bend space/time around themselves. As the Earth has more mass than the flake, the flake follows the bends created by the earth’s mass more then the Earth follows the bends created by the flake.

Either way – Both the flake and Earth are moving and it is not the movement that matters but the acceleration of the flake from one point (relative to another) that is happening rather than movement.

"or" is all of the above wrong :confused:

Please help me to understand this

Thank you

Alison
 
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Sounds like semantics. That's kinda like saying air doesn't exist, it's just molecules of gases floating in three dimensional space.
 
The rubber band analogy should only be used for the strong force.
As for gravity, your arguments for gravity existing/not existing (using the snow flake argument) are both the same. Einstein's theory of relativity says that space-time is curved by matter and the path that the snow flake will take in going from point a to point b is the the shortest distance between the two points constrained to the surface of the curved space-time.
In normal space (i.e. your desk) the shortest distance between two points will be a straight line. Now put your two points on the surface of a trampoline and place a bowling ball between them (but not on the line that connects them!). The trampoline surface is now bent, and the path of the shortest distance between the two points (constrained to the surface of the trampoline!) will look curved. The deviation in the once straight line is what we call gravity.

Gravity is a very hard concept to grasp. It took einstein 11 years to understand, and he's einstein!
 
So - sorry to get this. :-)
There is no direct force - say a force between 2 masses. Just a curve in space time that is created by the masses. All other objects (mass) will follow a streight line - along the curve. This being governed by the size of the mass - the more mass the more curve (force)

Is that right ??

I ask a simler question a while ag ans someone said that (in the snow flake anaolgy) the Earth moves outwards in all directions (towards the flake)

Sorry but I know some people will get this right away but it's taking me a while. How can the surface of the Earth move in all directions at once ? and if it does, is there a need for a curve for the flake to follow - it could just wait for the surface to rise up to meet it OMG
 
I can't answer all of your questions but I remember seeing a particular illustration for gravity (extremely simplified) that may help.

Imagine space as a tightly pulled sheet, on which everything in space lies. The greater the mass of an object, the greater the "dip" it created in the sheet, which causes objects near it to fall in towards it. However, this doesn't account for orbital inertia, among other things. Don't know if that helps, but it helped me.
 
You had best not worry about spacetime "bending" until you get a little further along. General relativity is a very math-intensive subject. No analogy involving snowflakes will ever come close to doing it justice.
 
Tac-Tics said:
You had best not worry about spacetime "bending" until you get a little further along. General relativity is a very math-intensive subject. No analogy involving snowflakes will ever come close to doing it justice.
The math is complicated, but the general idea isn't and can be understood by everyone The rubber sheet analogy is misleading, because it omits the time dimension of space time. Try the visualizations linked here:
https://www.physicsforums.com/showthread.php?p=2244927#post2244927
 
AlisonArulia said:
There is no direct force - say a force between 2 masses. Just a curve in space time that is created by the masses. All other objects (mass) will follow a streight line - along the curve.
Not all other objects. Only the free falling ones follow a straight line in curved space-time. And they don't need to have mass.
AlisonArulia said:
I ask a simler question a while ag ans someone said that (in the snow flake anaolgy) the Earth moves outwards in all directions (towards the flake)
That is nonsense. People are confusing movement and acceleration. The surface of the Earth is accelerated away from the center in the sense that it doesn't follow a straight line in curved space-time, This doesn't mean that it moves away from the center.
 
OMG - this is so much fun. I am learn all the time - 1st to everyone I want to thank you. I am really interested and people like you all make it so easy to understand. I say thank you again to every one, you are so kind to take the time to share your understanding and skill.

2nd - sorry about my english not being good enough to explain I all want. I hope you understand.
 
  • #10
Hi Alison,
I am trying to get my head around if there is some force (Gravity) that acts like an elastic band,...the more mass a thing has the stronger the elastic band.

yes, that small piece of an analogy is ok: just as you stated, but it is NOT good as a broader analogy...
Which has a stronger gravitational attraction, two masses close together, or the same two masses further apart?
They have a STRONGER attraction close together, right?; but that's when an elastic band would be LESS stretched reflecting LESS attraction ...you need an analogy that is strong for short distances and weak for long distances...

But your rubber band analogy does work well for hadron interactions, like quark attraction in a nucleus, where the force of attraction is stronger with greater distance. That's why individual quarks are not found floating around one by one.
 
  • #11
AlisonArulia said:
I ask a simler question a while ag ans someone said that (in the snow flake anaolgy) the Earth moves outwards in all directions (towards the flake)

The Earth had bulged outward because there is more centrifugal force near the equator so it has an orange-like shape.
 
  • #12
Naty1 said:
But your rubber band analogy does work well for hadron interactions, like quark attraction in a nucleus, where the force of attraction is stronger with greater distance. That's why individual quarks are not found floating around one by one.
If attraction increases with distance (let's say proportionally like in Hooke's law) you still have elliptical orbits. But the source of attraction is in center of the ellipse (instead in one of the focal points, like in Newtons inverse square law).

Ironically on the one pound note you see Newton next to a diagram of Hookesian gravity:
http://www.avemaria.edu/uploads/pagesfiles/734.jpg
 
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  • #13
If attraction increases with distance (let's say proportionally like in Hooke's law) you still have elliptical orbits.

I was not decribing anything with elliptical orbits...but now that you mention it:
I'm reminded the force between quarks does not diminish as they are separated...stays steady rather than increase, I think...
a little different than an "elastic" analogy. I think maybe the self repairing string and glueball is a better analogy for nuclear particles covered by QCD: when quarks are separated, say by a large force, the "gluons" forming the string repair to elongate the string and eventually the quarks are pulled back together...
 
  • #14
Gravity does not exist as a force, it is the effect of space-time, or dark matter warping.

I must admit I also find the 2 dimensional rubber sheet a really bad example. I also find this pulling term for gravity also a bad description, as it actually now being understood as a pushing force. I find the over simplistic concept of a ball immersed in a pool of water easier to get my head around, where gravity can be interpreted as the force of the water acting on the outside of the ball. If we then swap say Earth for the ball and dark matter for the water then it becomes clearer what gravity possibly is, and it also goes some way in explaining why we will never find what we could call the "Graviton" particle. This hypothsis also explains why we become lighter the deeper underground we travel, and why we become lighter the further we travel away from Earth. Also don't think of the Moon pulling on the oceans, consider it as sheilding the mass of water from some of the effects of the dark matter and releasing some of the dark matter pressure allowing the water to rise.

Of couse it is far more complex than this as the dark matter, whatever it is is 25% of the missing 96% of the missing universe, the rest currently being assumed as dark energy.

My current studies are in the area of dark matter and why we can only see the effects of it as it holds our galaxy together. Is it simply particles that are out of sync with our galactic time plane? And manifest themselves as neutral particles that we cannot dierectly detect other than the indirect pressure effect of this dark matter quasi-neutral soup that the galactic halo excerts or us? And is it something at the quantum level where particles flit in and out of existence from our galactic plane into other dimentions at various angular planes around our galactic halos sphere?
 
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  • #15
Suppose I made a tunnel right through the earthcore to the other side of the earth, Australia in my case, unfortunately I fall in my tunnel, would this be a correct description of my journey?:

Initially I'd accelerate faster and faster, but as I approach the center, I will slow down and at one point I will stop accelerating since the Earth as a almost spheric shape (a side question, how does a charge in a charged sphere behave, would it move, since there is no potentialdifference?) and the gravitational forces cancel each other out. So the formula with 1/r² only counts as long as I don't fall into the object. Because according to the formula, I would have infinite gravitational force working on me in the core.
At the end of my trip I will be shot in the air, any ways of calculating how high I'd fly?
 
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  • #16
JanClaesen said:
Suppose I made a tunnel right through the earthcore to the other side of the earth, Australia in my case,
Oh really? You must be living in the http://en.wikipedia.org/wiki/File:Antipodes_LAEA.png" then? :wink: In fact your tunnel would work for free fall only along the rotation axis. But let's forget about Earth's rotation and the lava.
JanClaesen said:
Initially I'd accelerate faster and faster,
No, you would accelerate less and less, but still get faster and faster. The force inside a uniform sphere is proportional to r. It is like you were connected with a spring to the center.
JanClaesen said:
but as I approach the center, I will slow down
You would slow down after passing the center with max speed.
JanClaesen said:
and at one point I will stop accelerating
In the center, for a brief moment you are not accelerated by Newtons force. In GR terms you are never accelerated in free fall.
JanClaesen said:
(a side question, how does a charge in a charged sphere behave, would it move, since there is no potentialdifference?)
It would have zero net force.
JanClaesen said:
So the formula with 1/r² only counts as long as I don't fall into the object.
Yes, inside a inform sphere it is a formula with r.
JanClaesen said:
At the end of my trip I will be shot in the air, any ways of calculating how high I'd fly?
The same height you started at the other side (any loses by friction omitted).
 
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  • #17
A.T. said:
Oh really? You must be living in the http://en.wikipedia.org/wiki/File:Antipodes_LAEA.png" then? :wink: In fact your tunnel would work for free fall only along the rotation axis. But let's forget about Earth's rotation and the lava.

No, you would accelerate less and less, but still get faster and faster. The force inside a uniform sphere is proportional to r. It is like you were connected with a spring to the center.

You would slow down after passing the center with max speed.

In the center, for a brief moment you are not accelerated by Newtons force. In GR terms you are never accelerated in free fall.

It would have zero net force.

Yes, inside a inform sphere it is a formula with r.

The same height you started at the other side (any loses by friction omitted).

Ah the middle of the Atlantic, that's funny :biggrin:
Do you have any derivation for the force inside a sphere? I'm wondering right now, if the Earth were an empty sphere, I wouldn't accelarate at all? (just like the potential in an empty, charged sphere is the same in the whole sphere) So the formula you have is for a massive sphere?
 
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  • #18
The r dependence is for a "full" sphere, yes, not a shell. As for a derivation: start with the fact that the gravitational force exerted by a spherical shell on an object outside the shell is
\mathrm{d}F = G \frac{\rho m 4\pi R^2 \mathrm{d}R}{r^2}
Here R is the radius of the shell, \rho is the volume mass density of the shell, and \mathrm{d}R is the shell's thickness. r is the distance from the center of the shell to the object outside the shell and m is the object's mass.

The gravitational force exerted by the shell on anything inside the sphere is 0. You can do an integral to figure this out, or just use a clever argument that patches of the sphere in opposite directions exert forces that cancel each other out. (see http://hyperphysics.phy-astr.gsu.edu/hbase/mechanics/sphshell2.html)

Now to compute the force due to an object partway inside a solid sphere, you divide it up into shells and integrate over only the shells which the object is not inside:
F = \int_0^r G \frac{\rho m 4\pi R^2 \mathrm{d}R}{r^2} = 4\pi \rho m G \frac{r^3 - 0^3}{r^2} = 4\pi \rho m G r
You can see that it's proportional to r.
 
  • #19
shell.. sphere wouldn't it be the same..?

dil
 
  • #20
dylan123 said:
shell.. sphere wouldn't it be the same..?

dil

A sphere is solid; a shell is hollow.

A hollow shell could have a mass approaching zero, depending on how thin the shell it is.
 
  • #21
couldn't a sphere do the same ??
 
  • #22
dylan123 said:
couldn't a sphere do the same ??

No. For a given density and radius, a sphere will have a fixed mass.

For a given density and outer radius, a shell's mass is dependent on the inner radius that bounds the hollow portion.

i.e

mass of a sphere: d x ( 4/3 pi r^3 )
mass of a shell: d x ( 4/3 pi r(outer)^3 minus 4/3 pi r(inner)^3 )

If r(outer) is to equal to 8000.00000 miles, and r(inner) is equal to 7999.99999 miles, then the shell is paper-thin and will weigh almost nothing.
 
  • #23
and if the radius is small..?
 
  • #24
is there a chat room on this site ??
 
  • #25
dylan123 said:
and if the radius is small..?

If the inner radius of a shell is small, its volume and thus mass will approach that of a sphere of the same radius.
 
  • #26
mass approach that of a sphere ? u lost me
 
  • #27
dylan123 said:
mass approach that of a sphere ? u lost me
A shell is a sphere with a hole at the centre.
If a sphere's mass is X, then a shell's mass is going to be X minus the hole at the centre.

If the hole is very small, then the shell is pretty much a solid sphere.
If the hole is very large, then the shell is pretty much a hollow sphere.

If the hole is extremely small, then you're basically got a sphere with no hole. The shell will have the same mass as a sphere of the same size.

If the hole is so large that it is just slightly smaller than the sphere itself, then you've basically got a very thin-walled, empty shell. It could be so thin that its entire mass could be next to nothing.
 
  • #28
so what happins inside this shell , this next to nothing shell?
 
  • #29
dylan123 said:
so what happins inside this shell , this next to nothing shell?
If Earth were hollow (and magically did not collapse in on itself), anywhere inside the hollow area would have zero gravity. You could be in the very centre or you could be hugging the inner wall. Either place, or anywhere in between, you would float weightless.
 
  • #30
i thought the shell was thin
 

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