Exploring Gravity: Does It Exist?

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In summary, the rubber band analogy should only be used for the strong force. 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.
  • #1
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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  • #2
Sounds like semantics. That's kinda like saying air doesn't exist, it's just molecules of gases floating in three dimensional space.
 
  • #3
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!
 
  • #4
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
 
  • #5
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.
 
  • #6
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.
 
  • #7
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
 
  • #8
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.
 
  • #9
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
[tex]\mathrm{d}F = G \frac{\rho m 4\pi R^2 \mathrm{d}R}{r^2}[/tex]
Here R is the radius of the shell, [itex]\rho[/itex] is the volume mass density of the shell, and [itex]\mathrm{d}R[/itex] 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:
[tex]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[/tex]
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
 
  • #31
No I think you would slow down slightly as you go through the crust and eventually you would burst into flames. No seriously, if you could do this initial innertia and then centifugal force would either try to throw back out the hole you entered, and you would go up and down like a piston in a cylinder, or of if you passed through the core with the inertia you would probably barely make it outside of the boundary of the molten iron core. It is really a question of balance between gravity and centrifugal inertia.
 
  • #32
dylan123 said:
i thought the shell was thin

It is as thick or as thin as you define. If your sphere is 4000 miles in radius, about the size of the Earth it could be a shell of:
- 3900 mile thickness, leaving an interior hollow space a mere 100 miles in radius.
of the Earth
- 1 mile thickness, leaving an interior hollow space 3999 miles in radius.
- 1 inch thickness, leaving an interior hollow space 3999 miles 5279' 11" in radius.

These things don't actually exist, the point of this thread is: what is the gravity at the centre of the Earth? Or, if the Earth were hollow, what would the gravity be like inside? Any question like this can be answered by studying the general principle, which is known as Newton's Shell Theory.
 
  • #33
Guesser7 said:
No I think you would slow down slightly as you go through the crust and eventually you would burst into flames. No seriously, if you could do this initial innertia and then centifugal force would either try to throw back out the hole you entered, and you would go up and down like a piston in a cylinder, or of if you passed through the core with the inertia you would probably barely make it outside of the boundary of the molten iron core. It is really a question of balance between gravity and centrifugal inertia.

Assuming there were nothing blocking your path, you would fall to the centre of the Earth and continue past it, rising right back up to the surface. You would just intersect the surface of the Earth at the peak of your arc before plunging back down again. The time for one complete passage back to your starting point would be about 90 minutes - not coincidentally, that is exactly the same length of time it takes to orbit the planet if you could do it at zero altitiude.
 

1. What is gravity?

Gravity is a natural phenomenon by which all objects with mass are brought towards one another. It is responsible for the motion of planets, stars, and galaxies in the universe.

2. How does gravity work?

Gravity is caused by the curvature of space and time by massive objects. The more massive an object is, the more it curves the space and time around it, causing other objects to be pulled towards it.

3. Is gravity the same everywhere in the universe?

No, gravity is not the same everywhere in the universe. Its strength depends on the mass and distance between objects. The larger the mass and closer the distance, the stronger the gravitational force.

4. How was gravity discovered?

The concept of gravity was first proposed by Sir Isaac Newton in the 17th century. He observed that objects fall towards the ground and developed the theory of gravity to explain this phenomenon.

5. Can gravity be manipulated or controlled?

As of now, there is no known way to manipulate or control gravity. However, scientists are constantly researching and exploring ways to harness the power of gravity for space travel and other applications.

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