## Can you make an object have a stronger graviational pull if you make is denser?

If I have 2 objects with equivalent mass. Is there anyway I can make one of them have a stronger pull by changing the density? If so are there any equations the help me predict to what extent?

Thanks.
 Sort of. Gravitational force is dependent on mass and distance. If the object is smaller, that means you can reduce the distance. Consider: here on Earth, you feel gravity at 1g. That is because of exactly two factors: - the mass of the Earth is 5x10^23g - your distance from the Earth's centre of mass is ~6200km This is the best you can do as far as G-pull goes. But if Earth were crushed down 1/10th of its current diameter, that means you could get ten times closer to its CoM. And that means you would experience a pull of 10^2 or 100gs. As for formulae, simply use F=G*m/r^2 where m is the mass of your object and r is its radius - or more relevantly, the minimum distance you can get from the centre of mass of the object. You will find that, for your smaller object, r can be smaller, therefore F will be larger.

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 Quote by zeromodz If I have 2 objects with equivalent mass. Is there anyway I can make one of them have a stronger pull by changing the density? If so are there any equations the help me predict to what extent? Thanks.
Loosely speaking, no. The gravitational attraction would be the same between the two.

For example, if the sun were to mysteriously collapse into a black hole (without some big supernova explosion that would tear the Earth apart), the Earth would orbit around around this black hole, just as it did the sun. A Year would still be a year. Gravitationally speaking, we wouldn't see a difference here on Earth (sunlight would be a different story though )

As a more mundane example, consider a dry sponge and a piece of duct-tape. Place both on a scale and measure their combined weight. Now, using the same strip of duct-tape, tightly wrap up the sponge so that its volume decreases. Again weigh the sponge-tape combination. The results are the same. The density increased, but the weight, i.e. gravitational attraction, didn't.

Now if the Earth's volume shrunk down to a much smaller size, you would feel a greater gravitational attraction on its new surface, only because you are now closer to the center of the Earth. But if you were to stand on a platform ≈6371 km (≈3,959 mi) away from the center of the Earth (just as you are now with its current radius), you weight would remain the same as it is now (in both cases you are the same distance from the Earth's center).

Notice I started this response with the phrase "loosely speaking." Getting more technical, the gravitational attraction and gravitational effects are only independent of density if the objects are rigid bodies and the mass distribution of each have spherical symmetry. But even so, it wouldn't matter much. But it can have a non-negligible impact if the objects are close together depending on how you change the orientation of one or both objects. This situation is responsible for ocean tides on Earth. (If the Earth were shrunk down to size of a basketball, there would be no more tides ... of course that would be the least of Earth's problems if that happened. ) In a similar vein, a neutron star in a close orbit to a large red giant companion could cause the neutron star accrete matter, "taken" from its companion, which wouldn't happen if the companion star was more compact.

## Can you make an object have a stronger graviational pull if you make is denser?

 Quote by collinsmark Lots of interesting, well written things
So in other words - No. Unless you are changing the density by adding mass with equivalent volume.

Though you may be able to double the gravitational pull of an object, it won't have much effect in real world... The earth is still going to hold the ball to the ground and friction isn't going to let it go much of anywhere. In deep space however, sure this is theoretically possible:

Force from Gravity = G*(mass of object 1)*(mass of object 2)/(distance between them)^2

where G = 6.67x10^(-11) m^3/(kg*s^2)
masses are in Kg
and distance is in meters
 Not being a physicist myself I got lost in the technical mumbo-jumbo. So what was the upshot? That the denser object has a more intense gravitational field immediately around it but from a significant distance they would have the same gravitational pull?

 Quote by slipperyfish Not being a physicist myself I got lost in the technical mumbo-jumbo. So what was the upshot? That the denser object has a more intense gravitational field immediately around it but from a significant distance they would have the same gravitational pull?
Yes.

Earth is ~3900 miles in radius and masses 6x10^24kg.
Imagine a very dense object X, only 1 mile in radius, yet massing 6x10^24kg.

On Earth's surface, 3900 miles from its center, we experience 1g.
If we were in a spaceship 3900 miles from object X, we would experience 1g.

Note that the Earth's surface is the closest we can get to Earth, so it does not exceed 1g.
However, we could fly closer to object X. If we flew to half that distance (1950 miles) we would now experience 2gs. If we flew to within 30 miles of object X (7 halvings) we would experience 128gs (2^7).
The surface gravity on object X (.5mi radius) is 4096gs.
 This is a very interesting subject. I woke up tonight (as I'm wont to do) with Einstein's (Was it his?) thought experiment about bowling balls and marbles on a trampolene surface to show the bending of space-time. I may have taken the analogy a little far, but I suddenly have a problem...I imagined the experiment with a somewhat more elastic surface (perhaps). If we have a marble, say, that has a very high mass, but a small radius (some super dense material) this would cause a deep curve with a small radius - where as a beach ball would produce a shallow dent with a wide radius. For the two to be attracted, then the event horizons of the two curves need to come into contact with each other. So this leads to several questions (that woke me up): 1-Is gravity, being a curvature of space-time as opposed to Newtonian force, of equal density itself or does size affect the curvature as well as mass? 2- Is the flexability of the "surface" (space-time) constant thoughout the universe or is it more apt to curve in some places tha others? 3- Is the "flexability" such that what I suggested (in my apparant dream) impossible in our universe. 4- Is it possible for a super dense object to bend space-time completely around itself - would we know? Maybe this would just be its own little universe/dimension???
 Recognitions: Gold Member Wolf, the curvature of space due to gravity of an object is only different if you compare two equally massive objects but not of equal density. Take your marble and beach ball for example. Lets say your marble is 1 in across and the beach ball is 10 in across. If both have the same mass then both have equal curvature at a distance from the center of mass of about 10 in and greater. Once you get INSIDE the surface of the beach ball the gravity is no longer centered at the center of mass. The closer you get to the center the more gravity is pulling "out" instead of "in", since all the matter is no longer on one side of you and is instead surrounding you. In effect you have less gravity per space than the marble does. The marble, being much smaller and denser, still has all its mass on one side of you, therefore all the gravity is concentrated as well. So once you get closer to the marble than 10 in, you start to experience more gravity than you did with the beach ball. So, like people said above, replacing the sun with a black hole of equal mass would have almost no difference in the overall gravity of the solar system EXCEPT if you got closer to the black hole than the surface of the sun is to it's center. Make sense?

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Hello Wolf5370,

Welcome to Physics Forums!
 Quote by Wolf5370 This is a very interesting subject. I woke up tonight (as I'm wont to do) with Einstein's (Was it his?) thought experiment about bowling balls and marbles on a trampolene surface to show the bending of space-time. I may have taken the analogy a little far, but I suddenly have a problem...I imagined the experiment with a somewhat more elastic surface (perhaps). If we have a marble, say, that has a very high mass, but a small radius (some super dense material) this would cause a deep curve with a small radius - where as a beach ball would produce a shallow dent with a wide radius. For the two to be attracted, then the event horizons of the two curves need to come into contact with each other.
I wouldn't use the term "event horizon" in your analogy. Event horizon has a very specific meaning, and I don't think it necessarily applies to your beach ball and marble analogy.

But anyway, let's continue with your analogy of the marble and beach-ball on the metaphorical elastic surface.

Imagine that you had a very dense marble and a less dense beach-ball, such that both the marble and beach-ball have the same mass. Also, let's assume that both are perfectly spherical and nothing is rotating.

When the beach-ball is put on the metaphorical surface, it will cause a dent in the surface. The slope (related to curvature) of the dent gradually becomes less as the distance away from the ball increases.

Now put the dense marble on the surface. Near the region of the marble, the slope (curvature) is much, much greater than that region directly under the beach-ball. However, like the case with the beach-ball, as you get further away from the marble, the slope (curvature) decreases.

Now here is the kicker: At a distance greater than or equal to the radius of the beach-ball, the slope (curvature) of each situation is identical. True, the situations differ at distances less than the radius of the beach-ball (namely the marble situation has steeper curvature), but at distances greater than or equal to the radius of the beach-ball, there is no difference at all.
 So this leads to several questions (that woke me up): 1-Is gravity, being a curvature of space-time as opposed to Newtonian force, of equal density itself or does size affect the curvature as well as mass?
Umm, I'm not quite sure I follow you here. But I'll take a stab at it anyway. Mass/energy (mass is really just one of several forms of energy) tells spacetime how to curve (how to shape itself). Spacetime curvature tells mass how to move.

The differences between a beach-ball and a marble is the mass distribution. But if you wanted to, you could break up the marble and/or beach-ball into a vast number of tiny, tiny bits of mass (such that each tiny chunk of mass has the same mass as any other tiny chunck). Then each tiny chuck of mass would have the same influence on spacetime curvature as any other tiny chunk of mass. The only difference now in the beach-ball and marble situations is where all the little bits of mass are relative to each other.*

*Technically, if there is any energy binding the pieces of mass together, you'll have to take that into consideration too. But that's pretty negligible on scales greater than atomic nuclei. So let's just assume that we're not ripping atoms apart.
 2- Is the flexability of the "surface" (space-time) constant thoughout the universe or is it more apt to curve in some places tha others?
It is a principle that laws of gravitation are the same everywhere in the universe (all else being the same except for position). This is just a principle though. Presently, there is no evidence that would indicate that it isn't true.
 3- Is the "flexability" such that what I suggested (in my apparant dream) impossible in our universe.
I don't think I understand the question.
 4- Is it possible for a super dense object to bend space-time completely around itself - would we know? Maybe this would just be its own little universe/dimension???
If an object is dense enough, a black-hole will form. Using the analogy of balls on a surface, the dense object would create an incredibly large curvature, near the object. In relativistic terms, the curvature would be large enough, at some close enough distance to the object, that nothing could escape once closer than that distance. This threshold is called the event horizon.

But an important point here is that as you get farther away from the object, the curvature is just like it would be if the object was bigger and less dense.

Imagine that the entire Earth was compressed to the size of a beach-ball. However, also imagine that you were suspended by some sort of platform with a height of exactly the radius of what the Earth is now. In other words, the Earth gets squished to beach-ball size, but you stay put (and don't fall toward the center along with it) due to the platform. From your vantage point up on the platform, gravity is exactly the same as it was before. You would measure g = 9.81 m s-2. You could jump as high as you used to, no more, no less. The moon would continue orbiting the squished up Earth, pretty-much just as it did before the Earth was squished.*

The difference would come into play if you were to climb down the platform toward the newly squished up Earth. Gravitational pull would be much greater the closer you get. If you were to get close enough, the tidal forces would turn you into spaghetti (i.e. you would be spaghettified).

*In this paragraph I'm ignoring certain minor differences that arise from the Earth not being perfectly spherical, rotation, etc.

 Quote by Wolf5370 PS: I knew Event Horizon was specific to black holes, but at 4am here, it seemed as good a descriptor as any even in incorrectly applied - I guessed (correctly) that you would get my gist. Threshold would have been a better term to use - or distance of influence perhaps. :D
There is no threshold. Distance of influence is infinite. There is no distance so far from any mass that spacetime is not curved by it.

This is one of the dangers of using analogies, such as trampolines, to extrapolate.
 No. Gravitational pull is governed by mass, not density. Earth is far more dense than Jupiter. But Jupiter's greater mass makes its gravitational pull much stronger.

 Quote by DaveC426913 There is no threshold. Distance of influence is infinite. There is no distance so far from any mass that spacetime is not curved by it.
Dave, does this mean that if I wiggle my little finger, I wiggle the entire universe (well, a little, anyway)?

 Quote by Oldfart Dave, does this mean that if I wiggle my little finger, I wiggle the entire universe (well, a little, anyway)?
It means that the influence of the gravity of your finger is non 0 at the limit of infinity or the size of the universe or whatever you want to call it yeah. there is no such thing as nothing in field theory, well there is but you get the point.

You wiggle the universe an extremely small amount, and it wiggles you.
 How about this. A star with higher gravitational pull will cause time to pass more quickly. This increase in time flow *is* gravity.

 Quote by ScottTheSculp How about this. A star with higher gravitational pull will cause time to pass more quickly. This increase in time flow *is* gravity.
That's interesting. I guess it's in line with how jets at high altitude (hence, further from the earth) will lose a second or so on their clock.

Just thinking out loud here, I could be off my rocker, but I wonder if that means that time may come to a stop altogether for an object drifting alone in deep space, far from any gravitational pull. Could this cause astronauts aboard a spacecraft to successfully make the 20 light-year voyage to Gliese 581g (the recently discovered earth-like exoplanet) without aging? And therefore return to earth still alive? Albeit long after their loved ones here had all passed away.

Shoot, but it would suck for them if during their voyage, which could be a few centuries on earth, we came up with a faster way to travel, and we passed them!
 Yep. To leave the solar system you would be pulling away from the time stream of your star and moving directly against it. You will age quite quickly. If you head directly at the star there is no time . . .but the end is near. The time stream is moving passed us at the "speed of light". Not messing with you. I have a theory ;-)