lugita15
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GM/Sqrt r wouldn't even be the right units!Mueiz said:Firstly in(3) is incorrect it should be GM/Sqrt r rather than GM/r
The discussion centers on the relationship between Poisson's Equation and Einstein's Field Equations (EFE), specifically how Poisson's Equation serves as a model for deriving EFE in the Newtonian limit. Participants clarify that while EFE is not derived from Poisson's Equation, it can be inspired by it, particularly in the context of gravitational fields. The conversation also highlights the differences in how density is treated in both equations, emphasizing that Poisson's Equation incorporates mass density in a volume context, while EFE considers local density at a point. Key references include Einstein's "The Meaning of Relativity" and various Wikipedia pages on Gauss's Law and Electrostatics.
PREREQUISITESPhysicists, mathematicians, and students of theoretical physics interested in the foundations of gravitational theory, particularly those exploring the connections between classical and modern gravitational equations.
GM/Sqrt r wouldn't even be the right units!Mueiz said:Firstly in(3) is incorrect it should be GM/Sqrt r rather than GM/r
No, you would get -3GM-0-0+3GM=0.Mueiz said:But no problem that is easy suppose we want to apply it in the pont (1,0,0) which is outside the source;
Then we have out(5)=-3GM-3GM-3GM+3GM=-6GM not equal 0
lugita15 said:GM/Sqrt r wouldn't even be the right units!
Gravitational field is inversely proportional to r^2. Gravitational potential is inversely proportional to r.Mueiz said:We want to calculate the lablacian of what?
of the gravitational field
How gravitational field is measured ?
GM/Sqrt r
lugita15 said:Gravitational field is inversely proportional to r^2. Gravitational potential is inversely proportional to r.
No, that's wrong. See this link.Mueiz said:Poission Equation is conserned with the Lablacian of gravitational field and not the potential see any textbook about poission equation
your calculation here is correct according to the incorrect form of Mr Dalelugita15 said:No, you would get -3GM-0-0+3GM=0.
What do you think the correct form is?Mueiz said:your calculation here is correct according to the incorrect form of Mr Dale
but not according to the correct form
lugita15 said:No, that's wrong. See this link.
It's quite simple. You solve Poisson's Equation to get the gravitational potential, then you take the gradient to get the gravitational field.Mueiz said:your link of wikipeadia says;
"This provides an alternate means of calculating the gravitational potential and gravitational field. "
which one to chose ?
-GM/r is correct:Mueiz said:Firstly in(3) is incorrect it should be GM/Sqrt r rather than GM/r
Obviously not. It is output. It is the Laplacian of the potential in Cartesian coordinates. It is undefined for x=y=z=0 and it simplifies to 0 for all other points.Mueiz said:Secondly what is the result of out(5)? you did not write it !
It does equal zero. Check your arithmetic.Mueiz said:But no problem that is easy suppose we want to apply it in the pont (1,0,0) which is outside the source;
Then we have out(5)=-3GM-3GM-3GM+3GM=-6GM not equal 0
-6GM equal 4 *pi *G *Density as I said
4* pi *G *density=-4 pi G M/(4/3 pi *1)=-6GM
Not only do you need to learn some basic differential equations, but you need to learn how to do simple algebraic substitution.Mueiz said:I will not say you need to learn some basic DE but I think you just did a mistake.
This doesn't even make any sense. The density is a scalar field, it cannot possibly be proportional to the Laplacian of a vector field. See a little further down in the link I originally posted.Mueiz said:Poission Equation is conserned with the Lablacian of gravitational field and not the potential see any textbook about poission equation
lugita15 said:What do you think the correct form is?
DaleSpam said:This doesn't even make any sense. The density is a scalar field, it cannot possibly be proportional to the Laplacian of a vector field. See a little further down in the link I originally posted.
http://en.wikipedia.org/wiki/Gauss'...vitational_potential_and_Poisson.27s_equation
Huh?Mueiz said:I mean the second derivative of poisson equation not Lablacian (this was a mistake)
The only thing that is equal to 4piGM is the flux of a gravitational field through a closed surface, in which case M is the mass enclosed by the surface. But the flux of the gravitational field involves a double integral (a surface integral to be precise), not a second derivative.Mueiz said:what is equal to 4*pi*G*M is the second dervative of gravitational field and not Lablacian of the potential
Mueiz said:We want to calculate the lablacian of what?
of the gravitational field
How gravitational field is measured ?
GM/Sqrt r
Well, the vector Laplacian of the gravitational field (one possible meaning of "the second d") is in fact 0 outside a point mass. However, since there are three dimensions there are an infinite number of possible second derivatives of the gravitational field. I don't know which one you are specifically referring to as "the second d", but you are correct that many of the possible second derivatives (besides the Laplacian) may be non-zero in vacuum.Mueiz said:The second d of gravitational field does not equal zero outside
For a point mass, yes. What is the density of a point mass?Mueiz said:The lablacian of the potential equals zero outside and undefined at the origin
Why don't you answer this question yourself by doing the following exercise. Start with the known expression for the gravitational potential inside a solid uniform spherical mass (i.e. a solid ball, not a hollow shell) of unit density (http://en.wikipedia.org/wiki/Gravitational_potential#Spherical_symmetry), take the Laplacian of that expression and see what you get. And yes, I can do this exercise but then how will you learn.Mueiz said:If poission equation relates Lablacian of Potential which is always zero why not just write it ; L(potential of GF)=zero ?
I don't know how you come up with any of this. This whole paragraph is simply incorrect. Please do the exercise above to see for yourself.Mueiz said:the only thing it say is that; outside the source
the lablacian of the potential equals zero and it cannot be applied in the presence of matter ,(in both cases there is no method to characterize the differences in gravitational properties and relate it quantitatively to matterial properties
I can't make sense of a lot of what you're saying, but I think you have one major misunderstanding about Poisson's equation which is leading to a lot of smaller confusions. It is true that for each point where there is no matter, Poisson's equation simply states that the Laplacian of the potential is zero. But the mere fact that the Laplacian is zero is not sufficient information to determine what the value of the potential is at that point, because there are an infinite number of possible functions whose Laplacian is zero. So you require some additional information, known as boundary conditions, to solve Laplace's equation (which is just Poisson's equation with the right hand side equal to zero). The boundary conditions are in the form of the distribution of mass throughout space; in other words you need to specify density as a function of position. Once you know the mass distribution, then you have sufficient information to solve the potential, because there is a theorem that says that there exists a unique solution to Laplace's equation for each set of boundary conditions.Mueiz said:The second d of gravitational field does not equal zero outside
The lablacian of the potential equals zero outside and undefined at the origin
If poission equation relates Lablacian of Potential which is always zero why not just write it ; L(potential of GF)=zero ?
also if poisson equation relates lablacian of the potential to the quantity 4*pi*G*dinsity (as you all claim) it can not be used as a model to find the constant "4PiG'' in EFEbecause Poission equation -as you understand it -can not relate the density of matter in a point to the properties of gravitational field in the absence of matter . the only thing it say is that; outside the source
the lablacian of the potential equals zero and it cannot be applied in the presence of matter ,(in both cases there is no method to characterize the differences in gravitational properties and relate it quantitatively to matterial properties While in EFE both in the presence and absense of matter in a point there exist a method to characterize gravitational field
(reply this question and leave my mistake in previous posts of using the word "lablacian of gravitational field'' instead of "second d of gravitational field dg/dr, g=dr/dt '')
I made this point back in post 15 (https://www.physicsforums.com/showpost.php?p=3086463&postcount=15) but hopefully he will pay attention now that more than one person is saying the same thing. Although, I am not placing any bets on itlugita15 said:The bottom line is that even though the Laplacian of the potential at a point of empty space is always zero, still the potential itself can and does depend on the magnitude and distribution of the surrounding matter.
Well, I guess it bears repeating.DaleSpam said:I made this point back in post 15 (https://www.physicsforums.com/showpost.php?p=3086463&postcount=15) but hopefully he will pay attention now that more than one person is saying the same thing. Although, I am not placing any bets on it![]()
Are you blind?Mueiz said:2\ I disagree that the left hand side of poisson equation is the Lablacian of the Potential
3\ I claim that the left hand side of poisson equation is dg/dr
DaleSpam said:Are you blind?
Apparently not given the number of links to Poisson's equations that you didn't see even after we put them in front of you.Mueiz said:I see what is in front of me
I was responding to your erroneous claims 2 and 3 regarding Poisson's equation, which is clearly defined in those links and in any textbook on the subject. We need to clear those up and you need to post the results of the exercise before going on to claim 4. The left hand side of Poisson's equation is clearly the Laplacian of the potential. If you cannot even understand that with so much evidence provided then any further discussion is pointless.Mueiz said:None of these Pages contain a proof that Lablacian(GM/r)=4*pi*G*density
Excellent copying and pasting, but that wasn't the exercise. The exercise was to find the Laplacian of the potential inside a spherical mass, not outside. The potential inside a spherical mass is not -((G M)/r). See the link which I gave above in post 51:Mueiz said:Everyone -even the blind - can see that Laplacian[-((G M)/r)] =0