Newtonian gravitation as a vector

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Discussion Overview

The discussion revolves around the vector representation of Newtonian gravitation, specifically how to express gravitational force as a vector in a three-dimensional space. Participants explore the mathematical formulation of gravitational force, its components, and the implications of using a vector field calculator.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about the directionality of vectors in a gravitational field, noting that they only seem to point in two directions.
  • Another participant provides the vector equation for Newtonian gravitation and asks for clarification on the original question.
  • There is a discussion about expressing the gravitational force in component form using unit vectors (i, j, k) and how to derive these components from the position vector.
  • One participant mentions using an online vector field calculator to visualize the gravitational force but finds discrepancies in the expected output.
  • Another participant suggests simplifying the problem to two dimensions to better understand the vector field representation.
  • There is a correction regarding the exponent in the gravitational force equation, with a participant asserting that the force should be expressed as inversely proportional to the square of the distance.
  • Participants discuss the mathematical derivation of the gravitational force components in both two and three dimensions, with some expressing uncertainty about the necessary mathematical background.
  • One participant seeks clarification on the derivation of the gravitational force components and how they would change in three-dimensional space.
  • A later reply attempts to clarify the derivation of the gravitational force vector, emphasizing the importance of understanding exponent rules.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the correct representation of the gravitational force vector, with multiple competing views on the mathematical formulation and the use of the vector field calculator. Some participants correct or refine earlier claims without establishing a definitive agreement.

Contextual Notes

There are limitations in the discussion regarding assumptions about the gravitational constant and the specific conditions under which the gravitational force is calculated. Participants also express varying levels of mathematical understanding, which may affect their interpretations of the equations.

Who May Find This Useful

This discussion may be useful for students and enthusiasts of physics and mathematics who are exploring the concepts of gravitational force, vector fields, and the mathematical representations of physical laws.

Isaac0427
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Hi guys! So I am a little congused about Newtonian gravitation. I understand the equation to get a scalar for the strength of gravity, but when I plugged it into a vector field calculator (with random values of m and M), all the vectors only pointed in one way. I do understand that r-hat could be positive 1 or negative 1 depending where m and M are, but still, the arrows can only go in 2 directions. I'm not sure if this is a stupid question, but I am a little confused.
 
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What exactly is your question ?
 
The vector equation for Newtonian gravitation reads:
\vec{F}_1 = \frac{G m_1 m_2}{|\vec{r}_{12}|^3} \vec{r}_{12}

That is, the force on particle one (in a system of 1 and 2) is directed along the vector connecting it to the second particle (\vec{r}_{12}). Given that, what exactly don't you understand?
 
Nabeshin said:
The vector equation for Newtonian gravitation reads:
\vec{F}_1 = \frac{G m_1 m_2}{|\vec{r}_{12}|^3} \vec{r}_{12}

That is, the force on particle one (in a system of 1 and 2) is directed along the vector connecting it to the second particle (\vec{r}_{12}). Given that, what exactly don't you understand?
So what would that be in the form of F(x,y,z)= F(x)i+F(y)j+F(z)k (or however you write it) using any random values of m and M. I am actually only 13 and I have only self tought myself some calculus (and I have watched videos), so I may be missing something in my math, but don't you need that kind of equation to get vector (x,y,z)?
 
Isaac0427 said:
So what would that be in the form of F(x,y,z)= F(x)i+F(y)j+F(z)k (or however you write it) using any random values of m and M. I am actually only 13 and I have only self tought myself some calculus (and I have watched videos), so I may be missing something in my math, but don't you need that kind of equation to get vector (x,y,z)?

The vector in my equation \vec{r}_{12} = ( x_2 - x_1 , y_2 - y_1, z_2 - z_1 ) written out in component form. Similarly the vector \vec{F} = (F_x,F_y, F_z ). Each component of the left hand side and right hand side are equal, which gives you your three equations. Does that make sense? Can you see how you might write that out in terms of your seemingly preferred i,j,k notation?
 
Nabeshin said:
The vector in my equation \vec{r}_{12} = ( x_2 - x_1 , y_2 - y_1, z_2 - z_1 ) written out in component form. Similarly the vector \vec{F} = (F_x,F_y, F_z ). Each component of the left hand side and right hand side are equal, which gives you your three equations. Does that make sense? Can you see how you might write that out in terms of your seemingly preferred i,j,k notation?
I do understand that, however as I pug it into a vector field calculator the vector for the point which m is at does not necessarily point towards M (0,0,0).
 
Isaac0427 said:
I do understand that, however as I pug it into a vector field calculator the vector for the point which m is at does not necessarily point towards M (0,0,0).
What exactly is a "vector field calculator" and what exactly are you pugging into it?
 
jbriggs444 said:
What exactly is a "vector field calculator" and what exactly are you pugging into it?
I plugged in Newtonian gravitation into an online vector field graphing calculator.
 
It is easiest to work in 2 dimensions and set ## m_2 ## at (0,0) so that the position vector of m_1 is ## \vec r = (x,y) ## and ## \vec r_{12} = - \vec r ##. You should then be able to get a 2D vector field plot that looks something like this. I'm not sure that helps you much though, or does it?
 
  • #10
MrAnchovy said:
It is easiest to work in 2 dimensions and set ## m_2 ## at (0,0) so that the position vector of m_1 is ## \vec r = (x,y) ## and ## \vec r_{12} = - \vec r ##. You should then be able to get a 2D vector field plot that looks something like this. I'm not sure that helps you much though, or does it?
That is what I did, however the equation you used was not Newtonian gravitation. When I plugged in Newtonian gravitation on that site (using random masses) that is not what it looked like.
 
  • #11
I think you will find that it was (I assumed ## Gm_1m_2 = 1 ## as all that affects is the scale of the arrows). What do you think I got wrong?
 
  • #12
MrAnchovy said:
I think you will find that it was (I assumed ## Gm_1m_2 = 1 ## as all that affects is the scale of the arrows). What do you think I got wrong?
Then it would be 1/(x^2+y^2), and it would not be to the 1.5th power.
 
  • #13
Isaac0427 said:
Then it would be 1/(x^2+y^2), and it would not be to the 1.5th power.

the magnitude of the gravitational force is 1/r^2 = 1/(x^2 + y^2). but the x and y components are
- x/r^3 = -x (x^2 + y^2)^(3/2) and -y/r^3 = -y (x^2 + y^2)^(3/2)
 
  • #14
willem2 said:
the magnitude of the gravitational force is 1/r^2 = 1/(x^2 + y^2). but the x and y components are
- x/r^3 = -x (x^2 + y^2)^(3/2) and -y/r^3 = -y (x^2 + y^2)^(3/2)
Could you show me the math behind that? If say GMm was 2 would it be -2x/r^3i-2y/r^3j? I think I see what the rule is for this. One final question: how would the formulas for each axis change in 3 dimensional space?
 
  • #15
Isaac0427 said:
Then it would be 1/(x^2+y^2), and it would not be to the 1.5th power.

No, note that the magnitude of the gravitational force is ## \frac{Gm_1m_2}{\lvert \vec r \rvert ^2} ## and the unit vector of its direction is ## \hat r = \frac{\vec r}{\lvert \vec r \rvert} ##, so we get
Nabeshin said:
\vec{F}_1 = \frac{G m_1 m_2}{|\vec{r}|^2} \hat{r} = \frac{G m_1 m_2}{|\vec{r}|^3} \vec{r}
To get from this to ## Gm_1m_2(x^2 + y^2)^{-3/2} ## you need to know more about working with exponents in expressions like ## x^{-3} ## and ## \sqrt x = x^{(1/2)} ## than I did when I was 13, have you covered this in your studies yet?
 
  • #16
MrAnchovy said:
No, note that the magnitude of the gravitational force is ## \frac{Gm_1m_2}{\lvert \vec r \rvert ^2} ## and the unit vector of its direction is ## \hat r = \frac{\vec r}{\lvert \vec r \rvert} ##, so we get

To get from this to ## Gm_1m_2(x^2 + y^2)^{-3/2} ## you need to know more about working with exponents in expressions like ## x^{-3} ## and ## \sqrt x = x^{(1/2)} ## than I did when I was 13, have you covered this in your studies yet?
Yes, I am actually 3 grades ahead in math besides my personal studies, and I was confused because I didn't know about r^3.
 
  • #17
Hmmm, I'd like to post a small correction and make the derivation clearer:

$$ \vec{F} = -G \frac{m_1m_2}{|\vec{r}|^2} \hat r = -G \frac{m_1m_2}{|\vec{r}|^2} \frac{\vec r}{\lvert \vec r \rvert} = -G \frac{m_1m_2}{|\vec{r}|^3} \vec{r} $$
 

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