What is the magnitude of the net gravitational force

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SUMMARY

The net gravitational force acting on a third sphere with a mass of 0.490 kg, placed at the point (4,0), due to two other spheres with masses of 65 kg and 79 kg, was calculated using the formula F_{g} = \frac{GMm}{r^{2}} with G = 6.67 × 10^{-11}. The initial calculation yielded an incorrect net force of 3.48 N, which was later corrected to 2.24 × 10^{5} N after addressing errors in angle determination and unit conversion. Additionally, the discussion explored the placement of the third sphere at (0,1.43) where the net gravitational force would equal zero.

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  • Understanding of Newton's Law of Universal Gravitation
  • Familiarity with gravitational constant G = 6.67 × 10^{-11} N(m/kg)²
  • Knowledge of trigonometric functions, specifically sine and cosine
  • Ability to solve quadratic equations
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  • Review gravitational force calculations using F_{g} = \frac{GMm}{r^{2}}
  • Learn about gravitational equilibrium and conditions for net forces to equal zero
  • Study the application of trigonometric functions in physics problems
  • Explore the implications of gravitational force in multi-body systems
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Students in physics, particularly those studying gravitation, as well as educators and anyone interested in solving gravitational force problems in a multi-body context.

QuarkCharmer
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Gravitation Force (Solved, thanks)

Homework Statement


A sphere with mass of 65kg and center at origin. Another sphere with mass 79kg at point (0,3), also centered at origin.

A.) What is the magnitude of the net gravitational force due to these objects on a third uniform sphere with mass 0.490 kg placed at the point (4,0)

Homework Equations


F_{g} = \frac{GMm}{r^{2}}
G = 6.67(10^{-11})


The Attempt at a Solution


I made this image to help:
j91o3k.jpg


Force from the 79kg sphere:
FG_{1}=\frac{G(.490)(79)}{5^{2}}

Force from the 65kg sphere
FG_{2}=\frac{G(.490)(65)}{4^{2}}

So the net force on the .490 kg sphere is given by:
\sqrt{(FG_{2} + FG_{1}cos(tan^{-1}(\frac{3}{4})))^{2}+(FG_{1}sin(tan^{-1}(\frac{3}{4})))^{2}}

I get the net force on the 0.490 kg sphere to be 3.48 N. Which is incorrect? I don't know what is wrong.
 
Last edited:
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What did you use for G?

You can find the cosine and sine of the angle at the 0.49 kg mass directly from the right triangle.

ehild
 
ehild said:
What did you use for G?

You can find the cosine and sine of the angle at the 0.49 kg mass directly from the right triangle.

ehild

I used 6.67 * 10^-11 for G.

What do you mean about the cos/sin ? arctan(3/4) is the angle near the .490kg sphere, so the equation should hold?
 
QuarkCharmer said:
I used 6.67 * 10^-11 for G.

What do you mean about the cos/sin ? arctan(3/4) is the angle near the .490kg sphere, so the equation should hold?

The sine of the angle is opposite/hypotenuse=3/5. The cosine is adjacent/hypotenuse=4/5. Is not that simpler than taking the cosine and sine of arctan(3/4)? It is not wrong, just strange.

Check your calculation. I think you forgot the 10^-11.

ehild
 
You are correct. I don't know why I was thinking that I needed to determine the angle via inverse trig.

I did the computations over and somehow it came out correct this time.
It was 2.24*10^5 N. I must have missed something somewhere.

Thanks

Now I am working through this part:

Where, other than infinitely far away, could the third sphere be placed such that the net gravitational force acting on it from the other two spheres is equal to zero?

But I'm still working it out.

I am thinking that:
\frac{G(.409)(79)}{d^{2}} = \frac{G(.409)(65)}{(3-d)^{2}}
\frac{(79)}{d^{2}} = \frac{(65)}{(3-d)^{2}}
9-6d+d^{2}=\frac{65}{79}d^}{2}

so basically the third sphere needs to be at the point (0,1.43) ?

Edit: Yeah that's all correct!

Thanks for the help.
 
Last edited:

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