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|pages=149
 
|pages=149
 
|isbn=978-0-85234-707-2
 
|isbn=978-0-85234-707-2
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|url=http://books.google.com/books?id=p5LkPwAACAAJ&dq=Andrews+Who+made&hl=en&sa=X&ei=ahTXUYX9A4qF4gTLoYGgCQ&ved=0CCsQ6AEwAA
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|url=https://books.google.com/books?id=p5LkPwAACAAJ&dq=Andrews+Who+made&hl=en&sa=X&ei=ahTXUYX9A4qF4gTLoYGgCQ&ved=0CCsQ6AEwAA
 
|quote= }}</ref>  
 
|quote= }}</ref>  
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Take a [[point source]] that is propagating something ([[light]], [[sound]], [[gravity]], [[electric field]], etc..) out. Thus
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Take a point source that is propagating something ([[light]], [[sound]], [[gravity]], [[electric field]], etc..) out.  
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The inverse square law can be derived by looking at the surface area of a [[sphere]] of radius ''r''.  The surface area of a sphere is 4&pi;r<sup>2</sup>.  As the radius increases, the surface area of the sphere goes up with the square of the radius and the intensity of the phenomena will be inversely proportional to the [[surface area]].   
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The inverse square law can be derived by looking at the surface area of a [[sphere]] of radius <math>r</math>.  The surface area of a sphere is <math>4 \pi r^2</math> As the radius increases, the surface area of the sphere goes up with the square of the radius and the intensity of the phenomena will be inversely proportional to the [[surface area]].   
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With gravity, the inverse square law can be seen in Gm<sub>1</sub>m<sub>2</sub> / r<sup>2</sup>.
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With gravity, the inverse square law can be seen as:
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<math>
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F= \frac{Gm_1m_2}{r^2}
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</math>
    
== Applications ==
 
== Applications ==
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* [http://hyperphysics.phy-astr.gsu.edu/hbase/Forces/isq.html Inverse Square Law] at Hyperphysics
 
* [http://hyperphysics.phy-astr.gsu.edu/hbase/Forces/isq.html Inverse Square Law] at Hyperphysics
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== Refrences ==
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== References ==
 
<references />
 
<references />
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[[Category: Physics]]
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[[Category:Laws of Physics]]
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[[Category:Physics]]
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