Forest UCM Energy CentralForce
A central force is defined as a force depends only on separation distance
- [math]\displaystyle{ \vec{F} = f(\vec r) \hat r }[/math]
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Coulomb force and gravitation force.
Spherical Coordinates
Forest_UCM_NLM_Ch1_CoordSys#Spherical
Gradient in spherical coordinates
The differential change of [math]\displaystyle{ \vec r }[/math] in spherical coordinates occurs in three directions.
In the radial direction
- [math]\displaystyle{ dr \hat r }[/math]
In the polar angle direction
- [math]\displaystyle{ r d \theta \hat \theta }[/math]
In the aximuthal angle direction
- [math]\displaystyle{ r \sin \phi d \phi \hat \phi }[/math]
The differential force of the displacement vector in spherical coordinates is
- [math]\displaystyle{ d \vec r = dr \hat r + r d \theta \hat \theta + r \sin \phi d \phi \hat \phi }[/math]
The derivative may be represented as
- [math]\displaystyle{ df = f(x+dx) -f(x) = \frac{df}{dx} dx }[/math]
in three dimensional cartesian coordinates this may be written in terms of the gradient as
- [math]\displaystyle{ df = \frac{df}{dx} dx + \frac{df}{dy} dy + \frac{df}{dz} dz =\vec \nabla f \cdot d \vec r }[/math]
To determine the gradient in sperical coordinates on just compares the two equations
- [math]\displaystyle{ \frac{df}{dr} dr + \frac{df}{d \theta} d\theta + \frac{df}{d\phi} d\phi =\vec \nabla f \cdot d \vec r }[/math]
- [math]\displaystyle{ \vec \nabla f \cdot d \vec r = \left . \vec \nabla f \right |_r dr }[/math]
comparing terms of the above with
- [math]\displaystyle{ d \vec r = dr \hat r + r d \theta \hat \theta + r \sin \phi d \phi \hat \phi }[/math]