Difference between revisions of "Forest UCM Energy CentralForce"

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:<math> \vec \nabla \right  = \hat r \frac{d}{dr}  + \hat \theta \frac{1}{r} \frac{d}{d \theta}  +  \hat phi \frac{1}{ r \sin \theta } \frac{d}{d\phi} </math>
+
:<math> \vec \nabla   = \hat r \frac{d}{dr}  + \hat \theta \frac{1}{r} \frac{d}{d \theta}  +  \hat phi \frac{1}{ r \sin \theta } \frac{d}{d\phi} </math>
  
  

Revision as of 13:54, 27 September 2014

A central force is defined as a force depends only on separation distance

[math]\vec{F} = f(\vec r) \hat r[/math]

ie

Coulomb force and gravitation force.

Spherical Coordinates

Forest UCM SphericalCoordUnitVec.png

Forest_UCM_NLM_Ch1_CoordSys#Spherical

Gradient in spherical coordinates

The differential change of [math]\vec r[/math] in spherical coordinates occurs in three directions.


In the radial direction

[math]dr \hat r[/math]

In the polar angle direction

[math]r d \theta \hat \theta[/math]

In the azimuthal angle direction

[math]r \sin \phi d \phi \hat \phi[/math]

The differential force of the displacement vector in spherical coordinates is

[math]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]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]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]\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]\vec \nabla f \cdot d \vec r = \vec \nabla f \cdot \left ( dr \hat r + r d \theta \hat \theta + r \sin \phi d \phi \hat \phi \right )[/math]
[math]= \left ( \vec \nabla f \right )_r dr +\left ( \vec \nabla f \right )_{\theta} r d\theta +\left ( \vec \nabla f \right )_{\phi} r \sin \theta d\phi [/math]

comparing terms of the above with

[math]\left ( \vec \nabla f \right )_r dr =\frac{df}{dr} dr \Rightarrow \left ( \vec \nabla f \right )_r =\frac{df}{dr} [/math]
[math]\left ( \vec \nabla f \right )_{\theta} r d\theta =\frac{df}{d \theta} d\theta \Rightarrow \left ( \vec \nabla f \right )_{\theta} d\theta =\frac{1}{r} \frac{df}{d \theta} [/math]
[math] \left ( \vec \nabla f \right )_{\phi} r \sin \theta d\phi =\frac{df}{d\phi} d\phi \Rightarrow \left ( \vec \nabla f \right )_{\phi} d\phi = \frac{1}{ r \sin \theta } \frac{df}{d\phi} [/math]


or

[math] \vec \nabla = \hat r \frac{d}{dr} + \hat \theta \frac{1}{r} \frac{d}{d \theta} + \hat phi \frac{1}{ r \sin \theta } \frac{d}{d\phi} [/math]



Forest_UCM_Energy#Central_Forces