Helios
- 267
- 63
So, with the mechanical index of refraction
n = \sqrt{ 1 - V/E }
we plug into the optical ray equation, ( s = arc length )
\nablan - [ \nablan . ( d\vec{r}/ds ) ]( d\vec{r}/ds ) - n ( d^{2} \vec{r}/ ds^{2} ) = 0
and get
\nablaV - [ \nablaV . ( d\vec{r}/ds ) ] ( d\vec{r}/ds ) + 2( E - V )( d^{2} \vec{r}/ ds^{2} ) = 0
Now with the replacements
\vec{F} = -\nablaV
( E - V ) = mv^{2}/2
and get
\vec{F} - [ \vec{F} . ( d\vec{r}/ds ) ] ( d\vec{r}/ds ) - ( mv^{2} )( d^{2} \vec{r}/ ds^{2} ) = 0
d\vec{r}/ds = \hat{T} is a unit vector tangential to the path
d^{2} \vec{r}/ ds^{2} = \hat{N}/R where \hat{N} is a unit normal vector and R is the radius of curvature of the path
So,
\vec{F} - ( \vec{F} . \hat{T} ) \hat{T} - ( mv^{2}/R )\hat{N} = 0
mv^{2}/R is the magnitude of the centripetal force
So with,
\vec{F} = F_{tangent}\hat{T} + F_{normal}\hat{N}
leads me to believe this derivation is correct. Comments?
n = \sqrt{ 1 - V/E }
we plug into the optical ray equation, ( s = arc length )
\nablan - [ \nablan . ( d\vec{r}/ds ) ]( d\vec{r}/ds ) - n ( d^{2} \vec{r}/ ds^{2} ) = 0
and get
\nablaV - [ \nablaV . ( d\vec{r}/ds ) ] ( d\vec{r}/ds ) + 2( E - V )( d^{2} \vec{r}/ ds^{2} ) = 0
Now with the replacements
\vec{F} = -\nablaV
( E - V ) = mv^{2}/2
and get
\vec{F} - [ \vec{F} . ( d\vec{r}/ds ) ] ( d\vec{r}/ds ) - ( mv^{2} )( d^{2} \vec{r}/ ds^{2} ) = 0
d\vec{r}/ds = \hat{T} is a unit vector tangential to the path
d^{2} \vec{r}/ ds^{2} = \hat{N}/R where \hat{N} is a unit normal vector and R is the radius of curvature of the path
So,
\vec{F} - ( \vec{F} . \hat{T} ) \hat{T} - ( mv^{2}/R )\hat{N} = 0
mv^{2}/R is the magnitude of the centripetal force
So with,
\vec{F} = F_{tangent}\hat{T} + F_{normal}\hat{N}
leads me to believe this derivation is correct. Comments?