Parameterization of Horn Torus Formed by Hertz Dipole Radiation Pattern
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Hello dear StackExchange community.
The spatial intensity distribution radiated by a Hertz dipole is $propto sin^2(varphi)$ perpendicular to the dipole axis.
In 2D, it is parameterized by
$ x(varphi) = sin^2(varphi) , cos(varphi) $
$ y(varphi) = sin^3(varphi) $
after using $ x = r ; cos(varphi) ;$ and $, y = r , sin (varphi) $.
Question: In 3D, the emitted intensity looks like this. The parametrization of a simple horn torus is clear (also explained already in this forum). But how does the parameterization change due to the different form of the smaller circle?
I hope my problem description was clear enough. Thanks in advance.
geometry multivariable-calculus trigonometry analytic-geometry parametric
add a comment |Â
up vote
0
down vote
favorite
Hello dear StackExchange community.
The spatial intensity distribution radiated by a Hertz dipole is $propto sin^2(varphi)$ perpendicular to the dipole axis.
In 2D, it is parameterized by
$ x(varphi) = sin^2(varphi) , cos(varphi) $
$ y(varphi) = sin^3(varphi) $
after using $ x = r ; cos(varphi) ;$ and $, y = r , sin (varphi) $.
Question: In 3D, the emitted intensity looks like this. The parametrization of a simple horn torus is clear (also explained already in this forum). But how does the parameterization change due to the different form of the smaller circle?
I hope my problem description was clear enough. Thanks in advance.
geometry multivariable-calculus trigonometry analytic-geometry parametric
add a comment |Â
up vote
0
down vote
favorite
up vote
0
down vote
favorite
Hello dear StackExchange community.
The spatial intensity distribution radiated by a Hertz dipole is $propto sin^2(varphi)$ perpendicular to the dipole axis.
In 2D, it is parameterized by
$ x(varphi) = sin^2(varphi) , cos(varphi) $
$ y(varphi) = sin^3(varphi) $
after using $ x = r ; cos(varphi) ;$ and $, y = r , sin (varphi) $.
Question: In 3D, the emitted intensity looks like this. The parametrization of a simple horn torus is clear (also explained already in this forum). But how does the parameterization change due to the different form of the smaller circle?
I hope my problem description was clear enough. Thanks in advance.
geometry multivariable-calculus trigonometry analytic-geometry parametric
Hello dear StackExchange community.
The spatial intensity distribution radiated by a Hertz dipole is $propto sin^2(varphi)$ perpendicular to the dipole axis.
In 2D, it is parameterized by
$ x(varphi) = sin^2(varphi) , cos(varphi) $
$ y(varphi) = sin^3(varphi) $
after using $ x = r ; cos(varphi) ;$ and $, y = r , sin (varphi) $.
Question: In 3D, the emitted intensity looks like this. The parametrization of a simple horn torus is clear (also explained already in this forum). But how does the parameterization change due to the different form of the smaller circle?
I hope my problem description was clear enough. Thanks in advance.
geometry multivariable-calculus trigonometry analytic-geometry parametric
asked Jul 29 at 18:58


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