Loss-free scanning antenna

Claim 1

A two dimensional scan, loss-free, Cassegrain antenna system, comprising: a. a stationary primary reflector in the geometric form of a parabolic surface having a front surface, a focal point, a focal length (f 1 ), and an axis passing through said focal point; b. a movable subreflector in the geometric form of a parabolic surface having a rear surface and a focal length (f 2 ), with said subreflector being smaller than, confocal with, forward of, and facing away from said front surface of said stationary primary reflector, and with said movable subreflector having an axis passing through said focal point of said stationary primary reflector whereat this axis intersects said stationary primary reflector axis and these said intersecting axes define an angle of rotation (α) of said movable subreflector, and wherein said focal length (f 2 ) of said movable subreflector and said focal length (f 1 ) of said stationary primary reflector are related to each other in accordance with the ratio expression: (f.sub.1 /f.sub.2)>1; c. and, a plane wave, movable, electromagnetic radiation source emitting a collimated beam and having an axis passing through said focal point of said stationary primary reflector whereat this axis intersects said stationary primary reflector axis and these intersecting axes define an angle of rotation (β) of said movable source, with said source interposed between said stationary primary reflector and said movable subreflector, and with said source simultaneously disposed such that all rays of said collimated beam emitted by said source impinge upon, and are reflected by, said rear surface of said movable subreflector and, in turn, impinge upon, and are reflected by, said front surface of said stationary primary reflector at a constant, preselected, scan angle (δ), wherein said scan angle is determined by use of the equations δ=β-2α and sin (β-α)=(f.sub.1 /f.sub.2) sin δ where: δ=constant scan angle β=angle of rotation of said movable source α=angle of rotation of said movable subreflector; whereby a relationship is established among the angles δ, β and α; and whereby said collimated electromagnetic radiation beam emitted by said source can be scanned, without loss, by said stationary primary reflector at a constant, preselected, scan angle without moving said primary reflector, and by rotating said source and said subreflector about said focal point of said primary reflector, while maintaining said relationship established by said equation.

Claim 4

A method of scanning a collimated beam of electromagnetic radiation with and from a primary reflector of a two dimensional antenna system, without loss and without moving said primary reflector, comprising the steps of: a. using a two-dimensional Cassegrain antenna system for said scanning, wherein said antenna system includes: said primary reflector in the geometric form of a parabolic surface having a front surface, a focal point, a focal length (f 1 ), and an axis passing through said focal point; a movable subreflector in the geometric form of a parabolic surface having a rear surface, and a focal length (f 2 ), with said subreflector being smaller than, confocal with, forward of, and facing away from said front surface of said primary reflector, and with said movable subreflector having an axis passing through said focal point of said primary reflector whereat this axis intersects said primary reflector axis and these said intersecting axes define an angle of rotation (α) of said movable subreflector, and wherein said focal length (f 2 ) of said movable subreflector and said focal length (f 1 ) of said primary reflector are related to each other in accordance with the ratio expression: (f.sub.1 /f.sub.2)>1; and, a plane wave, movable electromagnetic radiation source emitting said collimated beam and having an axis passing through said focal point of said primary reflector whereat this axis intersects said primary reflector axis and these said intersecting axes define an angle of rotation (β) of said movable source, with said source interposed between said primary reflector and said movable subreflector, and with said source simultaneously disposed such that all rays of said collimated beam emitted by said source impinge upon, and are reflected by, said rear surface of said movable subreflector, and in turn, impinge upon, and are reflected by, said front surface of said primary reflector at a scan angle (δ); b. and, while scanning, maintaining said scan angle (δ) at a constant preselected value, wherein said value of said scan angle is determined by use of the equation: δ=β-2α where: δ=constant scan angle β=angle of rotation of said movable source α=angle of rotation of said movable subreflector.

Claim 5

A method of scanning a collimated beam of electromagnetic radiation with and from a primary reflector of a two dimensional antenna system, without loss and without moving said primary reflector, comprising the steps of: a. using a two-dimensional Cassegrain antenna system for said scanning, wherein said antenna system includes: said primary reflector in the geometric form of a parabolic surface having a front surface, a focal point, a focal length (f 1 ), and an axis passing through said focal point; a movable subreflector in the geometric form of a parabolic surface having a rear surface, and a focal length (f 2 ), with said subreflector being smaller than, confocal with, forward of, and facing away from said front surface of said primary reflector, and with said movable subreflector having an axis passing through said focal point of said primary reflector whereat this axis intersects said primary reflector axis and these said intersecting axes define an angle of rotation (α) of said movable subreflector, and wherein said focal length (f 2 ) of said movable subreflector and said focal length (f 1 ) of said primary reflector are related to each other in accordance with the ratio expression: (f.sub.1 /f.sub.2)>1; and, a plane wave, movable electromagnetic radiation source emitting said collimated beam and having an axis passing through said focal point of said primary reflector whereat this axis intersects said primary reflector axis and these said intersecting axes define an angle of rotation (β) of said movable source, with said source interposed between said primary reflector and said movable subreflector, and with said source simultaneously disposed such that all rays of said collimated beam emitted by said source impinge upon, and are reflected by, said rear surface of said movable subreflector, and in turn, impinge upon, and are reflected by, said front surface of said primary reflector at a scan angle (δ); b. and, while scanning, maintaining said scan angle (δ) at a constant preselected value, wherein said value of said scan angle is determined by use of the equation: δ=β-2α where: δ=constant scan angle β=angle of rotation of said movable source α=angle of rotation of said movable subreflector.