A device for measuring a light radiation pressure is provided which includes a torsion balance, a laser, a convex lens, and a line array detector. The laser is configured to emit a first laser beam. The convex lens is located on an optical path of the first laser beam and configured to focus the first laser beam to a surface of the reflector. The line array detector is configured to detect a reflected first laser beam reflected by the reflector. The disclosure also provides a method for measuring the light radiation pressure using the device.

A device for measuring a light radiation pressure is provided which includes a torsion balance, a laser, a convex lens, and a line array detector. The laser is configured to emit a first laser beam. The convex lens is located on an optical path of the first laser beam and configured to focus the first laser beam to a surface of the reflector. The line array detector is configured to detect a reflected first laser beam reflected by the reflector. The disclosure also provides a method for measuring the light radiation pressure using the device.

The present invention relates to a system for measuring the power of electromagnetic radiation (EMR) using piezoelectric transducers (PZTs) and pyroelectric transducers (PRTs). According to an illustrative embodiment of the present disclosure, a target cell has a mirrored surface that can partially reflect and partially absorb EMR. Each target cell can include or be coupled to PZTs and PRTs. When incident EMR reflects off of targets cells, the reflected portion creates radiation pressure and the non-reflected portions creates heat. The PZTs convert the pressure into a first electric current, and the PRTs convert the heat into a second electric current. Measuring the first and/or second currents allows a user to calculate the original power of an EMR source. By utilizing multiple target cells placed in specially designed arrays, a user can calculate fluctuations of EMR power by time and location across the target cells.

The present invention relates to an optical energy meter. Illustrative embodiments of the present disclosure include a system controller, temperature sensing system, vibration sensing system, torque sensing system, graphical display system, climate control system, and vibration control system. The invention measures the radiation pressure of incident high power electromagnetic radiation. The measurement of radiation pressure can be used to determine the power of the radiation; that is, the purposes of the invention are to measure, with high precision and accuracy, and survive the power of an incident high power electromagnetic beam while minimizing size, weight, and power requirements.

The present invention relates to an optical energy meter. Illustrative embodiments of the present disclosure include a system controller, temperature sensing system, vibration sensing system, torque sensing system, graphical display system, climate control system, and vibration control system. The invention measures the radiation pressure of incident high power electromagnetic radiation. The measurement of radiation pressure can be used to determine the power of the radiation; that is, the purposes of the invention are to measure, with high precision and accuracy, and survive the power of an incident high power electromagnetic beam while minimizing size, weight, and power requirements.

A device for measuring a light radiation pressure is provided which includes a torsion balance, a laser, a convex lens, and a line array detector. The laser is configured to emit a first laser beam. The convex lens is located on an optical path of the first laser beam and configured to focus the first laser beam to a surface of the reflector. The line array detector is configured to detect a reflected first laser beam reflected by the reflector. The disclosure also provides a method for measuring the light radiation pressure using the device.

A device for measuring a light radiation pressure is provided which includes a torsion balance, a laser, a convex lens, and a line array detector. The laser is configured to emit a first laser beam. The convex lens is located on an optical path of the first laser beam and configured to focus the first laser beam to a surface of the reflector. The line array detector is configured to detect a reflected first laser beam reflected by the reflector. The disclosure also provides a method for measuring the light radiation pressure using the device.

The present invention relates to a system for measuring the power of electromagnetic radiation (EMR) using piezoelectric transducers (PZTs) and pyroelectric transducers (PRTs). According to an illustrative embodiment of the present disclosure, a target cell has a mirrored surface that can partially reflect and partially absorb EMR. Each target cell can include or be coupled to PZTs and PRTs. When incident EMR reflects off of targets cells, the reflected portion creates radiation pressure and the non-reflected portions creates heat. The PZTs convert the pressure into a first electric current, and the PRTs convert the heat into a second electric current. Measuring the first and/or second currents allows a user to calculate the original power of an EMR source. By utilizing multiple target cells placed in specially designed arrays, a user can calculate fluctuations of EMR power by time and location across the target cells.

The present application describes embodiments of a non-tracking solar energy collector comprising: (a) at least one solar radiation concentrator for collimating and directing the incident solar radiation rays to at least one focal point along the surface of a reactive reflector; (b) the reactive reflector mounted on top of an external cavity and having at least one transparency zone instantly formed at said at least one focal point of the solar radiation rays, for letting the solar radiation rays enter said external cavity, wherein said transparency zone is constantly moving along the surface of said reactive reflector following the position of said at least one focal point of the solar radiation rays; and (c) the external cavity containing a solar cell and capable of trapping the entered solar radiation rays by inner scattering of said solar radiation rays on the walls of said external cavity, wherein said inner scattering of said solar radiation rays inside said external cavity is preventing solar radiation to escape from said solar cell, thereby minimising solar radiation losses.

The present application describes embodiments of a non-tracking solar energy collector comprising: (a) at least one solar radiation concentrator for collimating and directing the incident solar radiation rays to at least one focal point along the surface of a reactive reflector; (b) the reactive reflector mounted on top of an external cavity and having at least one transparency zone instantly formed at said at least one focal point of the solar radiation rays, for letting the solar radiation rays enter said external cavity, wherein said transparency zone is constantly moving along the surface of said reactive reflector following the position of said at least one focal point of the solar radiation rays; and (c) the external cavity containing a solar cell and capable of trapping the entered solar radiation rays by inner scattering of said solar radiation rays on the walls of said external cavity, wherein said inner scattering of said solar radiation rays inside said external cavity is preventing solar radiation to escape from said solar cell, thereby minimising solar radiation losses.