Stirling cycle, concentrated solar power, solar irradiance, global radiation
The principle of concentrated solar power (CSP) is used in solar thermal power plants. Incoming irradiance is concentrated by mirrors and focused on a thermal collector, where a medium is heated. The most common approach is to use parabolic troughs heating up collector pipes in the focal line of the troughs. The collector pipes are filled with a heat transfer fluid transporting the thermal energy to a heat engine (e.g. a steam turbine) connected to an electrical generator.
Another way - for several reasons less common - is the use of a parabolic mirror (aka “dish”) focusing on the hot end of a Stirling engine.
Fig.:Solar dish-Stirling generator consisting of a parabolic mirror and a Stirling engine.
Source: https://de.wikipedia.org/wiki/Solar-Stirling (de. Use Google translate for en)
Fig.: Map of global irradiation on a horizontal plane.
Please consider the different color scales! The two irradiance diagrams are not directly comparable!
Source: https://en.wikipedia.org/wiki/Solar_irradiance
Fig.: Map of direct normal irradiation.
Please consider the different color scales! The two irradiance diagrams are not directly comparable!
Source: https://en.wikipedia.org/wiki/Solar_irradiance
Fig.: Beta-type Stirling engine, with only one cylinder, hot at one end and cold at the other. A loose-fitting displacer shunts the air between the hot and cold ends of the cylinder. A power piston at the open end of the cylinder drives the flywheel.
Source: https://en.wikipedia.org/wiki/Stirling_engine/
Fig.: P-V-diagram of a beta Stirling maschine: Ideal cycle vs. real cycle. The temperatures of the ideal isothermals are 400K and 850K , respectively.
Source: Egas, J. and Clucas D.M (2018)
The non-comprehensive list is for inspiration.