The second part of your question has to be considered in the Q_dot_rad, which is inside the term "Q_dot_in" of the above equation.
Which is calculated from the Stefan-Boltzmann's Law of Radiation.
The solar radiation not absorbed by the absorber's surface due to its optical properties: (emissivity, reflectivity, transmissivity and absorptivity) is considered in the epsilon greek letter in the Stefan-Boltzmann's law :
Q_dot_rad = eps*A*F*sigma*(T_sup^4 - T_sky^4)
which is the emissivity of the surface
remember that for any surfaces: Reflectivity + Transmissivity + Absorptivity = 1. (rho + tau + alpha = 1)
and for opaque surfaces and in thermal equilibrium:
tau = 0
alpha + rho = 1 ,and
epsilon=alpha.
The other consideration involving the collected/absorbed solar radiation is the one that has to be made due to the orientation and shape of the surface.
This factor is considered in the letter "F" in the Stefan-Boltzmann's equation, and it is called the "View Factor", or "Shape Factor". It's a geometric factor which depends on the shape of the surface, its orientation with respect to the radiation soruce and (sometimes) the surface's emissivity. You can easily find corresponding expressions of the View Factor to your case in a Heat Transfer HANDBOOK.
I can sand you my study: Equations and yelds of parabolic concentrators, that is developed for my thermionic converter which however does not work due to the space charge effect. It has a glass vacuum tube and internal reflectig screen. You should adapt the coefficients and the configuration to your case. Look at add files. This study it has been developed for extremely high temperatures, in the case of applications at lower temperatures the reflective pattern is probably not necessary but the covering with a glass is sufficient.
In the document I sent to you, energy balancing was developed with taking into account only irradiation, because, in my case, there is no convection or conduction, because the collector is under vacuum. There is not treatment of the containment glass because, in my case, it is transparent for both incoming and outgoing radiation. In the case of a collector without cover, you must remove the radiation patterns as the amount of energy lost by radiation will be small. In the air you need to add the subtracted energy share by convection. You can improve the uptake coefficient by blackening the collector but it can still be improved with a selective treatment (big alpha for the solar spectrum, and epsilon small at the design temperature). The same effect is obtained with the blackened collector protected by a cover glass that is transparent to solar radiation and opaque to infrared, with the further advantage of limiting convection or eliminating it if a manifold locked in vacuum glass tubes is also made partial. Good work and I wish you great success.