Taking account of cosine low of emission we write for the energy radiated per second by the ** in cavity # 1 as**
where A is an constant, dΩ is an element of solid angle around some direction defined by the symbol Ω . Integrating over the whole forward hemisphere we get
We find A by equating this to the quantity is stefan- Boltzman constant and d is the diameter of the **.**
where is the solid angle subtended by the ** of 2 at 1. {We are assuming area of **/ (distance)2}