Pression de radiation: application aux voiles solaires

θ
α1=α3= 0 α2α46= 0
α1=α3α2α4
α1=α3α2α1γ α4α1γ
θ=β= 0
β= 90 d−→ uθ−→ v0)
β=−90 d−−→ −uθ
−→
v0)

ν10−34
ν
ν
ν= 530 10−40
−→
v
τ