From: Computational analysis of cooling dynamics in photonic-crystal-based thermal switches
Case B | Case C | Case D | |
---|---|---|---|
r = h p /5 | \( -\left({k}_p\frac{\partial T}{\partial r}\right)=\left({k}_a\frac{\partial T}{\partial r}\right) \) | \( - \left(k\frac{\partial T}{\partial r}\right)=h\left({T}_p-{T}_a\right) \) | \( -\left({k}_p\frac{\partial T}{\partial r}\right)=\sigma \varepsilon \left({T}_p^4-{T}_a^4\right) \) |
0 ≤ φ ≤ 2π | |||
0 ≤ z ≤ h p |