Three Modes of Heat Transfer “radiation” “conduction” “convection” © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 1 Conduction dT Q kA dx L RTH kA © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 2 Convection Q RTH = Cooling by mass motion (diffusion + advection) in a fluid © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 3 Radiation 2 hc02 ebb ( ) 5 exp(hc0 / k BT ) 1 Q 1 F1 2 A1 (T14 T24 ) Linearize (when and why?): For black body (Ɛ=1) at 300 K: hrad 4(5.67 108 )(300)3 6 W/m 2 K Note: Usually nothing is a perfect “black body” and parts of the emissive spectrum may be missing (ex: photonic band gap crystals). © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 4 Boundaries and Lumped Elements • All problems have boundaries! • Heat diffusion equation needs boundary conditions • Dirichlet (fixed T): • Neumann (fixed flux ~ dT/dx): • When is it OK to “lump” a body as a single R or C? • Biot number: © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 5 Transient Cooling of Lumped Body Source: Lienhard book, http://web.mit.edu/lienhard/www/ahtt.html (2008) © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 6 What if Biot Number is Large • Bi = hL/kb << 1 implies Tb(x) ~ Tsurf (lumped OK) • Bi = hL/kb >> 1 implies significant internal Tb(x) gradient © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 7 Lumped Body Examples (Steady State) Boundary conditions: TL = 400 oC, TR = 100 oC 1) Assume NO internal heat generation (how does the temperature slope dT/dx scale qualitatively within each layer?) 2) Assume UNIFORM internal heat generation Rcyl Rslab © 2010 Eric Pop, UIUC ln(r0 / ri ) 2 lk L kA ECE 598EP: Hot Chips 8 Contact Resistance • RC = 1/hCA • BUT, also remember the fundamental solid-solid contact resistance given by density of states, acoustic/diffuse phonon mismatch ~Cv/4! (prof. Cahill’s lecture) © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 9 Notes on Finite-Element Heat Diffusion Ti-1 Δx T1 Ti A(kT ) p' g (T T0 ) 0 Ti+1 RC dui ui 1 ui 1 dx 2x T0 d 2ui ui 1 2ui ui 1 2 2 dx x TN L T0 Boundary conditions: (heat flux conservation) © 2010 Eric Pop, UIUC b1 M21 M22 M23 0 … … T2 T1 T1 T0 k A 1 x RC T1 … dT T T k1 A 1 1 0 dx RC M11 M12 0 … TN bN T b = MNN M ECE 598EP: Hot Chips Matlab: T = M\b 10 More Comments on “Fin Equation” L x x+dx d W tox SiO2 Si T0 • Same as Poisson equation with various BC’s • BC’s can be given flux (dT/dx) or given temperature (T0) • Very useful to know: – Thermal healing length LH (Poisson: screening length) – General, qualitative shape or solution d 2T hp (T T0 ) 0 2 dx kA © 2010 Eric Pop, UIUC general solution T T0 C1e x / LH C2 e x / LH sinh, cosh, tanh … etc. ECE 598EP: Hot Chips 11 Fin Efficiency (how long is too long?) L d W T=TB dT/dx ≈ 0 sinh, cosh, tanh, exp 8 6 exp 4 2 cosh tanh 0 -2 -4 -2 sinh -1 0 x/LH 1 2 • Fin efficiency η = actual heat loss by fin / heat loss if entire fin was at base temperature TB • Actual heat loss: tanh( L / LH ) • Here L / LH © 2010 Eric Pop, UIUC Not worth making cooling fins much >> LH ! ECE 598EP: Hot Chips 12 Poisson Equation Analogy with solution Liu (1993) Knoch (2006) and electrostatic screening length nt d nt Cox • Thermal fin is ~ mathematically same problem as 1-D transistor electrostatics, e.g. nanowire or SOI transistor • L < λ short fin, or “short channel” FET • L >> λ long fin (too long?!), or “long channel” FET © 2010 Eric Pop, UIUC ECE 598EP: Hot Chips 13