Chapitre 20 Transferts thermiques conductifs et convecto-conductifs Flashcards

1
Q

loi du rayonnement de Planck

A

uem = (8πhc)/λ⁵)(1/(e^(hc/λkbT)-1))

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2
Q

flux thermique

flux thermique surfacique

A

Iq = Pq = δQ(t)/dt
[Iq]=[P]=w
φ(P) = dIq/dS

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3
Q

vecteur densité volumique de flux thermique

A

Jq

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4
Q

Loi de Fourrier

A
Jq(r,t) = -λ(T)gradT(r,t)
[λ] = W.m^-1.K^-1
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5
Q

capacité thermique du système

capacité volumique du système

A
dC = d(δU)/dT
Cvol = dC/dtau=ρCm
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6
Q

premier principe pour les petits sytèmes

A

d(δU)/dt = dIq + δ²Wautre/dt=dIq + dPautre

=dIq + σr,el dtau

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7
Q

bilan de puissance local

A

ρcm ∂T(x,t)/∂t = - ∂Jq/∂x + σel,r

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8
Q

équation de diffusion thermique 1D cartésienne

A

∂T(x,t)/∂t = D ∂²T(x,t)/∂x² + σ/ρcm avec D = λ/ρcm

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9
Q

equation de diffusion en cylindrique

A

∂T(r,t)/∂t = D(1/r)(∂/∂r)(r∂T(r,t)/∂t) + σ/ρcm

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10
Q

equation de diffusion en sphérique

A

∂T(r,t)/∂t = D(1/r²)(∂/∂r)(r²(∂/∂r)T(r,t)) + σ/ρcm

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11
Q

bilan local général

A

ρcm ∂T(r,t)/∂t = -div(Jq(r,t))+ σ

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12
Q

équation générale de la diffusion 3D

A

∂T(r,t)/∂t = DΔT(r,t) + σ/ρcm

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13
Q

résistance thermique

A

Rq = ΔT/Iq
pour le barreau : Rq = T1-T2/Iq = L/λS
pour le cylindre : Rqcyl = ln(R2/R1)/2πλh
pour la sphère Rqsph = (1/R1 - 1/R)/(1/R1 - 1/R2) (T2-T1) + T1

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14
Q

Loi de Newton

A

φcc(0+) = J.ez = λ/δl(Tp-Tflu) on pose h = λ/δl

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15
Q

resistance conducto-convective

A

Rqcc = (Tp-Tflu) / Iq = 1/hS

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16
Q

définiton nombre de bolt

A

nombre adimensionné qui compare le conducto convectif et le conductif : B = hLc/λ