熱抵抗:直列の層を通る定常の熱流は、直列抵抗を流れる電流と同じように振る舞います:Q̇ = ΔT/ΣR。伝導層では R = L/(kA)、対流面では R = 1/(hA)。各層の温度降下はその熱抵抗に比例します。
各層の熱抵抗
R1 = L1/(k1A) = (50/1000)/(0.17·4) = 0.07353 K/W
R2 = L2/(k2A) = (75/1000)/(1.4·4) = 0.01339 K/W
熱流量
Q̇ = (T1 − T3)/(R1 + R2) = 23/0.08692 = 264.6 W
答え
Q̇ = 264.6 W
2.熱伝導
答え: U = 0.3265 W/(m²·K)
熱抵抗:直列の層を通る定常の熱流は、直列抵抗を流れる電流と同じように振る舞います:Q̇ = ΔT/ΣR。伝導層では R = L/(kA)、対流面では R = 1/(hA)。各層の温度降下はその熱抵抗に比例します。
直列の熱抵抗
Ri = 1/(hiA) = 1/(7.7·8) = 0.01623 K/W
R1 = L1/(k1A) = (50/1000)/(1.4·8) = 0.004464 K/W
R2 = L2/(k2A) = (100/1000)/(0.035·8) = 0.3571 K/W
Ro = 1/(hoA) = 1/(25·8) = 0.005 K/W
ΣR = 0.3828 K/W
熱通過率
U = 1/(A·ΣR) = 1/(8·0.3828) = 0.3265 W/(m²·K)
答え
U = 0.3265 W/(m²·K)
3.熱交換器 (LMTD)
答え: A = 1.974 m²
LMTD method: the temperature difference between the streams changes along the exchanger, so the rate equation uses its logarithmic mean: Q̇ = U·A·ΔTlm, with ΔTlm = (ΔT₁ − ΔT₂)/ln(ΔT₁/ΔT₂), where ΔT₁ and ΔT₂ are the differences at the two ends. Counter-flow gives a larger ΔTlm than parallel flow for the same inlet and outlet temperatures.