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Flat plate collector useful heat and outlet temperature

Short answer

Using Qu = Ac[FR(τα)GT - FR UL (Ti - Ta)]: Qu = 2[0.76×800 - 4.5×10] = 1126 W; efficiency = 1126/(2×800) = 70.4%; outlet temperature To = 30 + 1126/(0.03×4186) ≈ 39.0 °C; stagnation occurs at Ti - Ta = (0.76×800)/4.5 = 135.1 K.

A flat plate collector of area 2 m² has FR(τα)=0.76F_R(\tau\alpha) = 0.76 and FRUL=4.5F_R U_L = 4.5 W/m²K. The solar radiation incident on the collector plane is 800 W/m², the ambient temperature is 20 °C and water enters at 30 °C with a flow rate of 0.03 kg/s (cp=4186c_p = 4186 J/kgK). Calculate (a) the useful heat gain, (b) the collector efficiency, (c) the outlet water temperature, and (d) the maximum value of (Ti−Ta)(T_i - T_a) at which the collector still gives useful heat at this radiation.

Hottel-Whillier-Bliss equation

Qu=Ac[FR(τα) GT−FRUL (Ti−Ta)]Q_u = A_c\left[F_R(\tau\alpha)\,G_T - F_R U_L\,(T_i - T_a)\right]

(a) Useful heat

Qu=2 [0.76(800)−4.5(30−20)]=2 [608−45]=2×563=1126 W\begin{aligned} Q_u &= 2\,[0.76(800) - 4.5(30-20)] \\ &= 2\,[608 - 45] = 2 \times 563 = 1126\ \text{W} \end{aligned}

(b) Efficiency

η=QuAcGT=11262×800=0.704  (70.4 %)\eta = \frac{Q_u}{A_c G_T} = \frac{1126}{2 \times 800} = 0.704 \;(70.4\ \%)

(c) Outlet temperature

Qu=m˙ cp (To−Ti)To−Ti=11260.03×4186=8.97 KTo=30+8.97=38.97 °C\begin{aligned} Q_u &= \dot m\,c_p\,(T_o - T_i) \\ T_o - T_i &= \frac{1126}{0.03 \times 4186} = 8.97\ \text{K} \\ T_o &= 30 + 8.97 = 38.97\ \text{°C} \end{aligned}

(d) Stagnation condition

Useful heat becomes zero when FR(τα)GT=FRUL(Ti−Ta)F_R(\tau\alpha)G_T = F_R U_L (T_i - T_a):

Ti−Ta=0.76×8004.5=135.1 KT_i - T_a = \frac{0.76 \times 800}{4.5} = 135.1\ \text{K}

Answer: Qu=1126Q_u = 1126 W; η=70.4 %\eta = 70.4\ \%; To=39.0T_o = 39.0 °C; useful heat is zero when Ti−Ta=135T_i - T_a = 135 K (the collector is then at stagnation).

✓ Answer checked by Claude Opus 5.5 (high effort)

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