22-Mec-A1 Applied Thermodynamics and Heat Transfer · May 2014
Question 5 of 8: Composite Plastic–Cork Wall with Radiant Heating
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper: National Examinations — 07-Mec-A1 Applied Thermodynamics and Heat Transfer, May 2014. Open-book, 3-hour paper. Part A (Thermodynamics, Q1–Q4) and Part B (Heat Transfer, Q5–Q8); a complete paper is any five questions — three from one part and two from the other, all of equal value. Full worked solutions to all eight questions are given below.
Reference texts: Çengel & Boles, Thermodynamics: An Engineering Approach (9th ed., McGraw-Hill) — closed- and open-system energy balances, steam tables, gas power cycles, reciprocating compressors and vapour-compression refrigeration; Çengel & Ghajar, Heat and Mass Transfer (6th ed.) and Incropera, DeWitt, Bergman & Lavine, Fundamentals of Heat and Mass Transfer (8th ed., Wiley) — composite-wall conduction, internal-flow and cross-flow convection correlations, natural convection with radiation, and the ε–NTU heat-exchanger method. Freon-12 property data are taken from the appendix supplied with the exam; steam and air data from standard tables.
Question 5: Composite Plastic–Cork Wall with Radiant Heating (equal value)
Find. The radiant heat flux $q''$ (per unit area) that must be supplied at the plastic surface.
Figure 4 — Equivalent thermal network. Applied flux splits at the plastic surface node $T_s$: one branch convects directly to the room ($R_{\text{conv},p}=1/h$); the other conducts through the plastic to the glue interface ($R_\text{plastic}=L_p/k_p$), then through the cork ($R_\text{cork}=L_c/k_c$) and out by convection ($R_{\text{conv},c}=1/h$) to the room.
Approach. Fix the interface at 30 °C, compute the heat leaving through the cork branch, use it to find the small plastic-surface overtemperature, then add the convective loss at the plastic surface to obtain the total applied flux.
Heat through the cork branch. From the 30 °C interface out to the 25 °C room,$$q''_\text{cork}=\frac{T_i-T_\infty}{R_\text{cork}+R_\text{conv}}=\frac{30-25}{0.714+0.10}=\boxed{6.14\ \text{W/m}^2}.$$
Plastic-surface temperature. The same flux conducts through the thin, conductive plastic, so $T_s$ is barely above the interface:$$T_s=T_i+q''_\text{cork}R_\text{plastic}=30+6.14(0.00435)=30.03\ ^\circ\text{C}.$$
Total applied flux. At the plastic surface the applied heat both feeds the cork branch and makes up the direct convective loss to the room:$$q''=q''_\text{cork}+h(T_s-T_\infty)=6.14+10(30.03-25)=6.14+50.3=\boxed{56.4\ \text{W/m}^2}.$$
Check
Because the plastic is thin and highly conductive, almost the entire applied flux is lost by convection at the heated plastic surface (50.3 of 56.4 W/m²); only 6.14 W/m² actually crosses into the cork. If the intent were to insulate the plastic face against room convection, the required flux would drop to about 6.1 W/m². The result is quoted per unit bond area.