17-Phys-B6 Applied Thermodynamics and Heat Transfer · May 2013
Question 2 of 8: Two-Stage Reheat Turbine — Boiler Capacity
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. 98-Phys-B6 Applied Thermodynamics and Heat Transfer,
National Examination May 2013 — an open-book examination (any textbook, reference or
non-communicating calculator permitted). Part A (Thermodynamics, Q1–4) and Part B (Heat
Transfer, Q5–8) together form the paper; a complete exam is five answers, drawn either
three-from-A/two-from-B or two-from-A/three-from-B. Every question is nonetheless answered in
full below so the paper remains a complete study resource. All eight questions carry equal
value in the grading.
Reference texts. Y. A. Çengel & M. A. Boles, Thermodynamics: An
Engineering Approach, 8th ed. (ideal-gas cycles, vapour power cycles with reheat, gas
compressors, vapour-compression refrigeration); F. P. Incropera & D. P. DeWitt,
Fundamentals of Heat and Mass Transfer, 7th ed. (critical radius of insulation,
internal/external forced convection correlations, natural convection from horizontal cylinders,
radiation exchange, LMTD/effectiveness–NTU heat-exchanger analysis).
Given. Steam enters the HP stage at $4.50$ MPa, $350^{\circ}\text{C}$;
HP exhaust/extraction at $150$ kPa with $\dot m_{extract}=10{,}900$ kg/hr; remaining
steam reheated to $300^{\circ}\text{C}$ at $150$ kPa, expanded through the LP stage to
$7.5$ kPa; $\dot W_{turbine}=3730$ kW; $\eta_{HP}=84\%$, $\eta_{LP}=81\%$.
Find. The boiler (total steam) capacity $\dot m_{tot}$ in kg/s.
Figure — T–s diagram: HP expansion 1→2 (dashed 2s = isentropic,
solid 2 = actual), constant-pressure reheat 2→3 at 150 kPa, LP expansion 3→4
(dashed 4s = isentropic, solid 4 = actual, exiting into the superheated region at 7.5 kPa).
Approach. Get steam-table properties at each state (open-book — any
standard steam table), apply each stage's isentropic efficiency to get the actual enthalpy drop,
then close a power balance across both stages with the extraction removed between them.
State 1 — HP inlet. At $4.50$ MPa, $350^{\circ}\text{C}$ (superheated):
$h_1=3081.5$ kJ/kg, $s_1=6.515$ kJ/kg·K.
State 2s/2 — HP exhaust. Isentropic expansion to $150$ kPa
($s_{2s}=s_1$) lands in the two-phase region at $T_{sat}=111.4^{\circ}\text{C}$, giving
$h_{2s}=2421.0$ kJ/kg. Applying the stage efficiency,
$$h_2=h_1-\eta_{HP}(h_1-h_{2s})=3081.5-0.84(3081.5-2421.0)=\boxed{2526.7\ \text{kJ/kg}},$$
so $w_{HP}=h_1-h_2=554.8$ kJ/kg.
State 3 — after reheat. At $150$ kPa, $300^{\circ}\text{C}$
(superheated): $h_3=3073.3$ kJ/kg, $s_3=8.028$ kJ/kg·K.
State 4s/4 — LP exhaust. Isentropic expansion to $7.5$ kPa
($s_{4s}=s_3$) gives a wet state $h_{4s}=2504.6$ kJ/kg ($x_{4s}=0.971$). Applying the LP
stage efficiency,
$$h_4=h_3-\eta_{LP}(h_3-h_{4s})=3073.3-0.81(3073.3-2504.6)=\boxed{2612.6\ \text{kJ/kg}}$$
(this actually lands just INTO the superheated region, $T_4\approx60.5^{\circ}\text{C}$, since
the 81%-efficient expansion generates enough irreversibility to keep the steam dry — a
useful, if slightly counter-intuitive, check on the arithmetic), so $w_{LP}=h_3-h_4=460.7$ kJ/kg.
Boiler capacity from the power balance. The full flow $\dot m_{tot}$ does
HP work; only the remaining flow $\dot m_{tot}-\dot m_{extract}$ (with
$\dot m_{extract}=10{,}900/3600=3.028$ kg/s) does LP work:
$$\dot W_{turbine}=\dot m_{tot}\,w_{HP}+(\dot m_{tot}-\dot m_{extract})\,w_{LP}.$$
Solving for $\dot m_{tot}$,
$$\dot m_{tot}=\frac{\dot W_{turbine}+\dot m_{extract}\,w_{LP}}{w_{HP}+w_{LP}}
=\frac{3730+3.028\times460.7}{554.8+460.7}=\boxed{5.05\ \text{kg/s}}.$$