22-Mec-B2 Environmental Control in Buildings · December 2017
Question 2 of 8: Winter heating and humidification plant — preheater rating and washer efficiency
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. Engineers Canada national
examination 16-Mec-B2 Environmental Control in Buildings, December 2017,
three hours, open book. Eight problems of 20 points each;
candidates are required to solve five, and all questions carry the same value.
ASHRAE Psychrometric Chart No. 1 (SI and inch-pound) and a pressure–enthalpy
diagram for R-717 are appended to the paper as pages 6–8.
All eight problems are worked here. The paper mixes SI and inch-pound units deliberately:
Problems 1, 3 and 4 are SI, Problems 2, 6 and 7 are inch-pound, and Problem 8 is
SI with a Canadian climate. Each solution is worked in the units the question
uses, as the cover-page instructions require.
Reference texts for this subject.
W. P. Jones, Air Conditioning Engineering, 5th ed.,
Butterworth-Heinemann — the standard reference for this examination code;
Ch. 2–3 (psychrometry and the psychrometric chart), Ch. 6 (air-conditioning
plant cycles), Ch. 7 (the cooling coil, apparatus dew point and by-pass factor),
Ch. 9 (cooling towers), Ch. 15 (fans).
McQuiston, Parker & Spitler, Heating, Ventilating and Air
Conditioning: Analysis and Design, 6th ed., Wiley — Ch. 3 (moist air),
Ch. 5 (heat transmission in building structures), Ch. 8 (energy estimating and the
degree-day method), Ch. 12 (fans and duct design).
ASHRAE Handbook — Fundamentals — Ch. 1 (psychrometrics),
Ch. 14 (climatic design information), Ch. 21 (duct design), Ch. 25–27
(thermal and moisture performance of the building envelope), Ch. 30 (fenestration).
Stoecker & Jones, Refrigeration and Air Conditioning, 2nd ed.,
McGraw-Hill — Ch. 10–12 (vapour-compression cycle, compressors,
condensers and evaporators); ASHRAE Handbook — Refrigeration for
ammonia plant practice.
National Building Code of Canada and the National Energy Code of Canada for
Buildings (NRC), Appendix C climatic data; CSA and Canada Green Building Council
material for Problem 5.
Property basis used throughout. Moist-air
properties are computed from the ASHRAE Fundamentals ideal-moist-air
relations, so every state quoted here can be read back off the psychrometric chart
supplied with the paper:
with $h$ in $\text{kJ/kg}$ of dry air for $t$ in $\,{}^{\circ}\text{C}$ and in
$\text{Btu/lb}$ of dry air for $t$ in $\,{}^{\circ}\text{F}$. Ammonia properties
are quoted on the same datum as the attached ASHRAE p–h diagram
($h_f=200\ \text{kJ/kg}$ and $s_f=1.0\ \text{kJ/(kg}\cdot\text{K)}$ for saturated
liquid at $0\,{}^{\circ}\text{C}$); only differences enter the answers, so any
consistent chart or table gives the same duties.
Question 2: Winter heating and humidification plant — preheater rating and
washer efficiency (20 points)
$68\,{}^{\circ}\text{F}$ db, $48.5\,{}^{\circ}\text{F}$ dew point
Space heating load (all sensible)
$\dot Q_R$
$250{,}000\ \text{Btu/h}$
System air flow
$\dot V$
$7250\ \text{cfm}$
Outdoor air for ventilation
$\dot V_O$
$2400\ \text{cfm}$
Outdoor design state
$t_O,\ \phi_O$
$30\,{}^{\circ}\text{F}$ db, $60\%$ RH
Main heater rating
$\dot Q_{mh}$
$360{,}000\ \text{Btu/h}$
Plant
$-$
preheater → adiabatic spray cabinet → main heater
Find. The plant diagram with every state point characterised,
the cycle on the chart, the Btu/h rating of the preheater, and the adiabatic
saturation efficiency of the spray cabinet together with its make-up water rate.
Part (a) — the winter plant. Outdoor air mixes with return air at M, is preheated to 2, adiabatically humidified to 3 in the spray cabinet, and raised to the supply temperature S by the main heater.
Approach. Everything in this problem is determined —
there is nothing to assume. The all-sensible room load fixes the supply state, the
stated main-heater rating fixes the state leaving the washer, the washer is
adiabatic so it fixes the state leaving the preheater, and the preheater duty is
then simply what is left between the mixed state and that point.
Convert the air quantities to dry-air mass flow. Using
standard air ($13.33\ \text{ft}^3/\text{lb}$, i.e. $4.5$ lb of dry air per hour per
cfm), which is also the basis of the familiar $1.10\,\dot V\,\Delta t$ sensible
relation:
$$\dot m_{da}=4.5\times7250=32{,}625\ \text{lb/h},\qquad
x_O=\frac{2400}{7250}=0.3310$$
so $10{,}800\ \text{lb/h}$ of outdoor air mixes with $21{,}825\ \text{lb/h}$ of
return air.
Part (a) — fix the two given states. A
$48.5\,{}^{\circ}\text{F}$ dew point means the space humidity ratio is the
saturation value at that temperature:
Point
Description
$t$ (°F db)
$W$ (gr/lb)
$h$ (Btu/lb)
$\phi$ (%)
$t_{wb}$ (°F)
O
outdoor air
30.00
14.58
9.44
60.0
26.08
R
space / return
68.00
50.48
24.19
49.6
56.72
Mix the two streams at M. Mass-weighting $W$ and $h$ and
deriving the dry bulb:
$$W_M=0.3310(14.58)+0.6690(50.48)=38.59\ \text{gr/lb}=0.005513\ \text{lb/lb}$$
$$h_M=0.3310(9.44)+0.6690(24.19)=19.31\ \text{Btu/lb}$$
$$t_M=\frac{h_M-1061\,W_M}{0.240+0.444\,W_M}=55.50\,{}^{\circ}\text{F}
\quad(59.2\%\ \text{RH})$$
Find the supply state S from the room balance. The room
load is entirely sensible, so the air adds no moisture to the space and leaves it
with the moisture it arrived with: $W_S=W_R=50.48\ \text{gr/lb}$. The energy
balance on the room gives
$$h_S=h_R+\frac{\dot Q_R}{\dot m_{da}}=24.19+\frac{250{,}000}{32{,}625}
=31.85\ \text{Btu/lb}
\;\Rightarrow\; t_S=99.51\,{}^{\circ}\text{F}\ (18.0\%\ \text{RH})$$
As a check against the familiar shortcut,
$\Delta t=250{,}000/(1.10\times7250)=31.3\ \text{F}^{\circ}$, giving
$99.3\,{}^{\circ}\text{F}$ — the same answer to within the rounding built
into the $1.10$ coefficient.
Work backwards through the main heater to state 3. The
main heater is sensible, so it too leaves $W$ unchanged, and its stated rating
fixes how far below the supply temperature the washer must deliver:
$$h_3=h_S-\frac{\dot Q_{mh}}{\dot m_{da}}=31.85-\frac{360{,}000}{32{,}625}
=20.82\ \text{Btu/lb}
\;\Rightarrow\; t_3=54.14\,{}^{\circ}\text{F}\ (81.2\%\ \text{RH})$$
This is the step that makes the problem determinate. Without the stated rating the
split of duty between the preheater and the main heater would be a free choice.
Work backwards through the adiabatic washer to state 2.
The spray cabinet exchanges no heat with its surroundings, so the only energy
crossing its boundary is the enthalpy of the make-up water that replaces what
evaporates:
$$h_2=h_3-(W_3-W_2)\,h_f(t_3)
=20.82-(0.007211-0.005513)(22.3)=20.78\ \text{Btu/lb}$$
The washer adds moisture but no dry air, so $W_2=W_M=38.59\ \text{gr/lb}$ and
$$t_2=\frac{h_2-1061\,W_2}{0.240+0.444\,W_2}=61.58\,{}^{\circ}\text{F}
\quad(47.6\%\ \text{RH})$$
Part (c) — the preheater rating. The preheater takes
the air from the mixed state M to state 2:
$$\dot Q_{pre}=\dot m_{da}\,(h_2-h_M)=32{,}625\,(20.78-19.31)
=\boxed{48{,}100\ \text{Btu/h}}$$
This is the same duty whether the preheater sits in the outdoor-air branch or in
the mixed stream, because it is the same air raised through the same total enthalpy
rise. Placed in the outdoor-air branch alone — the usual arrangement, since
that is where freeze protection is wanted — it would raise the $2400$ cfm of
outdoor air by about $18\ \text{F}^{\circ}$, from $30$ to roughly
$48\,{}^{\circ}\text{F}$.
Part (d) — adiabatic saturation efficiency. An
adiabatic washer moves the air along its own thermodynamic wet-bulb line, and the
wettest state it could possibly deliver is saturation at the adiabatic saturation
temperature of the entering air. For state 2 that is
$t^{*}=51.00\,{}^{\circ}\text{F}$, at which $W^{*}=55.52\ \text{gr/lb}$. The
efficiency is the fraction of that potential actually realised, and it may be
written either on humidity ratio or on temperature:
$$\eta_{\text{sat}}=\frac{W_3-W_2}{W^{*}-W_2}
=\frac{50.48-38.59}{55.52-38.59}=0.704
\qquad
\eta_{\text{sat}}=\frac{t_2-t_3}{t_2-t^{*}}
=\frac{61.58-54.14}{61.58-51.00}=0.703$$
$$\eta_{\text{sat}}=\boxed{70.4\%}$$
The two forms agreeing to a tenth of a per cent is the check that states 2 and 3
really do lie on one wet-bulb line — a typical figure for a single bank of
sprays.
Part (d) — make-up water. The water the cabinet must
replace is exactly the moisture the air leaves with:
$$\dot m_w=\dot m_{da}\,(W_3-W_2)=32{,}625\,(0.007211-0.005513)
=\boxed{55.4\ \text{lb/h}}$$
which is $6.6$ US gal/h, or about $25\ \text{kg/h}$. Confirm the whole plant: the
two heaters supply $48{,}100+360{,}000=408{,}100\ \text{Btu/h}$, and the air gains
$\dot m_{da}(h_S-h_M)=408{,}900\ \text{Btu/h}$, of which
$800\ \text{Btu/h}$ arrived as the enthalpy of the spray water. The balance closes.
Part (b) — the winter cycle on the inch-pound chart. M→2 is sensible preheat, 2→3 runs up the wet-bulb line through the adiabatic washer, 3→S is the main heater, and S→R is the all-sensible room load line.
Check: assumptions declared under cover-page instruction 1.
(i) The stated air quantities are taken as standard-air volumes, so
$\dot m_{da}=4.5\dot V$ and the mixing ratio equals the volumetric ratio; this is the
convention behind the $1.10$, $0.68$ and $4.5$ coefficients the question implies.
(ii) The spray cabinet is adiabatic and the make-up water enters at the leaving air
temperature, which is what recirculating spray water does; taking the make-up at
mains temperature instead changes the preheater duty by well under $1\%$. (iii) Fan
and duct gains are neglected, so the state leaving the main heater is the state
entering the space. Note that the preheater duty is not a free choice here:
the stated main-heater rating of $360{,}000$ Btu/h closes the one degree of freedom
that otherwise exists between the two heaters.