Abstract:
This thesis presents an experimental investigation related to nucleate
pool boiling of saturated liquids from plain as well as copper coated mild steel
heating tubes of various thicknesses at atmospheric and subatmospheric
pressures. It also includes the effect of heat flux, pressure and coating
thickness on boiling heat transfer coefficient of various liquids on coated tube
surfaces. In addition, it prescribes a criterion for enhanced boiling of liquids on
copper coated tubes.
The experimentation includes saturated pool boiling of water, methanol
and isopropanol from an electrically heated horizontal mild steel tube having
18 mm I.D., 32 mm O.D. and 145 mm effective length. It has been coated with
copper by means of plasma spraying technique. Calibrated PTFE
(polytetrafluoroethylene) coated copper-constantan thermocouples of 30 gauge
have been used to measure tube surface and liquid temperatures.
Thermocouples have been positioned in wall thickness of heating tube at top-,
sides- and bottom- position to measure temperature of heating tube.
Thermocouple probes have been located outside superheated boundary layer
surrounding the tube corresponding to surface thermocouples' positions to
measure liquid bulk temperature. A digital multimeter has been used to
measure e.m.f. of thermocouples. Adequate precautions have been taken to
ensure radial flow of heat from heating surface to liquid pool and negligible heat
loss to surrounding. Experiments have been conducted by following standard
operating procedure which includes thermal stabilization of tube surface,
removal of dissolved air from liquid pool, attainment of steady state condition
and recording of power input, pressure and liquid and surface temperatures.
The reproducibility of experimental data has been checked by rotating the
heating tube surface and found no change in data. Heat flux has been
increased progressively from 15,670.20 to 43,151.57 W/m2 in six steps and
pressure from 23.02 to 98.68 kN/m2 in five steps. The thicknesses of copper
coating on mild steel tube surface have been 19, 26, 33, 41 and 60 |am. The
maximum uncertainty associated with average heat transfer coefficient has
Abstract
been found to be ± 3.98%. Thus, experimental data of this investigation have
been considered to be within acceptable tolerance limits.
Data analysis has shown surface temperature to increase from bottom to
side to top position of a plain heating tube for a given value of heat flux at
atmospheric and subatmospheric pressures. However, liquid temperature
remains uniformly constant irrespective of heat flux at a given pressure.
Further, local heat transfer coefficient, at a given circumferential position, has
been found to vary with heat flux according to power law relationship, hv oc q°7
for all the pressures of this investigation. Adimensional equation of the form:
hy = Cv q07p032 has been developed for all the boiling liquids where C is a
constant whose value depends upon circumferential position on heating tube,
its surface characteristics and boiling liquid. Average value of heat transfer
coefficient of a plain heating tube has been found to be related with heatflux by
the relationship, h oc q07. A dimensional equation for the boiling of all the
liquids: h = Ci q07p032 has been developed by the method of least squares
within a maximum error of ± 7% where Ct is a constant representing surfaceliquid
combination factor. Above equation has been reduced into a
nondimensional form: (hVhi*) = (p/p-,)032 to overcome the difficulty in the
estimation of constant, Ci owing to its improbable nature. This equation has
been tested against the experimental data of [4,10,23,32,99,100] for saturated
boiling of various liquids on heating surfaces of differing characteristics at
various pressures and found to match excellently. Besides, it can also be used
to generate the value of heat transfer coefficient for boiling of liquids at
subatmospheric pressures without resorting to experimentation from the
knowledge of experimentally-determined values of heat transfer coefficient at
atmospheric pressure only. Above correlation can also be used for examining
the consistency of experimental data of boiling heat transfer irrespective of
heating surface and boiling liquid involved. The experimental data for boiling of
liquids at pressures higher than one atmosphere could not be correlated by
above equation due to the fact that power law relationship between heat
transfer coefficient and heat flux, h <x q07 does not hold true for pressures
greater than one atmosphere.
Abstract
Experimental data on copper coated mild steel heating tubes for
saturated boiling of water, methanol and isopropanol at atmospheric and
subatmospheric pressures have been analysed and found to disobey power
law relationship, hocq07 which holds true usually for the boiling of liquids on a
plain surface. Instead, it is governed by the relationship, h<xqn where the value
of exponent, n depends upon coating thickness and boiling liquid. In fact, its
value is less than 0.7. Boiling of methanol and isopropanol have resulted
similar behaviour. Further, an increase in thickness of coating has lowered the
value of exponent of q for all the liquids of this investigation on coated surfaces.
But the value of exponent for water has always been found to remain more
than that of methanol and isopropanol. The value of exponent, n for methanol
and isopropanol has been found to be identical for all the thicknesses of copper
coating. A dimensional correlation relating heat transfer coefficient with heat
flux and pressure for saturated boiling of a liquid on a mild steel tube coated
with copper of a given thickness has been obtained by least squares method in
the following form: h = C2 qxpy where the value of constant, C2 and exponents, x
and y depend upon liquid, heating surface characteristics and thickness of
coating on heating tube surface.
Comparison of boiling characteristics on a coated tube with those on an
uncoated tube surface has shown significant enhancement in the value of heat
transfer coefficient for the boiling of all the liquids except that of a 60 ^m thick
coated heating surface. Heat transfer coefficient of a copper coated tube has
increased upto a certain value and thereafter decreased with increase in
thickness of coating. In fact, heat transfer coefficient of a thick coated surface
becomes even lower than that of an uncoated one for some values of heat flux.
As regards, the effect of pressure the behaviour is same. However, the region
of heat flux for which heat transfer coefficient of a thick coated surface may be
lower than that of an uncoated one at atmospheric pressure shrinks with
decrease in pressure and ultimately may vanish. These observations have
been consistently obtained for all the liquids -water, methanol and isopropanol.
The ratio of boiling heat transfer coefficient at top position to that at
bottom position of a coated tube surface has been found to be lower than that
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Abstract
of a plain heating tube surface subjected to same values of heat flux and
pressure. Hence, magnitude of thermal stress in coated tubes is likely to be
lower than that of plain tube. In view of above, employment of copper coating
on a mild steel heating tube surface for boiling of liquids is likely to enhance
heat transfer coefficient and reduce thermal stress to increase its service life.
Therefore, use of coating on a surface is advantageous from thermal as well as
material engineering point of view.
The thermal performance, %of a coated heating tube surface has been
evaluated by defining it as a ratio of heat transfer coefficient on a heating
surface coated with a given thickness of copper to that of an uncoated one for
the boiling of a liquid subjected to same value of heat flux and pressure. It is
related to heat flux and pressure by the following dimensional equation,
%= C3 qapp where constant, C3 and exponents, a and (3 depend upon heat flux,
pressure, boiling liquid and thickness of coating. Based upon the logic of ^>1
for the suitability of a surface, a criterion q'ap'p < C3 has been established for
enhanced boiling of a liquid on a mild steel heating tube surface coated with
copper of a given thickness. This criterion can be used to determine the range
of heat flux for enhanced boiling of liquids on a copper coated tube surface at a
given pressure. Alternatively, it can also be used to obtain the range of
pressure for enhanced boiling of liquids at a given value of heat flux.