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Florida Scientist:
Quarterly Journal of the Florida Academy of Sciences
Vol. 50 Spring, 1987 No. 2
Gaseous Fluoride Emissions from Gypsum Settling and Cooling Ponds
Howard E. Moore
Department of Chemistry, Florida International University, Miami,
FL 33199
ABSTRACT: Previous estimates
of hydrogen fluoride fluxes from cooling and gypsum settling ponds
associated with the manufacture of phosphate fertilizer are reviewed
and a theoretical estimate based on vapor pressures of HF-H2O solutions
is presented. The latter yields fluxes from 122 to 195 kg HF/day for
a 450 metric ton P2O5/day plant. Sixty percent or more of
the total plant release of HF is due to the ponds. Derived atmospheric
residence times for HF (1 to 5 hr.) indicate that fluoride is dispersed
throughout Central Florida at ppb levels in particulate form and may
be an environmental hazard to adjacent agricultural industry.
The primary purpose of this paper is
to give a brief review of the literature relating to the emissions
of fluorides, i.e., hydrogen fluoride and silicon tetrafluoride, from
gypsum settling ponds and cooling ponds associated with phosphate
fertilizer production in Central Florida (Fig. 1). A theoretical estimate
of these emissions is presented for comparison to experimentally determined
values. An excellent review of atmospheric fluoride emissions and
the effect of fluoride on plants and animals was compiled by the National
Research Council, National Academy of Sciences (NAS, 1971). A study
of emission control practices in the phosphate industry was published
by the Department of Health Education and Welfare (Crane et al., 1970).
Based upon data obtained by Crane and coworkers (1970), the National
Academy of Science study group (NAS, 1971) stated that vaporization
from the ponds may constitute 90% or more of the total fluoride emissions
to the atmosphere. In 1972, emission control regulations were promulgated
in Florida for all phosphate production operations except the ponds
(State of Florida, 1985). As a consequence of recognition by the industry
that fluorides are hazardous to workers and in response to these regulations,
fluorides that were formerly allowed to escape to the atmosphere in
the operations are now efficiently trapped and conveyed to the settling
and cooling ponds, where their ultimate fate is largely unknown (State
of Florida, 1983). It now appears probable that these ponds contribute
a large majority of the overall fluoride emissions from the phosphate
industry to the atmosphere. The fate of fluorides in the atmosphere
is poorly known. They may have injurious effects on the various agricultural
industries adjacent to phosphate mining areas. This is discussed further
below.
PHOSPHATE FERTILIZER PRODUCTION - Sauchelli (1960) stated that, despite
the more-than-a-century period in which superphosphate has been manufactured
in all parts of the world, the chemistry of the acidulation reaction
is still not precisely known. This is still true to some extent today.
The composition of Florida pebble phosphate is given in Table 1 (Sauchelli,
1960). The main component in the phosphate ore is fluorapatite, 3[Ca3,(PO4)2]*CaF2.
The ore appears to contain excess fluoride as CaF2 or as fluorosilicates.
The important reactions in the process appear to be as follows (Sauchelli,
1960):
(1) 3[Ca3(PO4)2] CaF2 + 10H2SO4 >
6H3PO4 + 10CaSO4 + 2HF
(2) H2SO4 + CaF2 > CaSO4 + 2HF
(3) 4HF + SiO2 > SiF4 + 2H2O
(4) 4H3PO4 + Ca3(PO4)2 > 3Ca(H4PO4)2
From these reactions, it appears most of the fluoride is released
as SiF4. This is passed through scrubbers and converted to fluosilicic
acid, H2SiF6 (Waggaman, 1969), (Eqn. 5).
(5) 3SiF4 + 4H2O > SiO2 2H20 + 2H2SiF6
A portion of the fluoride remains with
the superphosphate. This amount varies with the strength of the sulfuric
acid used and is from 25 to 50 percent of the fluoride originally
present (Sauchelli, 1960); Waggaman, 1969; Crane et al., 1970). The
remainder of the fluoride is transferred to the gypsum settling ponds.
Table 1: Composition
of Florida Pebble Phosphate
CaO --
46-50%
P2O5 -- 30-36%
CO2 -- 1.5-4.4%
F -- 3.3-4.4%
SiO2 -- 7.3-9.8%
Other Oxides -- 1.7-5.7%
H2O -- 0.3-2.6%
State of Florida (1985) emission standards,
which apply to the various steps in the manufacture of phosphate fertilizers,
allow for a total emission of 0.21 kg of fluoride per metric ton of
P2O5 produced. While there is probably no such thing as a typical
phosphate complex, a model plant is assumed (Cross and Ross, 1969)
that produces 450 metric tons of P2O5 per day and thus is allowed
to discharge to the atmosphere 95 kg of fluoride (State of Florida,
1985). As mentioned above, these regulations do not cover emissions
from the settling and cooling ponds. The model plant above has associated
with it 65 ha of settling ponds and 40 ha of cooling ponds. Measurements
by Schiff and coworkers (1981) show both types of ponds have similar
fluoride contents.
Sauchelli (1960) states that under certain conditions the fluosilicic
acid may decompose. Thus, the ponds may appear to be in a quasi-equilibrium
of the type:
2HF(aq) + SiF4(aq) = H2SiF6(aq)
H2SiF6(aq) = H+(aq) + HSiF6-(aq)
HF(aq) = HF(g)
SiF4(aq) = SiF4(g)
This is in accord with the fact that HF and SiF4 are found in the
vapor state over solutions of fluosilicic acid (Jacobsen, 1923) and
that fluosilicic acid cannot be isolated in the pure state (Colton,
1958). The ratio of HF to SiF4 in the gaseous state increases with
a decrease in fluosilicic acid concentration (Baur, 1903). The
concentrations of soluble fluoride in the ponds range from 4,000 to
14,000 ppm with value over 10,000 ppm being quite common (Cross
and Ross, 1969; Crane, 1970; Tatera, 1971. Schiff et al., 1981).
Most of the measured fluoride must exist as HF. Pond water analyses
are usually performed with a fluoride specific electrode on samples
that are either made basic or are highly diluted with water thus raising
the pH. Fluoride electrodes are not sensitive to combined fluoride
such as HF or SiF4, but are sensitive to OH- at pH greater than 8
(Skoog, 1985). Also, the ponds generally have pH values between 1.2
and 1.8 (Schiff et al., 1981). For a pond with 10,000 ppm soluble
fluoride and pH of 1.5, 98% of the fluoride exists as HF rather than
F (K for HF = 7.2 * 10-4 at 25 C; Weast, 1979). This analytical technique
and calculation gives no indication as to the concentration or volatility
of SiF4. "Surveillance is advisable (Crane et al., 1970)"
as, "the fate of the material is largely unknown (State of Florida,
1983)."
FLUORIDE FLUX ESTIMATES -- Three previous estimates of fluoride emissions
from ponds, which are based on experimental measurements of atmospheric
HF over ponds, have been made. Crane and Ross (1969) installed a "greenhouse"
with a stack and exhaust fan directly on a settling pond. They then
pulled air through the assembly at a rate which gave concentration
values in the enclosure equal to those on the bank adjacent to the
pond. They then estimated the emission rate to be 11.8 kg/day for
65 ha pond. The 40 ha cooling pond would be expected to add 7.3 kg/day
for a total of 19.1 kg/day. Crane and Ross stated that they thought
these to be minimum emission values.
Crane and coworkers (1970) reported on a similar experiment in which
air was drawn at a known rate through an enclosure over a twenty foot
long air, gypsum-pond water interface. The values obtained were shown
to be temperature dependent and ranged from 0.56 kg/ha day at 50 C
to approximately 2.8 kg/ha day at 80 C. For the example above these
would lead to 59 to 294 kg/day. Crane and coworkers (1970) state that
they do not believe the air reached its ultimate saturation value
and that the values are low. The water as it enters the pond may be
at somewhat higher temperatures initially, thus fluxes may be much
higher than over the pond as a whole.
Tatera (1970) made measurements on pond water that was transported
to a laboratory where studies were conducted in a wind tunnel. He
also could vary wind speed and temperature. He determined emission
rates could vary from 0.36 to 20.5 kg/ha day, the actual emission
rate being very dependent on temperature and wind speed and less dependent
on fluoride content of the pond water. He also stated that other mechanisms
such as perculation and photochemical reactions must account for additional
emissions of fluorides to the atmosphere. Measurements by Tatera (1970)
yielded 12.1 kg/ha day for a typical pond. This would result in 1270
kg/day emission from the ponds in the example above.
Grant (1984) stated that about 100 kg of fluoride are produced per
metric ton of P2O5. Thus for a 450 metric ton/day plant, 45,000 kg
of fluoride would be processed and 1270 kg would be only a 2.8% release
to the atmosphere. These authors believe their fluxes to be the minimums
and because they vary so widely, an independent method of estimation
seems appropriate.
Very approximate estimates of the fluoride flux from gypsum ponds
can be made on the basis of HF vapor pressures over HF-H20 solutions
and H2O evaporation rates along with a consideration of atmospheric
conditions. The use of HF vapor pressures from HF solutions rather
than fluorisilicic acid solutions appears as the concentration of
HF in the pond waters is measured by the fluoride specific electrode
as mentioned above.
VAPOR PRESSURE OF HYDROGEN FLUORIDE SOLUTIONS -- The vapor pressure
of water and hydrogen fluoride over pure hydrogen fluoride solutions
has been measured by Fredenhagen and Wellman (1932); Khaidukou and
coworkers (1936); Brosheer and coworkers (1947) and Munter and coworkers
(1949). The best data at lower concentrations appear to be those given
by Brosheer and coworkers (1947). These data are given in Fig. 2 and
3 for temperatures of 25 C. Tatera (1971) also has given data, but
his values appear low.
Waters in the settling and cooling ponds are saturated with several
calcium salts and hence are not pure HF-H2O solutions. However considering
them as pure solutions the mole fraction of HF corresponding to 10,000
ppm fluoride is 0.010. Addition of other solutes will tend to reduce
the mole fraction of HF, but to what extent is not certain. More important
may be the nature of the solutes and the pH of the solutions. As mentioned
above, at a pH of 2 or below most of the fluoride will be in the form
of HF and not F-. Molecular HF is volatile while F- is not. Other
solutes in the pond may cause a salting-out effect and increase the
vapor pressure of HF over the ponds. Field measurements of the vapor
pressure of HF over the actual cooling and settling ponds need to
be made.
The vapor pressure of water above the cooling and settling ponds will
be effected by the same factors as for hydrogen fluoride. The biggest
variable in determining both vapor pressures may be temperature as
shown (Fig. 2 and 3).
WATER EVAPORATION RATES -- The flux of hydrogen fluoride to the atmosphere
can be estimated from the evaporation rate of water and the vapor
pressures of hydrogen fluoride and water (MacKay and Walkoff, 1973).
The estimation of evaporation rates is not an easy task (Chow, 1964).
The evaporation rate of water depends on the temperature of the water
and air, wind velocity, atmospheric pressure, chemical purity of the
water, and the depth of the water body.
Evaporation rates can be estimated in several ways. The two most common
methods are from averages of evaporation as determined by evaporation
pans and from evaporation equations based on modifications of Dalton's
law.
The most commonly used pan is the U.S. Weather Bureau Class A Land
Pan (Chow, 1964). Evaporation rates using this pan have been published
by the Weather Bureau (Kohler et al., 1955). True evaporation rates
for open ponds and shallow lakes are generally about 0.70 of the pan
value. Evaporation rates depend upon the depth of the pond or lake.
Deeper lakes have lower evaporation rates. Also the evaporation rate
decreases as the salinity increases. About 1 percent decrease in the
evaporation occurs with 1 percent increase in specific gravity. The
evaporation rate occurs with 1 percent increase in specific gravity.
The evaporation rate of ocean water is thus 2-3 percent lower than
fresh water. This may have a decided effect on estimates of evaporation
from settling ponds, but may be offset by the shallow depth of these
ponds.
Evaporation rates derived from pan measurements are 152-165 cm/yr
for Central Florida. Actual measurements on lakes are given as 122-132
cm/yr. The 0.70 factor applied to the pan values yields 114 cm/yr
or 0.31 cm/day. No correction is made for the salinity of the ponds.
Evaporation rates for shallow ponds and lakes can also be determined
from a Dalton's law type equation given by Rohwer (1933):
(10) E = 1.958 {(1.465-0.0186B)
(0.44 + 0.190W) [exp Pw/Pa)]}
where B is the barometric pressure, W
is the wind velocity, and Pw an Pa are the saturation and actual water
vapor pressures. B, Pw, and Pa are in Torr, W is in km/hr, and E in
cm/da.
Schiff and coworkers (1981) give a wind speed of 19.6 km/hr, an air
temperature of 85 C and a relative humidity of 95 percent during the
times when they were sampling. Using these values (Eqn. 10) gives
an evaporation rate of 0.174 cm/da or about half of that estimated
from pan values.
The flux of gaseous HF to the atmosphere from the pond may not follow
the evaporation rate of water exactly. If equilibrium for both HF
and H2O is reached and the air mass over the pond is exchanged with
surrounding air, the replacement air may have a high humidity, thus
suppressing the evaporation rate of water, but be void of HF. Under
these conditions the HF would continue to escape to the atmosphere
and the HF flux would be greater than estimated from the evaporation
rate of water. Since no information is available, the calculations
which follow do not consider salinity or exchange of air over the
pond with high humidity air which is void of HF.
ATMOSPHERIC FLUXES OF HYDROGEN FLUORIDE -- The flux of HF from the
surface of the pond, F, is given by:
(11) F = E[(PM)HF/(PM)W]
where E is the evaporation rate of water.
P and M are the saturation vapor pressures and molecular weights of
HF and water. The vapor pressures are both temperature and concentration
dependent as shown above in Figures 2 and 3. However, the ratio of
vapor pressures is less dependent on temperatures, so the effect of
temperature on the flux is largely governed by the change in evaporation
rate with temperature.
Using a value of 10,000 ppm HF for a
gypsum settling pond (Schiff et al., 1981), the vapor pressures of
water and hydrogen fluoride are 23.48 and 0.024 Torr at 25 C. Introducing
the evaporation rates calculated above leads to fluxes at 2.1 x 10-4g/m2
min (pan evaporation) and 1.3 x 10-4 g/m2 min (Dalton's law equation).
Using vapor pressure values at 40 C gives similar values. A summary
of flux values is given in Table 2.
TABLE 2: Summary
of HF Flux Data for a 105 Hectare Pond
Cross and Ross (1969)
- 19 HF, kg/day
Crane et al. (1970) - 59-294 HF, kg/day
Tatera (1970) - 38-2140 HF, kg/day
Present Estimate - 123-195 HF, kg/day
ATMOSPHERIC CONCENTRATIONS OF HF -- Surface
air concentrations may be related to the flux by (Crank, 1956):
(12) C = F/(DA)1/2
where D is the turbulent diffusion coefficient
and A is the removal rate of HF from the atmosphere. The mean residence
time or the time to remove 1/e of a species from the atmosphere is
given by T = 1/A. Eqn 12 assumes a uniform flux over an infinite horizontal
plane. This may not be applicable in the strict sense as the ponds
have finite areas and replacement air may be void of HF as mentioned
above. However, Eqn 12 should provide some insight into the residence
time of HF as related to air concentrations near the settling ponds.
Values of D vary with altitude and generally
range from zero at the ground to 1200 m2/min in the open troposphere
(Jacobi and Andre, 1963; Ikebe and Shimo, 1972). With a wind speed
of 20 km/hr over open land at 1 m altitude, D has an approximate value
of 12 m2/min.
The value of the atmospheric residence time for HF has not been determined.
It must be very short as HF is a very reactive gas and will undergo
deposition on plant and other surfaces including aerosols in the atmosphere.
An estimate of the value of T can be obtained from measured values
of HF near the ponds through the use of Eqn 12. Schiff et al. (1981)
found atmospheric concentrations ranging from 20 to 60 ppb. Earlier
values ranged from 0 to 170 ppb (Hendrickson, 1961; Huffstutler and
Starnes, 1970). If a value of 60 ppb (50 ug/m3 is assumed, calculated
values for T, range from 0.5 min to 2.2 hr.
Data on gaseous HNO3, a similar compound, is available for comparison.
Parrish and coworkers (1936) measured particulate NO3 along with gaseous
HNO3, NO, and NO2 in a non-urban site west of Boulder, CO. Based on
their measurements, they concluded that most of the gaseous HNO3 is
removed by deposition rather than by attachment to aerosols and subsequent
rainout or washout. A T for gaseous HNO3 was estimated to be between
17.5 and 8.8 hr for the winter and summer months, respectively. The
shorter residence time corresponds to more humid conditions in the
Rocky Mountains.
Jacob and coworkers (1986) studied the
H2SO4 - HNO3 - NH3 system at high humidities and in fogs. They concluded
that the residence time of gaseous HNO3 was less than 12 hr. They
developed a stirred-tank model to explain their experimental values
and adopted a deposition velocity for gaseous HNO3 of 3 cm/s. Measurements
of the deposition velocity in clear air over a grass field in Central
Illinois yielded a mean value of 2.5% + 0.9 cm/s (Huebert and Robert,
1985). Deposition velocity is related to residence time by
(13) I/T = (v/h) + Aa + Kc
where v is the deposition velocity, h
is the atmospheric mixing height, Aa is the removal rate by aerosol
attachment and kc is the removal rate by chemical processes. The latter
is important for HNO3, but not for HF as gaseous HNO3 undergoes photolysis
while HF does not.
Residence times calculated from deposition
velocities are very dependent on the atmospheric mixing height. Parrish
and coworkers (1986) assumed a mixing height of 1100 m, while Jacob
and coworkers (1986) assumed 400 m. These appear to be typical values
except under extremely stable conditions when the mixing height may
be on the order of 100 m (Wallace and Hobbs, 1977). Values of 300
and 1000 m for the mixing height combined with the data of Huebert
and Robert (1985) yield 3.3 and 11 hr, respectively, for T, for gaseous
HNO3. Aerosol attachment should result in even shorter residence times
as indicated by Eqn 13.
Attachment reactions for ions to particles
in the atmosphere with diameters less than 0.1 um is quite rapid.
For Rn-222 daughters the attachment rate has a T, corresponding to
0.33 t5o 1.85 min. (Porstendorfer and Mercer, 1980). Once formed,
aerosol particles undergo coagulation until they reach a radius of
approximately an hour (Nakatani, 1980). The attachment of HF to aerosols
may be somewhat slower as attachment in the case of HF depends upon
having sufficient NH3 to partially neutralize the acid. HF would not
be expected to attach to a highly acidic sulfate particle, however,
if attachment rates are similar to deposition rates then T for HF,
assuming it is similar to HNO3, would vary from 1.2 to 5.5 hours.
Best estimates of T for gaseous HF thus appear to be on the order
of 1 to 5 hours.
Once attached to aerosols, fluoride will
have a residence time corresponding to the residence time of the aerosols.
Based on Rn-222 daughter measurements, Moore and coworkers (1973;
1980) calculated mean residence time for atmospheric aerosols of about
5 days. Based on a long range transport model for sulfate over the
Eastern United States, Kleinman (1983) estimated a residence time
of 4.4 days. In the same model calculation, Kleinman (1983) found
the average distance from source to receptor for sulfate to be 583
km. Thus it appears most of the gaseous HF will be confined to the
region of emission, but particulate fluoride may be spread throughout
Central Florida. In Sarasota County, FL a mean of 0.14 ppb gaseous
fluoride has been determined in ambient air samples for the years
1980-1985; however, no data on particulate fluoride are available
for comparison (Sarasota County, 1985).
The above discussion gives no insight
into the flux or fate of SiF, in the atmosphere. It is a less reactive
gas which should have a longer residence time and be transported over
greater distances before reaction. This should be investigated further.
BIOLOGICAL EFFECTS OF FLUORIDE EXPOSURE -- In plants, exposure to
elevated fluoride concentrations is most evidenced by the development
of leaf margin and tip necrosis. Injury to plants at lower fluoride
levels may result in decreased plant dry weight, vigor, leaf size
and fruit quality and quantity. The threshold levels at which these
symptoms become evident is difficult to ascertain accurately. Possible
effects of citrus become of interest in Florida. While citrus, like
other species, exhibits a range of tolerances, threshold levels for
growth effects appears to be in the range of 50-100 ppm (dry weight)
on the leaves.
Concentrations on the leaves of plants can be related to atmospheric
concentration by:
ÆL=KCT
where ÆL is the increase in fluoride concentration on leaves above
normal background levels due to an atmospheric concentration, C, maintained
for time, T. K is the apparent accumulation rate factor. Accumulation
is not constant as implied by the equation but appears to decrease
with time. Thus exposure to high concentrations for short periods
of time may not have the same effect on exposures to lower concentrations
over longer periods of time. This is illustrated by the work of McCune
(1969) on citrus which indicates that exposure to 1-10 ppb fluoride
for 10-12 months will produce foliar markings as readily as exposure
to 5,000-10,000 ppb fluoride for 1 hour. McCune suggests an ambient
exposure limit of 1 ppb to prevent damage to citrus. Data by Brewer
and coworkers (1969) support these findings.
Also of interest is data on plants used as forage for cattle. Data
on orchard grass appears typical of other forage crops tested. The
work of Benedict and coworkers (1965) indicates a value of K equal
to 1.1 for orchard grass at fumigation levels of 0.6 to 0.9 ppb and
times ranging from 21 to 120 days. Thus orchard grass would accumulate
50 ppm fluoride in a month at ambient fluoride levels of 1.5 ppb.
Crippling skeletal fluorosis has been observed in cattle exposed to
high levels of fluoride (McClure, 1970). A concentration of 40 ppm
has been cited as an official allowable maximum of fluoride on plants
which are used as forage for cattle (Lewis, 1970). State of Florida
(1978) analyses on grass samples from Polk, Hillsborough, and Manatee
counties in Florida during the years 1976-78 show mean levels of 9
to 117 ppm for monthly samples. These levels must accumulate airborne
fluoride. The Peace River, which
flows through Polk, Hardee and Desoto Counties, FL was found to contain
46 ppm fluoride in 1961 (Waldbott, 1978). More recent samples run
in the author's laboratory showed 4.2 ppm at Bowling Green, FL and
from 30.5 to 48.5 ppm (11 samples) in the remainder of the river down
to Arcadia, FL. While these levels are equal to or above those considered
injurious to cattle, only two cases of crippling fluorosis in cattle
have been reported in Florida in recent years (State of Florida, 1986).
Ambient concentrations of atmospheric fluorides from the phosphate
production operations do not appear to be at levels which would be
injurious to humans at the present time. The 1 ppb level proposed
by McCune (1969) to protect citrus would be adequate for both livestock
and humans. The State of Florida does not presently have a standard
regulation on ambient fluoride levels in the atmosphere. Some insight
into what the level should be for the protection of humans can be
gained by comparison to levels for other atmospheric pollutants. Limits
for human exposure to several air contaminants are given in Table
4 (Weast, 1979) along with the State of Florida ambient standards.
The exposure limits are concentrations above which "exposures...shall
be avoided, or protective equipment shall be provided and used."
By comparison proposed ambient standards for protection of humans
would be in the range of (1) 0.3 ppm for 3 hours; (2) 0.06 ppm for
24 hours; and (3) 0.03 ppm annual mean. These regulations should apply
to a combined total of gaseous and particulate fluoride as they appear
to be equally injurious.
CONCLUSIONS -- Based on the evidence above, settling and cooling ponds
associated with phosphate fertilizer production account for 60% or
more of the total fluorides released to the atmosphere in the process.
The HF is rapidly attached to aerosol particles and may be dispersed
throughout Central Florida in the particulate form. These low levels
of fluoride can result in accumulations which may be injurious to
plants and animals. Several awards were given to farmers in suits
brought against aluminum refining plants for damage due to fluoride
emission during the period 1095-1962 (Waldbott et al., 1978). Waldbott
and coworkers also suggest that the decline in the cattle industry
in Florida from 1954 to 1965 was due to fluoride emissions from phosphate
plants.
More information is needed on the airborne concentrations of gaseous
and particulate fluorides in Central Florida. More information should
be gained on the chemistry of the ponds with the objective of seeking
a suitable way to lower fluoride fluxes. Liming is one obvious way
to lower fluxes but is too costly. Understanding the chemistry may
aid in developing less costly control methodology.
To learn more about the phosphate
industry, see www.fluoridealert.org/phosphate/overview.htm
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