• No results found

69 occ urring, after collection and before analysis, if

the carbon dioxide gas in the sample is substantially above or below the air equilibrium value. Errors in

the field measurement may also be caused by the

inferior equipment used.

Therefore, to eliminate these two main sources of

error in pH measurement, samples were collected and taken quickly to a field laboratory for determination on a good quality pH meter. For particular studies in the changes in pH of a given loch water the same pH meter was set up at the loch side using a portable petrol-powered generator for a power supply.

Method The samples of loch water were collected in

500 ml screw-cap jars under water, sealed to exclude

air bubbles and to prevent gaseous exchange with the atmosphere. These samples were then taken to the field,

laboratory and analysed immediately. Samples could be

collected from any location on the loch surface or up to any depth colonised by macrophytes by means of aqualung diving.

An aliquot of this sample was taken and titrated against 0«02M HC1 standard acid. This acid was freshly

made up using distilled water that had been boiled for

at least an hour and cooled with a soda lime tube to prevent any reabsorption of carbon dioxide. The

apparatus used to perform the titration is shown in

Acid/ reservoir •-Burette Electrode pH Meter Magnetic stirrer Figure 3•8

The apparatus set up in the field laboratory for

titration of loch water samples* The burette is refilled between titrations directly from the acid reservoir, the soda-lime tubes preventing entry of carbon dioxide to the system. The magnetic stirrer kept the contents of the flask mixed during the titration.

70

burette to be filled from the standard HC1 reservoir

without allowing any absorption of carbon dioxide

from the atmosphere. Thus, when the apparatus was set up many samples could be analysed rapidly and in

succession.

The magnetic follower in the titration flask

ensured that the acid added was mixed rapidly and that the pH electrode read correctly. The individual

titrations were carried out as quickly as possible to prevent exchange between atmospheric carbon dioxide and the contents of the flask becoming significant. The samples were first taken to an end point of pH 8»3, if already above this, and then titrated to an approx­ imate end point of about pH 5*0. An approximate value of T.A. was then calculated and knowing the initial pH

and conductivity range of the sample the approximate

total carbonic acid was calculated using Tables 11.1 and 11.2 in Appendix II after Colterman (1969). The true end point pH is then read off Table 11.3 and the

sample titration•continued to this. The volume of

standard acid required to get to this end point gives

the T.A. The total, carbonic acid is also calculated.

Results Samples were taken from four limestone lochs (L. Borralie, L. Caladail, L. Croispol and L, Lanlish) and from one peat loch (L. Meadie) in the area studied in Durness. Samples were collected at various locat­ ions and depths corresponding to the range of veget­ ation present. One such set of results for these lochs /

is given in Table 3.9. The values of pH, total

alkalinity and total carbon dioxide of the four lime­

stone lochs are similar and in contrast to the non limestone loch. The pH and T.A. values of the lime­ stone lochs show that although these waters have a high total carbon dioxide, there will only be a small amount of this present as free carbon dioxide. This will be biologically significant ranging from several times the atmospheric concentration around pH 8 to several times less at ph 9,

Table 3*9

Analysis of water samples from selected lochs in the Durness area in May 1973» The total^ alkalinity and the total carbon dioxide are given in units of m.eq*!*”^»

Borralie Caladail Croispol Lanlish Meadie

pH 8.66 8*72 8*37 8.34 7*14

TA. 2.33 3.02 . 3.44 2 .3 6 0.012

3.3 Dissolved Carbon Dioxide

All dissolved'gases are held in solution by their

respective partial pressures in the gas phase assoc­ iated with the liquid phase (Henry’s law). Therefore, when carbon dioxide partitions itself between the gas

and liquid phases, by diffusion, the amount in solution

will be in equilibrium with the partial pressure (pCOg)

in the gas phase* Thus, the solubility coefficient

will be defined as

Dissolved CO^ (moles l”^) = pCOg .

However it will now be important to make the distinct­ ion between dissolved carbon dioxide gas and hydrated

carbon dioxide as in equation 2. The gas solubility

law will apply only to the dissolved gas.

Although there are seasonal changes in the con­

centration of carbon dioxide in the atmosphere (Bisch- off, 1960), for the purpose of the present study it is reasonable to consider the atmospheric partial pressure of carbon dioxide above a loch water to be constant.

The solubility will be temperature dependent and the

variation of the solubility coefficient with tempera­ ture is given in Figure 3.10.

Photosynthesis and respiration by aquatic plants

will cause fluctuations in the dissolved carbon dioxide and total carbonic acid of the loch water. The diss­

olved carbon dioxide changes will cause a displacement

moles/l,/Atm, xlO' 700 600 500 4oo 3500 8 4 12 16 20 o Figure 3,10

The variation of the solubility coeficient of carbon dioxide in water with temperature, (Drawn from data given in Riley and Chester, 1972,) The solubility coeficient is given

from: ■ Cone, dissolved C0_ Partial pressure CO^

C-raoles/li

equilibria. The magnitude of the shift of equilibria will be related to the 'pCOg* buffering capacity of a water type for changes in total carbonic acid

(Kanuisher, 1963). The net effect of this will be that in a water of given alkalinity the change in the

dissolved carbon dioxide, that will occur for a given

change in total carbonic acid, will be less than that of distilled water. This difference in change of diss­ olved carbon dioxide will be related to the alkalinity of the loch water concerned. The difference in fpCOg* buffering capacity for waters of different alkalinity has been experimentally determined (Kanwisher 1960), Figure 3.11 shows this difference in tpCOg* buffering capacity for fresh distilled water and sea water, where the same change in total carbonic acid produces a much larger change of dissolved carbon dioxide in distilled water than sea water.

The higher the alkalinity the greater the ipCOg* buffering capacity and hence the dissolved carbon

dioxide increase or decrease will be partially absorbed, that is reduced to a smaller change than would occur in distilled water. The remaining difference between the dissolved carbon dioxide and tpCOg,* of the atmos­

phere will be equilibrated by net diffusion through the

gas-liquid phase interface. It can be shown that the

exchange between gaseous carbon dioxide and water may

be slow compared to other gases such as oxygen. Thus, a dissolved oxygen deficit is more quickly replaced by

pCO^ Difference between air and water in atmospheres X 10^ 4000 Fresh water 2000 1000 Sea •wa 1 2

ml/Litre CO^ added to water

The experimentally determined partial pressure variation of carbon dioxide with changes in total carbon dioxide in sea and fresh water. From Kanwisher (i9 6 0)

diffusion from the gas phase than a carbon dioxide deficit. This is mainly due to the vastly different partial pressures of oxygen and carbon dioxide in the atmosphere rather than a significant difference in the diffusion of oxygen and carbon dioxide in water. The

wind velocity and associated turbulence of the water

surface have been shown to increase the movement of carbon dioxide across the air-water boundary

(Kanwisher, 1962, 1963).

Thus, as the return to equilibrium of carbon dioxide between the gas and liquid phase will be diffusion limited in the liquid phase, it will be slow. Differences between dissolved and gaseous

carbon dioxide caused by biological activity, ip water, may persist for several months (Teal and Kanuisher,

1965; Tailing, 1976).

The following investigations were undertaken to

measure the extent of pH changes in water bodies due to a net removal of carbon dioxide by photosynthetis activity of macrophytes.

To Demonstrate that an Aquatic Macroohyte will remove

Dissolved carbon dioxide from Pond Water faster than

the diffusive supply from the Atmosphere

Method A glass tank (18" x 12" x 24") containing

growing P. perfoliatus plants collected from L. Croispol

and rooted in soil, was placed in the laboratory window

where it would receive sunlight during the day, A pH

75

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