Physical-Chemical Water Sampling

(Exercises for ZO 419/519 Laboratory)

Introduction

In this exercise, you will learn to use the instruments with which we will measure physical and chemical conditions in Yates Millpond.  Below you will find instructions for using each instrument correctly, and directions and formulas necessary to derive limnological information from the field data. You may be assigned to any of the devices or procedures when we are out on the pond, and the accuracy of class data will depend on your knowing the correct technique.

Be sure to record the manufacturer's name and model number of the instruments we use.  You will have to include this information in the methods section of your report on Falls Lake. The techniques described in this chapter do not have to be repeated in your methods section; simply reference this guide.

Collecting Surface and Deep Water Samples

We will use an "integrating euphotic zone sampler," which is simply a piece of pipe with a stopper to put in the upper end. The pipe is lowered vertically into the lake to the desired length  (depth of mixed layer), stoppered, and retrieved over a bucket marked "Surface." On deck, the contents are drained out into the bucket.

The name implies that this simple tube samples the euphotic zone directly, but the thickness of the euphotic zone varies between stations on one date, and between dates at one station. Usually it extends deeper than the depth sampled by the tube. A better name for the tube would be "surface water sampler."

We will use a Van Dorn water bottle mounted horizontally to collect deepwater samples.  Cock the two end stoppers open by attaching cable loops to the trigger pegs, then lower the sampler to a point 30-50 cm from the bottom. Locate this depth by raising the bottle after it contacts the sediments. Gently swing it back and forth for about 30 seconds to flush out any water taken in at shallower depths or mud picked up from the bottom, then send the "messenger" weight down the line to release the end stoppers. Retrieve the sampler and open one stopper to let the water drain into the "deep" bucket.

Van Dorn bottles have a spring valve and air vent which allow water to be transferred to a closed bottle without exposure to air, but most of our measurements are not affected by aeration, so we will not use this feature.

The surface water sample from each station is subsampled to measure pH, alkalinity, turbidity, phytoplankton identities, and chlorophyll and nutrient concentrations. The bottom water sample is subsampled to measure pH, alkalinity, turbidity, and nutrient concentrations.
 

Turbidity

Particles suspended in the water scatter light, causing turbidity. Some of the more common particles in Yates Millpond will be suspended clay, phytoplankton, zooplankton, and tiny pieces of detritus.

Turbidity is measured in nephelometric turbidity units (NTU) in a portable nephelometer, or turbidity meter. It measures the sideways scatter of light by particles suspended in water using a photoreceptor at right angles to a light source.

Before the first measurement, calibrate the instrument with the enclosed standard.  Polish and place the standard vial into the well and slowly rotate it until a minimum reading is obtained, then adjust the scale to 0.02 with the calibration knob.

Fill the screw-capped nephelometer cuvette with water from the lake, carefully wipe the outer surface dry and clean with an absorbent, lint-free cloth, and place it in the well. Allow the sample to stand for a minute or two to allow bubbles to dissipate and the largest particles to settle out before taking the reading. Slowly rotate the vial until you obtain the minimum reading, and record it.
 

pH

We will measure pH of water samples directly with a hand-held, field pH meter. Before taking measurements, calibrate the instrument with buffer at pH 7 using the small screwdriver.

Initial pH readings can be combined with alkalinity titration.  Rinse the probe thoroughly with water from the sample before taking a measurement. Immerse the end of the probe completely in a subsample and allow the meter to stabilize.  Record this first reading as the current sample's pH.

Typical pH in our local waters ranges widely, from above 10 in highly productive waters on warm, still days, to less than 6 in deep, anaerobic water during summer stratification.  Because our waters are poorly buffered, fluxes of CO2 associated with higher rates of photosynthesis and respiration can drive pH of surface water layers through a wide daily cycle.  pH in fresh samples can change rapidly if the water is aerated, allowing CO2 concentrations to equilibrate with the atmosphere. If you initially measure a pH of 9.0 in Yates Millpond surface water on a warm, still day, you should be able to watch it decline over several minutes as carbon dioxide diffuses into the water from air. Similarly, water from near the bottom at pH < 6.0 might gradually rise toward as excess (supersaturated) carbon dioxide diffuses out into the air.  Take initial pH measurements as soon as possible after collecting water samples and with a minimu o fstirring.  These changes in pH will not affect alkalinity, however.
 

Alkalinity

Alkalinity may be estimated by titrating with a pH meter in the sample. Pour 200 mL of lake water from each sample depth into a graduated beaker, record the initial pH and the initial level in the titration burette, then add the weak sulfuric acid (0.02 N) in small increments (1 drop at a time, about 0.05 mL) and observe the pH after each addition. If the initial pH is higher than 8.3, record the volume of acid needed to titrate the sample to or just below a pH of 8.3. Then continue to titrate until pH drops below 5.0, and record the total volume of acid used.

During the titration, pH will change very slowly until you pass 5.0, but then drop quickly with the addition of only a little more acid. Take note of the pH after each drop below 5.5 so you won't overshoot the end point. After you have done a sample or two, you may add about 75% of the expected acid volume quickly, then titrate to the endpoint more carefully.  In Yates Millpond, the endpoint should be reached after 2 - 9 mL of acid has been added.

For more precise estimates, you may use the "Gran titration" method. This method requires you to record the pH after each additional drop of acid throughout the titration. Calculate, for each drop of acid, the value of the index:

 F1 = [H+] x (Va + Vw)

    where,

F1 = a pH index
[H+] = molar concentration of hydrogen ion
Va = cumulative volume of acid added, and
Vw = volume of the initial lake water sample.


Convert pH to [H+] by taking 10-pH.  Plot Va versus F1 on logarithmic paper (or log F1 versus Va on linear graph paper).  The resulting curve should be horizontal at first, then beyond a point where the water's pH has dropped below 5, the line should bend upward and continue straight at that angle. Calculate the slope of the rising portion of the line and rearrange the formula for a straight line to calculate the value of X for Y = 0.

That X intercept is the exact volume of acid required to reach the end point.

From the sample volume (200 mL), the acid normality (20 meq L-1), and the mL of acid used to reach the final end point (including any acid necessary to titrate to pH 8.3), calculate alkalinity with the formula:

 AT = (Va x Na)/Vw
    where,

AT  = alkalinity, in milliequivalents per liter (meq L-1)
Va  =  volume of acid used to titrate to the endpoint in liters (calculate as mL/1000)
Na  =  normality of acid used in milliequivalents per liter (meq L-1)
Vw  =  volume of lake water titrated in liters
The value for alkalinity in meq L-1 may be converted to commonly used units of "mg CaCO3 L-1."  The molecular weight of calcium carbonate is about 100 and there are 2 equivalents per mole of this salt, so the conversion factor is 50. Multiply alkalinity in meq L-1 by 50 to obtain alkalinity in mg CaCO3 L-1. Remember, however, that simple acid titration does not determine how much, if any, of the alkalinity was actually accounted for by calcium compounds. Do not use this number as an estimate of actual calcium concentration in the water.
 

Measurements in the Pond

Light

We will measure light with a submarine photometer (or simply, light meter). The photoreceptor at the end of the lowering cable is fragile and expensive, so please protect it carefully from breakage when it is not in use. It is mounted on a frame and plugged into the data logger (a fancy meter) by a cable which is marked in depth intervals. The receptor is lowered into the water to the desired depth and light intensity is read directly from the data logger.

Take readings just below the water surface (0.05 m), then every 0.5 m to a maximum of 2.0 m. The meter is neither stable nor accurate at readings below about 25 micro-einst.

The photoreceptor is sensitive only to wavelengths which are absorbed and used by chlorophyll and other photosynthetic pigments, called "PAR" (Photosynthetically Active Radiation). Some limnologists still use foot-candles or lumens as units of light. Others prefer to convert units to the amount of energy, as calories or joules, per unit surface area (usually 1 cm2) and time (usually sec). Our meter gives data in micro-einsteins (micro-einst) cm-2 s-1, which is a measure of the photon flux adjusted for varying quantum energies of photons at different wave frequencies.

Calculating the Extinction Coefficient

For your Yates Millpond data report, you must calculate extinction coefficients from the light intensity data. The most practical form of the equation for this index is:

 e = (lnI0 - lnIz)/z
   where,

e = the extinction coefficient
I0 = light intensity at a shallower depth (micro-einst cm-2 s-1)
Iz = light intensity at a greater depth, and
z  = depth interval between shallower and deeper measurements (m)
The higher the extinction coefficient, the more rapidly light is attenuated in the lake. Much of the excess of light attenuation over that caused by pure water is due to suspended clay in our area.

Secchi Disk Visibility

This is a measure of the depth to which an observer can see through water, measured with a Secchi disk. A black and white plate is lowered slowly into the water on the shaded side of the boat. When it just disappears, the depth is noted. Then it is lowered a bit further and retrieved slowly until it just reappears, and again the depth is noted. The average of these two depths is the Secchi disk visibility depth.

Although the Secchi is a generally reliable and widely used method of measurement of light attenuation, several errors and technical problems must be considered.  People differ in visual acuity, so some variation is inevitable with so many different people taking measurements. Reflection of light off the surface interferes with ability to see the disk. This effect is worst in full sunlight and when the sun is at low angles.  For greatest repeatability, readings should be made between 10:00 a.m. and 2:00 p.m., local standard time, and be made in shadow.

Oxygen, Temperature and Conductivity

These three are especially important environmental variables in general limnology.  They provide a wealth of information about environmental gradients and boundaries, chemical and physical conditions in the water, and even the activity of primary producers and decomposers in limnetic communities.  Fortunately, they may be measured quickly and conveniently with a single instrument, the OCT meter. These three factors may be used to define conditions of stratification in the lake.

In use, the probe of the meter is lowered to the surface (0.05 m), 0.25 m, 0.5 m, 0.75 m, 1.0 m, then at 0.5 meter intervals to the bottom.  Readings for temperature, specific conductance (the second of the sequential conductivity readings on the YSI Model 85 meter we are using), oxygen concentration, and oxygen % saturation are recorded at each depth.

Temperature Measurements

Temperature is read directly from the display, and should be recorded for each depth in units of degrees Celsius (= centigrade) to the nearest 0.1 C. Temperature readings should be taken first, before you start swinging the probe.

Oxygen Measurements

Oxygen concentration should be recorded for each depth in units of mg L-1 (same as ppm). To take accurate oxygen measurements, you must keep water moving steadily across the probe tip. Sweep it smoothly back and forth as you take each reading until a maximum, stable value is observed.

The oxygen probe takes about 15 minutes to reach electrical equilibrium after it is turned on, so turn on the meter a little while before you plan to take measurements in the pond.

The oxygen reading will quickly drop to 0 when the probe hits bottom, but also when the probe passes into an anaerobic  water layer. Learn to tell the difference when the line goes slack and the probe has hit bottom.

Oxygen Saturation Values

The % oxygen saturation combines the oxygen concentration and the absolute solubility of oxygen at a particular water temperature.

 %  = ([O2]/[Osat]) x 100
     where,

%    = percent saturation
[O2] = observed oxygen concentration, and
[Osat] = saturated concentration of oxygen at the local temperature at sea level.
Saturation levels indicate how much biological processes have affected the water recently. At the beginning of summer stratification, or perhaps even during the previous night, oxygen concentrations at mixed depths were exactly saturated, that is, in equilibrium with the air. Water just at the surface of lakes should be at or close to 100% saturation because exchange of oxygen with the air by diffusion and wave turbulence usually occurs at a faster rate than photosynthesis or respiration. However, in enriched or contaminated lakes, changes due to biological activity may exceed physical exchange rates even at the surface, and saturation levels may be much higher or lower than 100% at any depth, even near the surface. Supersaturation is frequently observed near the surface of Yates Millpond on hot, still days.

The OCT meter calculates % saturation of oxygen for you. The only potential error comes from variations in air pressure at the lake surface, which can change under the influence of weather systems and altitude. Yates Millpond's surface altitude is about 75 m, which, on the average, requires a correction in the value for 100% oxygen saturation by  - 0.1 mg L-1. The most precise % saturation values require detailed information on barometric pressure at the time of measurement. We will not go to that effort, since the important patterns are apparent without the greater accuracy.

Salinities in the brackish range (> 0.5 g L-1) also decrease oxygen's solubility, but Yates Millpond is completely freshwater, not brackish.  You must take that into consideration if you are measuring estuarine or marine waters.

Specific Conductance

Specific conductance is a measure of the ability of the water to carry an electric current, which is determined by the combined concentration of all electrolytic ions in solution. Horne and Goldman (1994) neglect it, but it has its limnological uses. The OCT meter gives uncorrected conductivity and specific conductance in sequence as the down arrow is pressed. Specific conductance is adjusted for the effects of temperature. Adjustment is necessary for comparisons because less current passes at lower temperatures, even if electrolyte concentrations are the same.

Units of specific conductance are mSiemens, which is similar to the unit formerly used in the United States, micro-mho cm-1. Our local surface waters have relatively low conductivity (45 - 90 micro-S) , but higher values can occur when waste effluents, groundwater, or salts dissolved from sediments are present.

Salinity is the weight of inorganic salts in solution. In the oceans, the composition of salts is constant in proportion, and changes in salinity apply proportionally to all component salts. This allows oceanographers to make a simple conversion from specific conductance to salinity. But a direct conversion is not possible in inland waters because many different ions can occur in widely varying proportions.  For that reason, salinity is rarely reported for fresh or non-estuarine, brackish waters.

Near the sediments biological processes indirectly have a major effect on specific conductance. First, CO2 from bacterial respiration at the mud surface builds up, lowering pH and dissolving carbonates from the sediments which increase both conductance and alkalinity. Then, when oxygen is entirely depleted by microbial respiration and anaerobic bacteria take over, major chemical changes begin to occur. Iron, manganese, and other metals are reduced and become more soluble. You may expect to see higher specific conductances as the probe nears the bottom, and highest specific conductances where there is no oxygen in the water near the mud.


Useful Methodological References:

Lind, O. T. 1979. Handbook of Common Methods in Limnology. The C.V. Mosby Company, New York. 199 p.

Wetzel, R. G. and G. E. Likens. 1989. Limnological Analysis. Saunders Publ. Co., New York. 357 p.


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Maintained by Sam Mozley, s_mozley@ncsu.edu.

Last modified on August 7, 2002