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Oxygen Handbook Xylem Analytics Germany Sales GmbH & Co. KG, WTW Dr.-Karl-Slevogt-Straße 1 D-82362 Weilheim Germany Tel: +49 881 183-0 Fax: +49 881 183-420 Email: Info.WTW@Xyleminc.com Internet: www.WTW.com
More than 70 years of experience Dissolved oxygen is determined via a partial pressure measurement, with the oxygen dissolved in the liquid depending on the pressure of the gas found above the surface. In 1965 we were ready for serial pro- duction of sensors for measuring dissolved oxygen to the market with our WTW brand. Since then the measurement technology for this pa- rameter, which is decisive for the lives of flora and fauna in water among other things, has seen continuous development. Today we additionally offer optical dissolved oxygen sensors which facilitate precise measure- ments at lowest maintenance efforts and with highest precision. This handbook wants to give some understanding of the measurement technology by practical tips, support users and allow interested people learning about the principles of measurement. We are happy to be at your disposal at any time, just give us a call! Dr. Robert Reining and Ulrich Schwab (Directors of Xylem Analytics Germany GmbH)
Content SECTION 1 Fundamentals6 1.1 Dissolved Oxygen Sensors ��������������������������������������������������� 7 SECTION 2 Calibration and analytical quality assurance 11 2.1 Calibration ����������������������������������������������������������������������������� 11 2.1.1 Calibration in watervapor-saturated air �������������������� 11 2.1.2 Calibration in air-saturated water ������������������������������ 13 2.1.3 The calibration process in the measuring meter ����� 13 2.2 Sensor function check ��������������������������������������������������������� 14 2.2.1 Test in water-vaporsaturated air ��������������������������������� 15 2.2.2 Test in air-saturated water ������������������������������������������� 15 2.2.3 Test using zero solution ����������������������������������������������� 15 SECTION 3 Measurement and analytical quality assurance 17 3.1 Cleaning the sensor ������������������������������������������������������������� 17 3.2 Regenerating the sensor ����������������������������������������������������� 17 3.3 Unit and display of the measuring result �������������������������� 19 3.3.1 Display as a concentration value ������������������������������� 19 3.3.2 Display as oxygen saturation percentage ���������������� 19 3.4 Potential error sources ���������������������������������������������������� 20 3.4.1 Polarization times (running-in time) before measurement ���������������������������������������������������������������� 20 3.4.2 Drift check (AUTOREAD) �������������������������������������������� 20
3.4.3 Importance of flow ������������������������������������������������������ 20 3.4.4 Salt content correction ������������������������������������������������ 22 3.4.5 Impact of interferring gases ��������������������������������������� 22 3.4.6 Solubility function �������������������������������������������������������� 23 SECTION 4 Optical oxygen measurement 24 4.1 The principle of optical measurement ������������������������������ 24 4.2 Characteristics of the optical dissolved oxygen sensors ����������������������������������������������������������������������������������� 26 4.3 Calibration of optical dissolved oxygen sensors ������������� 27 4.4 Cleaning of optical dissolved oxygen sensors ����������������� 27 4.5 Impact of interferring gases ����������������������������������������������� 28 Bibliography29 Further handbooks 30 About us 31 Information around the clock! ��������������������������������������������������� 31
Oxygen Handbook SECTION 1 tial pressure in the further discus- sion. In dry atmospheric air the Fundamentals oxygen partial pressure is 20.95% of the barometric pressure. This Oxygen is not just a component percentage is reduced over a wa- of the air; it also appears in fluids ter surface because water vapor as a dissolved gas. An equilibrium also has a vapor pressure and state is then reached when the thus a partial pressure (Fig. 2). oxygen partial pressure, that is, the part of the overall pressure Under saturation conditions it fol- caused by the oxygen, is the same lows from above: in both air and fluid (Fig. 1). The pO2 (T) = 0,2095 · (pair - pW (T)) fluid is then oxygen-saturated. In relation to physical-chemical cor- rectness, it should be added that with as the oxygen partial the partial pressure in the fluid is pressure, pair as the barometric actually fugacity. The equating of pressure and as the water both values is, however, permissi- vapor pressure. highlights ble in the relevant pressure range temperature-dependent values. for the measurements, whereby In most cases however statements we can limit ourselves to the par- of oxygen concentration at O2 Dry Air above a O22 atmospheric air water surface O22 N2 Barometric pressure O2 O2 O2 CO2 Water vapor O2 Rare gases pressure Fig. 1 Principle of partial pressure Fig. 2 Air composition 6
are desirable. This is proportion- For water this effect plays a subor- ally linked to the oxygen partial dinate, negligible role. pressure and of course to the The effect of dissolved materials type of fluid, reflected by the Bun- is somewhat different. They can sen coefficient . both reduce and increase the solubility of oxygen. A salt content (sodium chloride) of one percent in water leads to a saturation con- with as the molar mass of the centration of 8.54 mg/L instead of oxygen and as the mole vol- 9.09 mg/L at 20°C. ume. For the measurement of the oxygen concentration the tem- Organic materials, on the other perature must be known. If the hand, normally increase the ab- result is desired in % saturation, sorption of oxygen into water. The the current barometric pressure is maximum saturation concentra- also required. tion increases with the proportion of the organic substance. Pure These comparisons demonstrate ethanol, for example, dissolves that water can dissolve more oxy- 40 mg/L of oxygen. gen at a high rate of barometric pressure than under low baromet- ric pressure conditions. 1.1 Dissolved oxygen sensors As the temperature rises the water vapor pressure rises, i.e. the oxygen partial pressure falls. To emphasize this impact here is a comparison between 20°C and 40°C at an barometric pressure of 1013 hPa. While at 20°C 9.09 mg/L of oxygen dissolves in water, at 40°C the amount is only 6.41 mg/l. The volume change linked with the temperature change depends Fig. 3 Cross-section through a on the fluid under examination. galvanic dissolved oxygen sensor 7
Oxygen Handbook The bases for the electrochemical following electrode reactions take determination of oxygen concen- place (Fig. 4). tration are membrane-covered Oxygen is reduced at the cath- electrochemical sensors. [1] The ode: main components of the sensor are the oxygen-permeable mem- O2 + 2 H2O + 4 e- → 4 OH- brane, the working electrode, the counter electrode, the electrolyte Here “the cathode supplies elec- solution and potentially a refer- trons” and the oxygen which has ence electrode (Fig 3). diffused through the membrane reacts with the water hydroxide Between the gold cathode and ions. anode, which is made from either lead or silver, there is a voltage Gold cathode that causes the oxygen to react electrochemically. The resulting e- - e- e- e e- e- current is higher, the higher the H2O + O2 OH- concentration of oxygen is. The measured parameter is the cur- Membrane rent in the sensor, which can be O2 converted into the concentration of the dissolved oxygen following Fig. 4 Principle of electrode reac- a calibration. If the anode is made tions from silver, the meter supplies the The electrode metal is oxidized at required voltage (amperometric the anode, whereby the electrons sensor). If the anode is made from required for the cathode reaction lead, it is a self-polarizing sen- are set free. The reactions that sor i.e. the voltage is created by take place are either the two electrodes in the sensor itself in the same way as a battery Ag → Ag+ + e- (galvanic sensor). The measuring or meter only evaluates the current. Pb → Pb2+ + 2 e- In the case of the electrochemi- cal determination of oxygen the 8
The equations of the anode reac- lead or silver coating, fouling is tions highlight the effect of the a biological coating of the gold electrolyte solution. The compo- cathode which would take place if nents of the electrolyte solution the ions were not captured. bind the metal ions that result Amperometric sensors can be from the anode reactions. operated as a three-electrode The electrolyte solutions must be cell with an additional silver/silver suitable for the type of electrode. bromide electrode. They no lon- The CellOx® 325 or StirrOx® G ger have any anode in the tradi- galvanic sensors require a ELY/G tional sense. One of the silver/sil- solution and amperometric ver bromide electrodes takes on sensors such as the TriOxmatic® the task of the counter electrode require a ELY/N solution. (current dissipation), and the other the task of an independent Ag+ + Br- → AgBr ↓ reference electrode. This is cur- or rentless and shows a fundamen- Pb2+ + 2 OH- → 2 Pb(OH)2 ↓ tally better potential constance Pb(OH)2 → PbO + H2O than a conventional electrode. The potential of the reference This is visually represented below electrode is determined by the for the silver electrode (Fig. 5): concentration of the bromide ions and correspondingly represents an ion-selective electrode. As a result the concentration of the electrolyte solution can be moni- tored, this being a further feature of this sensor type. For WTW® sensors this is carried out in the so-called AutoReg Function in the TriOxmatic® sensors for online Fig. 5 Anode reaction with the measurements. silver electrode The sensors’ polarization times are The resulting, sparingly soluble also different and must be main- substances also prevent the 9
Oxygen Handbook tained according to the operat- is constantly taking place, the ing instructions. The polarization electrolyte solution is also being time is the time which elapses used up when the sensor is not between connecting the sensor connected to the measurement and beginning of the measure- meter during rest times. It may ment. It corresponds to the run-in thus be the case that regeneration period required to gain a stable is required even when no mea- measured value. Following a refill surement has been carried out. and change of the sensor head The “battery is thereby consumed”. (see Regenerating Sensors) the The role of the sample tempera- new components contain an ture for oxygen measurement undefined percentage of oxygen stems from the temperature- which must first electrochemi- dependency of the different cally react. In addition a current variables (e.g. Bunsen absorption flows as result of the polarization coefficient) have been already of the electrodes. This current is mentioned in the equations at the comparable with the loading of a beginning. condenser. In addition, the oxygen perme- The polarization time does not, ability of the membrane is also however, just play a role following temperature-dependent. For this sensor regeneration. reason, except the external tem- As already explained the gal- perature sensor (sample tempera- vanic sensor is self-polarizing, i.e. ture!) a further one is required polarization continues even after and this is found in the sensor unplugging the sensor from the head. With these two temperature meter. As a result no waiting time values the meter is able to com- is required when reconnecting. pensate temperature in-flow to For amperometric sensors polar- the membrane’s oxygen perme- ization must be carried out for a ability (IMT Isothermic Membrane certain of time following every Temperature Compensation). unplugging (see the operating in- structions). This permanent stand- by is, however, linked to a slight disadvantage. As the polarization 10
SECTION 2 Calibration and analytical quality assurance 2.1 Calibration signal at the sensor zero point is less than the sensor’s resolution. Analogous to the pH measure- ment, a calibration must also Current be carried out for the dissolved Water-vapor- oxygen measurement at certain saturated air time intervals. The reason for this is the consumption of the electro- lyte solution in the sensor head Sensor zero point Oxygen concentration through the measurements, as it is clear from the previous electrode Fig. 6 Representation of linear cali- reactions. The ions of the electro- bration through two points lyte solution bond the resulting This is described as a zero-current metal ions, whereby the composi- free sensor. For the experimenter tion of the solution changes. The the calibration with WTW meters recommended calibration interval is then practically a one-point depends on the dissolved oxygen calibration. sensor used. Two weeks is suf- ficient for portable meters and The second point of the calibra- up to 2-3 months for stationary tion curve can be determined in WTW® dissolved oxygen sensors. different manners (Fig. 6). Every linear calibration function The reason for this is that in equi- is set through at least two points. librium state the oxygen partial In the case of a dissolved oxygen pressure is the same in fluid and measurement with WTW® me- in air. ters, one point is the straight line 2.1.1 Calibration in of the sensor’s zero point. At the water vapor saturated air absence of oxygen, the sensor This condition is met over a large surface of water, such as a lake or 11
Oxygen Handbook even the aeration tank of a waste- The water vapor partial pres- water treatment plant. sure is merely a function of temperature if air humidity is at 100%. In order to determine this value, the sensor is additionally equipped with a temperature measurement probe. Fig. 7 We provide specific air It is important that the user calibration vessels for laboratory ensures that there are no water measurements. droplets on the membrane. The calibration would then partly take The air’s oxygen partial pressure place in water. is calculated from the barometric pressure using the formula given above Electrolyte solution in sensor pO2 (T) = 0,2095 · (pair - pW (T)) Membrane Water-vapor In line with this relationship the saturated air current barometric pressure Fig. 8 Effect of water droplets on must be measured at the mea- the sensor membrane surement location (not the one Caution is therefore particularly based on sea level, as is the prac- recommended if the sensor has tice with weather forecasts). This been stored in the calibration ves- used to be carried out by users sel for a longer period of time and with a barometer or approximate- condensation droplets may have ly resolved via the input of the formed or fallen onto the mem- height above sea level. Modern brane. The membrane must be meters automatically determine checked before calibration in any the current pressure with an inte- case and, if necessary, dried with grated pressure sensor. a soft paper cloth (Fig. 8). 12
It is sufficient if the sponge in the The option of calibration in water OxiCal® is moist (Fig. 7). It should, vapor saturated air is supported however, never be wet. The user by every WTW® meter and is, should only moisten the sponge as indicated by the points given with distilled water and squeeze above, certainly to be preferred in it. The dampness is fully sufficient. comparison to a calibration in air- 2.1.2 Calibration in air- saturated water. It has also to be saturated water applied when working according to the Standard (ISO 5814). The water is vented until the oxygen partial pressure in water The relative, not the absolute and air is the same. However, this slope (as is the case for pH mea- method conceals some risks: suring meters) is displayed in % for the calibration result. • The barometric pressure in the ventilation hose is al- 2.1.3 The calibration ways a little greater than the process in the measuring normal barometric pressure meter and thus the water is always a The oxygen meter takes the elec- little over-saturated following trode signal (current!) and com- venting. pares it with the oxygen partial pressure, which is obtained using • The temperature in the water equation (1) for the current air decreases as a result of the conditions of barometric pres- venting (cooling by evapora- sure pair and temperature . The tion). meter thus obtains a slope that • If a temperature equalization allows measured currents to be is waited for, the water will be converted into the oxygen partial a little over-saturated. value . At the same time a comparison is made between the • The point of complete satura- actual measured value and the tion is hard to estimate. There average saturation current of the is the risk of under-saturation. electrode type following the refill • Oxygen-consuming substanc- (nominal current). The result rep- es lead to under-saturation resents the relative slope S. 13
Oxygen Handbook With reference to the average tion, there is the visual check and saturation current, slopes greater three characteristic measurement than 1.00 are also possible. A points. slope of 0.81 following a calibra- The gold cathode is examined tion means that the slope is 81% for the visual check. If it is no of the nominal value. It does not longer gold in color, but instead indicate anything about the preci- covered with lead or silver, the sion of the measurement, but sensor shows high values and rather is a reference for estimating is generally no longer free of a the remaining operating time, i.e. zero-current. A remedy to this the time until the next change of can be found through regenerat- the electrolyte solution is recom- ing the dissolved oxygen sen- mended. sor according to the operating This also applies to the mean- instructions. The gold cathode ing of the sensor symbols in the should be polished only using a display of the modern oxygen special, moistened polishing strip meters which evaluate the service with circular movements and little life of the sensor in the same way. pressure. Only this strip has to be used in any circumstances as a The calculation of the oxygen scratched and unpolished elec- concentration is correctly carried trode surface damages the sensor out with the internally stored and negatively affects the measur- absolute slope in nA/hPa. ing reliability. 2.2 Sensor function Caution: The anodes, regardless check of whether they are made from For pH measurements, calibration lead or silver, must not be pol- data offer a direct possibility to ished in any case. assess the quality of the measur- More comprehensive than the ing set-up of meter, electrode subjective, visual check is an and standard buffer solution. evaluation at the three special This is not possible for oxygen measurement points: measurement due to the relative slope. Nevertheless, in order to gain results from the sensor func- 14
1st in water vapor saturated air, This is also the initial reason for 2nd in air saturated water and which we succesfully looked for 3rd in oxygen free water. an alternative to the calibration in air-saturated water which was 2.2.1 Test in water vapor saturated air common beforehand. If no value is found in this tolerance interval, In water vapor saturated air the sensor should be sent to the should provide a value between plant to be checked. 100 and 104% oxygen satura- tion. If the values are below this 2.2.3 Test using zero benchmark, it is likely that the solution membrane has become wet dur- This test proves the absence ing calibration, and there may be of zero current in the sensors. too much water in the calibration At a oxygen content of 0 mg/L vessel. The target value of above a sensor should only display a 100% saturation results from the maximum of the resolution of the different viscosities of water and meter (1 digit). The check is car- air as well as the tension of the ried out with a sodium sulfite solu- water surface. Expressed in a sim- tion. Sulfite reacts with dissolved plified manner, it is easier for the oxygen to sulphate, whereby oxygen molecules to permeate dissolved oxygen is removed the membrane in air than in water. from the water. The production is The normal measurement mode simple, as might be expected. A assumes a liquid sample, so on air teaspoon of sodium sulfite is dis- the reading exceeds 100%. solved in 100 ml tap water. After 2.2.2 Test in air saturated 15 minutes of leaving the solution water undisturbed it is free of oxygen. It must be kept undisturbed as oth- After calibration the value in erwise oxygen from the surround- air-saturated water should show ings will once more be stirred in. between 97 and 102% satura- tion. The theoretical value is at One minute after the immersion 100% and is difficult to repeat. of the sensors the measuring The cause of the relatively wide meter should display a value of tolerance is not the sensor, but maximum 2% and of a maximum rather the saturation procedure. 0.4% after 15 minutes. If not, the 15
Oxygen Handbook sensor is no longer free of zero current and must be cleaned again or sent to the service. After the test, thoroughly rinse the sen- sor with distilled water, in order to remove the rest of the sodium sulfite solution. Galvanic sensors with lead coun- ter electrodes (CellOx® 325 and StirrOx® G) may be immersed for a maximum of 3 minutes. Then also rinse them thoroughly with distilled water. The cleaning of the sensors is very important in order to avoid poisoning and thereby permanent damage. 16
SECTION 3 Measurement and analytical quality assurance The measuring of the oxygen con- Any high mechanical stress of centration is now easy. Immerse the membrane has to be avoided the sensor into the fluid to be at all cleaning activities, as their examined and take the reading. thickness is in the µm range and it That is basically correct, however can easily be damaged. Ideally a a few important points should be soft paper cloth should be used. considered nevertheless. Cleaning in an ultrasound bath should be avoided as the coating 3.1 Cleaning the sensor of the anodes may spall. The part of the sensor that is sensitive to contamination is the 3.2 Regenerating the membrane. Contamination makes sensor itself evident in electrochemical A regeneration of the sensor is sensors through lower readings required if the AutoReg Func- for measurements or reduced tion is activated or the slope has slope during calibration, because strongly decreased after calibra- the complete surface of the tion (S
Oxygen Handbook if the membrane is damaged or with a soft cloth in order to contaminated. remove easily soluble salt crusts. A spotted coating fol- It comprises the change of the lowing the regeneration of electrolyte solution, the cleaning the lead or silver electrodes of the electrodes and a change of will not have an impact on the the membrane head. measurement. It is important that the operating • For the polishing of gold instructions are strictly adhered electrodes, only use a moist- to in order to avoid faults. The fol- ened WTW polishing strip, as lowing points should be empha- it has a suitable granulation sized: for polishing and causes no • The sensor must be separated scratches. from the meter. In the case • It is also recommended using of a connected sensor, upon a new membrane head, as immersion in the cleaning the correct positioning of the solution, no chemical reaction membrane and the spacer takes place between the solu- grid on the gold cathode is tion and the oxidized refer- no longer guaranteed when ence electrode surface, but reusing the used and stressed an electrolytic decomposition head (Fig.9). of the cleaning solution may take place. Gold cathode • In correspondence with the operating instructions, use Electrolyte Spacer suitable cleaning solution and filling grid electrolyte solution for the Membrane sensor! A solution for silver Fig. 9 Schematic diagram of the electrodes cannot regenerate membrane head any lead electrode. • Only the gold cathode can be polished, the counter elec- trodes must only be cleaned 18
• This spacer grid is clearly vis- ible if the membrane head is held against the light. • In the regeneration of three- electrode sensors (e.g. TriOx- matic®) the sensor may only be immersed to a depth that the already mentioned third electrode is not wetted by the cleaning solution (see operat- Fig. 10 Saturation ing instructions). 3.3.2 Display as oxygen • The polarization time after re- saturation percentage generation has to be adhered The meter measures the sensor to. current and calculates the oxygen 3.3 Unit and display of partial pressure in accordance with the calibration. The current the measuring result barometric pressure is measured The result of an oxygen measure- for the calculation of the satura- ment can be documented in dif- tion partial pressure. The display ferent ways: corresponds to the quotient, con- 3.3.1 Display as a verted into percent (Fig. 10). concentration value The meter requires the relevant data from the calibration curve to calculate, under consideration of the temperature dependence of the individual parameters, the concentration in mg/L (the display in ppm is for media with a den- sity numerically equal to 1 g/mL; Fig. 11). Fig. 11 Concentration 19
Oxygen Handbook For many meters the oxygen measured value is considered to partial pressure can also be dis- be the actual measured value. played in hPa. ∆β/∆t Oxygen concentration [mg/L] 3.4 Potential error sources ∆β/∆t 3.4.1 Polarization times (running-in time) before measurement Time [s] If the sensor has been separated from the meter, a correspond- Fig. 12 Oxygen concentration dependent on time ing polarization time is required for the start of the measurement A subjective assessment of the upon reconnection of ampero- measured value stability is omit- metric sensors (gold-silver elec- ted and the repeatability of the trode systems). Galvanic sensors measurement is improved. (gold-lead electrode systems) are Particularly recommended for the not affected by this, as these are determination of the biochemi- self-polarizing and can be used cal oxygen requirement is the immediately. Only after regenera- use of the AUTOREAD function tion a certain waiting time has to as precision measurements with be adhered before measuring. significantly higher reliability can 3.4.2 Drift check be carried out. (AUTOREAD) 3.4.3 Importance of flow Similar to the case of the pH measuring meters the drift check For a correct oxygen measure- tests the stability of the sensor ment the sensor’s membrane signal (Fig. 12). Here the temporal must have a constant flow on change of the measured values is it. The diffusion of the oxygen examined and and the response molecules into the sensor head of time of the sensor is evaluated. If electrochemical sensors causes the drift or the change is below an oxygen impoverished area a defined value, the signal is suf- which results in an apparently low ficiently stable and the currently oxygen concentration. The con- centration in front of the mem- 20
brane must be the same as in the the membrane. This is driven by rest of the sample. an electromagnetic alternating field from a laboratory stirrer. Sensor head Sensor head The great advantage of this O2 O2 equipment is the dimension of O2 the stirring attachment. It has the O2 O2 same diameter as the sensor and O2 Flow is mounted on the sensor head. O2 O2 O2 O2 This facilitates a simple measure- O2 O2 ment in sample flasks, such as O2 O2 O2 O2 the Karlsruhe bottles for the BOD measurement. Fig. 13 Diffusion behavior with and without incident flow The WTW sensor StirrOx® G has been specifically designed for the This condition can be fulfilled BOD measurement. A propeller either by stirring the sample or is installed in the sensor shaft and moving the sensor in the sample. provides flow to the membrane. The stirring effect is hereby so strong that the homogenization of the sample is also assured. If agitators or magnetic stirrers are used, the possible forma- tion of eddies must be taken into account. The dissolved oxygen sensor must not be positioned in the eddy because air at the Fig. 14 Stirring attachment for membrane would falsificate the laboratory dissolved oxygen sen- sors measuring result. This can be prevented by reducing the stir- We offer specific stirring attach- ring frequency or positioning of ments (Fig. 14) which rotate like the sensor outside of the eddy small turbine blades and con- formation. stantly provide fresh samples to 21
Oxygen Handbook In the case of the installation in tion tank is non-critical due to the pipes the sample bypasses the high sample volume. In an open sensor head and provides suffi- beaker glass, on the other hand, cient flow. WTW provides station- the oxygen concentration can be ary measurement systems with easily changed through stirring. specific mounting fixtures for In the case of optical sensors, pipes. which, as a matter of principle, do Alternatively the sensor can be not require any flow to function, moved in the measured medium. the stirring does still help to reach For example, stirring the sensor in the end value faster. a beaker glass or by slewing it in 3.4.4 Salt content correction a lake. For measurements at great depths, armatures for measure- The temperature-dependent ments up to 100 m are available. Bunsen coefficient (see Equation 2) changes if substances are dis- It must be ensured that the stir- solved in the water. This effect is ring causes no falsification of the taken into account by the input of measured values. This may par- salinity. The salinity can be deter- ticularly be the case if the sample mined with a conductivity meter examined is over- or under-sat- and, to some extent, the salt urated with oxygen and oxygen content of seawater in g/kg. This can be expelled or stirred in. Oxy- function can be also be used for gen over-saturation is, for exam- other waters, as the deviations are ple, to be found in still waters in often small. summer if the photosynthesis of 3.4.5 Impact of interferring rampant algae produces oxygen. gases An example of oxygen under-sat- The membrane of the dissolved uration is the BOD determination oxygen sensor can also be per- where bacteria lower the oxygen meated by other gases alongside concentration by respiration in the oxygen (Fig. 15). Karlsruhe Bottles. Correspondingly the sample volume is also of importance. A measurement in a lake or aera- 22
Sensorkopf into acidic, the measuring meter Sensor head displays too high readings. CO2 N2 H2S O2 NH3 The greatest danger for dissolved oxygen sensors comes from hydrogen sulfide because this H2S O2 NH3 poisons the counter electrodes CO2 N2 through the sulfide ion created by Fig. 15 Permeability of the mem- neutralization reaction. brane for different gases The sensors can cope with a small Nitrogen is not very reactive and amount but a longer exposure does not play any role here. will noticeably shorten the sensor operation time. Hydrogen sulfide The interference by ammonia is is easily detected due to its smell, negligible due to the high pH of which is similar to rotten eggs and the electrolyte. can be noted even in the smallest Carbon dioxide, on the other concentrations without the need hand, is problematic. The buffer for measurement technology. capacity of the electrolyte solution 3.4.6 Solubility function is sufficient for short-term expo- If the aim is to determine the sure, but under longer-lasting ex- concentration of the dissolved posure carbon dioxide shifts the oxygen in non-water-based fluids, pH value into the aciduous range the corresponding solubility func- and leads to too high readings. tion must be known. In this case, Here galvanic sensors can regen- the oxygen measurements are to erate the buffer capacity better be carried out analogous to the than amperometric sensors, as measurement in water. they form excess hydroxide ions through the electrode reactions. In the case of high carbon dioxide content (e.g. in beer, champagne, lemonade), the buffer capacity of the electrolyte solution in the sensor is insufficient. The pH shifts 23
Oxygen Handbook SECTION 4 Optical oxygen measurement In the past few years a further fluorescence (Fig. 16). As part of technology has been established this, dye molecules are excited by for dissolved oxygen measure- light. Upon return to the ground ment. Oxygen is no longer solely state the absorbed energy is electrochemically measured but emitted in the form of light with also optically. [2] Of course the changed (larger) wavelengths. basics of oxygen determination There are substances which mea- also remain applicable here. Cor- surably affect this mechanism de- responding to the measurement pending on their concentration. technology there are new aspects These are the so-called quench- which are explained below. ers. This means that these ma- 4.1 The principle of terials absorb the energy of the excited state so that the dye can optical measurement no longer emit fluorescent light A sensor for optical measurement and is thereby “extinguished”. The is also described as an optode. intensity of the fluorescent light Optodes equipped with special becomes smaller the higher the dyes show optical measurable concentration of the quencher reactions when they come in con- molecule is. This context is basi- tact with the specific molecules. A cally described in the Stern-Vol- mass and energy conversion does mer Equation: not take place as for example with the Clark cells. It is only an I0 = 1 + k SV ⋅ c Q energy conversion because a I incident light beam of a certain Here I0 is the light intensity with- wavelength is changed into light out the quencher, I the intensity of longer wavelength and other with the quencher in a corre- properties than the original light. sponding concentration, kSV the This type of reaction is known as 24
Stern-Volmer constant and cQ the means of this dye suitable mem- concentration of the quencher. In branes can be produced for the this context is also interesting that measurement of oxygen in fluids not only the intensity but also the or gases. temporal decay of the fluorescent LEDs serve as the light source. light after excitation continues to The exciting of the fluorescence behave correspondingly with the takes place in a modulated man- Stern-Volmer Equation. ner (Fig. 17). The light emitted from the dye in the membrane is Green LED Detector detected, converted into an elec- trical signal and converted into an oxygen signal. Intensity Phase Fig. 16 Luminescence excitation using light of a short wavelength Fig. 17 Simplified representation (green here), emission of a red of modulated stimulus and emit- and so low-energy fluorescent ted fluorescence beam beam. Green graph: light periodi- What does this mean for the dis- cally beamed in, red graph: light solved oxygen measurement? emitted from the dye at a shifted There are dyes which are excited phase resulting from the changed by visible light and react on oxy- decay ratio. gen with a high selectivity. The oxygen molecules serve as the quenchers described above. They extinguish or change the light resulting from the dye depending on the oxygen partial pressure. By 25
Oxygen Handbook 4.2 Characteristics of optical dissolved oxygen sensor, there is diffusion of the dissolved the optical dissolved oxygen in the water depending oxygen sensors on the concentration into or out The significant difference from of the membrane. This process the classical dissolved oxygen naturally runs faster the better sensors is that optical sensors the exchange takes place at the consume no oxygen. There are interface. A stirring supports this no electrochemical reactions. In exchange. addition, there is a further charac- There is no polarization time teristic: The optical sensor does for optical sensors as it has no not require any flow to replace electrodes which have to reach an “consumed” oxygen. Stirring sys- operating condition. tems are then superfluous. In ad- dition, there is no necessity for the Optical dissolved oxygen sensors electrolyte change or cleaning the are sensors which have active electrode system. The life span of components (LEDs, detector, pro- the optical sensor caps with the cessor). In contrast to the electro- dye-containing membrane usually chemical sensors, they are more is at least one year. power consuming which leads to a markedly reduced operating Electrochemical sensors form in time in the case of portable sys- water a 10 µm thick layer of water tems. Additionally optical sensors molecules that can not be stirred. need different meters. As consequence this layer serves as an additional diffusion barrier. The measurement range is notice- On air these sensors show a satu- ably restricted in comparison ration signal of about 102 %. The to the electrochemical sensors optical sensor measures 100 % air above. The reason for this is the saturation as this barrier does not quenching. Simplified, no oxygen exist here. leads to a strong signal, a large amount of oxygen leads to a weak However it may be reasonable signal. In general the measure- to apply flow to an optical sen- ment range does not exceed ap- sor. As with all systems with interfaces, even when using the 26
prox. 200% air-saturation respec- Of course a calibration carried out tively 20 mg/l. by the user is also possible. It is implemented analogously to the 4.3 Calibration of optical electrochemical sensors in water- dissolved oxygen vapor-saturated air in the calibra- sensors tion vessel. As already mentioned above, the resulting saturation An advantage of the optical display is at 100%. dissolved oxygen sensors is that very stable drift behaviour. 4.4 Cleaning of optical The changes in the membrane dissolved oxygen are mainly caused through the irradiated light. A decrease in sensors sensitivity results, triggered by the The sensitive surface of an opti- so-called bleaching to a decrease cal oxygen sensor is protected in intensity and a change of the by a light proof top layer. This phase shift. top layer is very thin and must therefore not be scratched or These changes are generally damaged as otherwise this could much smaller than 5% of the initial lead to malfunctions. In relation value over the course of a year. If to the cleaning the same mea- this tolerance can be accepted, sures apply as to the conventional the sensor does not need to be oxygen membranes. In the case calibrated. of easily adhesive contamination We apply the dye to changing careful cleaning with a soft cloth is caps that the user simply puts recommended, further notes can onto the sensor. These exchange be found in the operating instruc- caps contain a chip with the tions. specifications of the individual membrane determined in the pro- duction process (“factory calibra- tion”). These data are automati- cally transferred to the sensor and used for the correct calculation of the oxygen concentration. 27
Oxygen Handbook 4.5 Impact of hydrogen sulfide, which results from the putrefaction processes interferring gases in many waters, that here dissem- In contrast to the amperomet- bles an oxygen signal. This signal ric sensors, carbon dioxide and is reversible, the sensor does not hydrogen sulfide play no role undergo any damage. in relation to the operation life of or damage to the sensors. It must solely be noted that, for example, hydrogen sulfide also functions as a quencher due to its molecular mass. An example from practice would be the decreasing oxygen content in limnological depth measurements at increas- ing depths, which seem to un- dergo an increase if the sensor is immersed into soft sediment. However the reason for this is the 28
Bibliography [1] DIN EN ISO 5814, Water qual- ity – Determination of dissolved oxygen – Electrochemical probe method, 2013 [2] DIN ISO 17289 : 2014-12 Water quality – Determination of dissolved oxygen – Electrochemi- cal probe method 29
Oxygen Handbook Further handbooks Order our handbooks and tips for practice! • pH Handbook • Conductivity Handbook WE SUPPLY • • Ion-Selective Handbook (in preparation) Practical Photometry Tips KNOW • • • Titration Handbook Viscometry Handbook Refractometry Handbook HOW Meters Lab undand ProLab Electrodes Titration Titrations pH, Fibel Serien Handbook pH,ISE, ISE,LF LFUND UNDOO22MESSEN MESSEN——GENAU, GENAU,ZUVERLÄSSIG, ZUVERLÄSSIG,SELEKTIV SELEKTIV Titrations Fibel pH, ISE, COND AND O2 | PRECISE - RELIABLE - SELECTIVE IN LABAND AND FIELD OFTITRATION IN LAB AND THEORIE THEORY FIELD DER UNDPRACTICE PRAXIS TITRATION THEORIE UND PRAXIS DER TITRATION 30
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