conductometric and potentiometric titration
Transcription
conductometric and potentiometric titration
Politechnika Gdańska Wacław Grzybkowski CONDUCTOMETRIC AND POTENTIOMETRIC TITRATION Gdańsk 2002 CONTENTS 1. TITRATION 3 2. CONDUCTOMETRIC TITRATION 5 3. POTENTIOMETRY 3.1 pH measurements 3.2 Potentiometric titration 14 14 16 TITRATION Titration is process of chemical analysis in which the quantity, amount or concentration, of some constituent of a sample, known as an analyte, is determined by adding to the measured sample an exactly known quantity of another substance with which the desired constituent reacts in a definite, known proportion. The process is usually carried out by gradually adding a standard solution (i.e., a solution of known concentration) of titrating reagent, or titrant, from a burette, essentially a long, graduated measuring tube with a stopcock and a delivery tip at its lower end. Titrations may be carried out by hand from the burette or automatically. At the equivalence point of a titration, an exactly equivalent amount of titrant has been added to the sample. The experimental point at which the completion of the reaction is marked by some signal is called the end point. This signal can be the colour change of an indicator or a change in some chosen, e.g., electrical property that is measured during the titration. The difference between the end point and the equivalence point is the titration error, which is kept as small as possible by the proper choice of an end-point signal and a method for detecting it. For many titration reactions it is possible to find a suitable visual colour indicator that will signal the end point at, or very close to, the equivalence point. Such titrations, classified according to the nature of the chemical reaction occurring between the sample and titrant, include: acid-base titrations, precipitation titrations, complex-formation titrations, and oxidation-reduction (redox) titrations. In acid-base titration (i.e., the titration of an acid with a base, or vice versa), the indicator is a substance that can exist in two forms, an acid form and a basic form, which differ in colour. For example, litmus is blue in alkaline solution and red in acid solution. Phenolphthalein is colourless in acid solution and pink in alkaline solution. A wide choice of acid-base indicators is available, varying not only in the colours of the two forms but also in the pH value at which the colour occurs. Precipitation titrations may be illustrated by the example of the determination of chloride content in a sample by titration with silver nitrate, which precipitates the 3 chloride in the form of silver chloride. The presence of the first slight excess of silver ion (i.e., the end point) can be marked by the appearance of a coloured precipitate. One way in which this can be done is by employing potassium chromate(VI) as the indicator. Potassium chromate reacts with the first slight excess silver ion to form a red precipitate of silver chromate. Another method involves the use of an adsorption indicator, the indicator action being based on the formation on the surface of the precipitate of an adsorbed layer of silver indicator salt, which forms only when an excess of silver ions is present. The most important titrations based upon complex-formation reactions are those involving the titration of metal ions with the reagent disodium ethylenediaminetetraacetate (a salt of edetic acid, or EDTA). The indicators are dyes that have the property of forming a coloured complex with the metal ion. As the titration proceeds, the reagent reacts first with uncomplexed metal ions, and, finally, at the end point it reacts with the metal-indicator complex. The colour change corresponds to the conversion of the metal-dye complex into the free dye. In oxidation-reduction (redox) titrations the indicator action is analogous to the other types of visual colour titrations. In the immediate vicinity of the end point, the indicator undergoes oxidation or reduction, depending upon whether the titrant is an oxidizing agent or a reducing agent. The oxidized and reduced forms of the indicator have distinctly different colours. Alternatively, for many titrations the end point can be detected by electrical measurements. These titrations may be classified according to the electrical quantity that is measured. Potentiometric titrations involve the measurement of the potential difference between two electrodes of a suitable cell; conductometric titrations, the electrical conductance or resistance of the solution being titrated; and amperometric titrations, the electric current passing during the course of the titration. In the titrations just mentioned the end point is indicated by a marked change in the electrical quantity that is being measured. 4 CONDUCTOMETRIC TITRATION In this experiment we shall be concerned with electrical conduction through aqueous solutions. Although water is itself a very poor conductor of electricity, the presence of ionic species in solution increases the conductance considerably. The conductance of such electrolytic solutions depends on the concentration of the ions and also on the nature of the ions present ( through their charges and mobilities ). Conductance behaviour as a function of concentration is different for strong and weak electrolytes. Electrolytic solutions obey Ohm’s law just as metallic conductors do. Thus the current i passing through a given body of solution is proportional to the potential difference U, and i= U R where R is the resistance of the body of solution in ohms [Ω] . The conductance G is defined as the reciprocal of the resistance G= 1 R and is expressed in siemens [S], that is in ohms-1 [Ω−1] or mhos. The conductance of a homogeneous body of uniform cross section is proportional to the cross section A and inversely proportional to the length l : G=κ A l where κ is the conductivity or the specific conductivity expressed in S·cm-1 or in Ω−1·cm-1. The conductivity is thus the reciprocal of the resistivity. The conductivity of 5 a solution in a cell of an arbitrary design and dimensions can be obtained by first determining the cell constant k, being the effective value of l/A, by measuring the resistance of a cell filled with the solution of known conductivity. One of the standards solution that can be used for making this calibration is 0.02000 molar solution of potassium chloride, with conductivity equal to 0.002768 S·cm-1 at 25ºC. Once the cell constant has been found, conductivity can be calculated from the experimental resistance by using equation κ= k R The conductivity of a solution depends on the concentrations and mobilities of the ions present. It is convenient to define a new quantity, the molar conductance Λ, by Λ= 1000 κ c where c is the molar concentration, that is expressed in mol·dm-3. 1000 is the factor arising from the fact that 1 dm3=1000 cm3. Thus, the molar conductance is expressed in S·cm2·mol-1. The molar conductance is sometimes described as the actual conductance of that volume of solution which contains one mol of solute when placed between parallel electrodes 1 cm apart with a uniform electric field between them. In order to compare the conductances of the electrolytes differing in the ionic composition the equivalent conductance Λeq is defined Λ eq = 1000κ c eq where c is the equivalent concentration, that is expressed in equiv.·dm-3 For a strong electrolyte the molar and/or equivqlent conductances are roughly constant, decreasing to some extent owing to changes in mobilities with increasing concentration but approaching a finite value Λο at infinite dilution. Typical plots of equivalent conductance against square root of the salt concentration are presented in Figure 1. As is seen, if the conductance is plotted against the square root of the concentration a linear relationship 6 Λ = Λ0 − β c is valid at low concentration range. Fig.1. Plots of equivalent conductance of the strong electrolytes as a function of c 1/ 2 , at low concentrations the plots are linear as is indicated by broken lines. It was first described by Kohlrausch (1900) and is found to be universal for strong electrolytes. Moreover, this relationship known as Kohlrausch’s law was deduced from the effect of ion attraction on the mobilities. Using this relation, Λο for strong electrolytes can be obtained experimentally from conductance measurements. At infinite dilution the ions act altogether independently, and it is then possible to express Λο as the sum of the limiting conductances of the separate ions : Λ0 = λ0+ + λ0 It is known as the law of independent migration of ions. For hydrochloric acid we can write [ ] [ ] Λ0 [HCl] = λ0 H+ + λ0 Cl while for sulphuric acid [ ] [ Λ0 [H2 SO 4 ] = 2 λ0 H + + λ0 SO 24− 7 ] For weak electrolytes, thus for weakly ionized solutes, Λ varies markedly with concentration because the degree of dissociation varies strongly with concentration. The limiting molar conductances of weak electrolytes we can calculate with the help of the law of independent migration of ions. Thus, for acetic acid, we can write: [ ] [ [ ] [ Λ0 [CH3 COOH] = λ0 H + + λ0 CH3 COO − ] ] [ ] [ ] [ ] [ ] = λ0 H + + λ0 CH3 COO _ + λ0 Na + − λ0 Na + + λ0 Cl − − λ0 Cl − = Λ0 [HCl] + Λ0 [CH3 COONa] − Λ0 [NaCl] For sufficiently weak electrolytes, the ionic concentration is small and the effect of ion attraction on the mobilities is slight; thus we may assume the mobilities to be independent of concentration and obtain the approximate equation Λ Λ0 α= which may be used to calculate the value of fractional ionization α, known also as the degree of dissociation. If one measures Λ for a weak electrolyte at concentration c and calculates Λο from conductometric data for strong electrolyte or from known values of the limiting conductances of the individual ions, it is possible to obtain the actual degree of ionization of the weak electrolyte at this concentration. Then the value of respective equilibrium constant, KC, can be estimated using the Ostwald’s Dilution Law KC = α 2c 1− α For determining electrolytic conductance by measuring the resistance of the solution in a conductivity cell, the use of direct current circuitry is impractical, since the electrodes would quickly become polarized; that is, electrode reactions would take place. Polarization can be prevented by (1) using high frequency alternating 8 current, so that the quantity of the electricity carried during one half cycle is insufficient to produce any measurable polarization, and at the same time by (2) employing platinum covered with platinum black, having an extremely large surface area, to facilitate the adsorption of the tiny quantities of electrode reaction products produced in one-half cycle, hence, reducing the polarization effect. Classical circuit employed to such measurements is a Wheatstone Bridge adapted for use of a high frequency alternating current. However, a variable capacitance is necessary to achieve a true balance and eliminate the non-ohmic effects. Determination of the ac impedance can be also carried out with an automatic bridge that employs a frequency generator and gives a direct read-out. Such an equipment is employed for measurements during conductometric titration. In all measurements of impedance, careful temperature control is essential, since viscosity of water, for example, changes in the region near room temperature by about of 3% per degree. It was mentioned above that the measured conductance of an electrolyte solution depends primarily on the concentration and types of the ions. Conductivity measurement can thus provide a sensitive measure of the changes taking place in ionic composition in the course of chemical reaction occurring in the solution during conductometric titration. Consider a solution of a strong acid, hydrochloric acid, HCl for instance, to which a solution of a strong base, sodium hydroxide NaOH, is added. The reaction H+ + OH → H2 O occurs. For each amount of NaOH added equivalent amount of hydrogen ions is removed. Effectively, the faster moving H+ cation is replaced by the slower moving Na+ ion, and the conductivity of the titrated solution as well as the measured conductance of the cell fall. This continues until the equivalence point is reached, at which we have a solution of sodium chloride, NaCl. If more base is added an increase in conductivity or conductance is observed, since more ions are being added and the neutralization reaction no longer removes an appreciable number any of them. Consequently, in the titration of a strong acid with a strong base, the 9 conductance has a minimum at the equivalence point. This minimum can be used instead of an indicator dye to determine the endpoint of the titration. Conductometric titration curve, that is a plot of the measured conductance or conductivity values against the number of milliliters of NaOH solution, is shown in Fig. 2. Fig.2. Conductometric titration curve for hydrochloric acid titrated using solution of sodium hydroxide. The position of the equivalence point may be localized precisely as the point of intersection of two straight-lines both determined using readings obtained before and after the minimum observed, respectively. It makes the conductometric titration more objective and independent of a nature of an indicator used in the end-point method. This is one of advantages of the instrumental method. The same reaction of neutralization takes place when a solution of strong base is titrated using a solution of strong acid. Thus, analogous effects and very similar shape of conductometric titratration curve are observed. Consider the titration of solution of weak acid, such as acetic acid CH3COOH, using a solution of strong base, NOH. As we know, the weak acids, as well as other weak electrolytes, are dissociated into very small extent and they exist in solution essentially in form of the neutral acid molecules. When a solution of NaOH is added the reaction occurs CH3 COOH + Na + + OH- → Na + + CH3 COO − + H2 O and, as is seen, the undissociated molecules of acetic acid are transformed into dissociated molecules of potassium acetate. The changes are accompanied by increase in conductivity of the solution, Figure 3. 10 Fig.3. Conductometric titration curve for acetic acid titrated using solution of sodium hydroxide. It should be noted, however that an initial decrease in a conductivity of the solution may be observed after addition of the first drops of titrant. This minor importance effect is related to neutralization reaction of the protons resulting from a dissociation and existing even in a solution of the weak acid H+ + OH → H2 O Thus, an mild increase in conductivity of a titrated solution is observed until the equivalence point is reached, at which we have a solution of sodium acetate, CH3COONa. If an excess of titrant, that is the potassium hydroxide solution, is added a sharp increase in conductivity is observed. This distinct difference in a rate of increase is related to the fact that the excess OH- anions, as well as the protons, exhibit particular mechanisms of charge migration More detailed inspection of the conductometric titration curve presented in Fig.3. indicates that the equivalence point is less sharp than that observed for the strong acid. Thus, it should be localized as the intersection point of two lines determined by two section of the conductometric curve. The slope of the first part of the conductometric curve is dependent on a strength of the acid. It means that it is positive for very weak acid only. 11 The method of conductometric titration is thus well adapted to the estimation of mixtures of acids of differing strengths. When a mixture of strong and weak acid is titrated a plot of conductance against alkali added takes form of Fig.4. Fig.4. Conductometric titration curve for the hydrochloric acid – acetic acid mixture titrated using solution of sodium hydroxide. As is seen, the conductometric titration curve is a combination of the diagrams obtained during the titration of strong and weak acid respectively, where the first endpoint corresponds to a neutralization of the strong acid present in the sample and the second one is associated with a neutralization of the weak acid in the solution under investigation. The volume of the alkali consumed by the latter is given by a difference of the respective volumes. Analogous conductometric titration curve is obtained for an oxalic acid, solution titrated using a solution of strong base, NaOH. Oxalic acid, chemical formula H2C2O4 or (COOH)2, is the simplest dibasic, i.e. diprotic carboxylic acid. As is seen, its molecule consists of two carboxylic groups only and a dissociation equilibria are described by the following two equations H2C2O 4 → H+ + HC2O 4 − HC2O 4 → H+ + C2O 4 12 − 2− The dissociation constant for the second proton is significantly smaller, and so pK2 > pK1. Hence, the solution of the oxalic acid may be considered as an equimolar mixture of two acids of differing strength. The dissociation constant for the second proton is significantly smaller, and so pK2 > pK1. Hence, the solution of the oxalic acid may be considered as an equimolar mixture of two acids of differing strength. It seems to be rather obvious that an analogous conductometric titration curve describes a conductometric titration of solution of weak base, such as ammonia, using a solution of strong acid. The conductometric titration method can also be employed in other volumetric estimations, e.g. the determination of halides by titration with silver nitrate. Correction for the relatively small change of volume during the titration is readily made by plotting not the measured conductance or conductivity, but the values of product of the conductance and total volume of the sample, against the volume of titrant added. 13 POTENTIOMETRY pH MEASUREMENT Perhaps the most common potentiometric measurement is that of pH. pH was defined originally as − lg CH+ or lg( 1/ C H+ ) , where CH+ is the concentration of hydrogen ion. Today instead of CH+ one would write aH+ , the activity of hydrogen ion. The experimental determination of pH potentiometrically leads to a value which is neither strictly concentration nor activity of hydrogen ion but something in between. The measurement of the pH of a solution is simple in principle, fo it is based on the measurement of the potential of hydrogen electrode immersed in the solution. The left-hand, i.e. the reference electrode of the cell is typically a saturated calomel electrode (SCE) with potential E(cal). The pH of the cell is therefore pH = E + E(cal) ( −RT / F) ln10 pH = E + E(cal) (− 59,16 mV ) or at temperature of 250C The practical definition of the pH of a solution X is pH ( X) = pH (S) − E (RT / F) ln10 pH ( X) = pH (S) − E ( 59.16 mV ) or at 250C, where E is the potential of the cell Pt | H2 (g) | s(aq) || 3.5 MKCl (aq) || X(aq) H2 (g) | Pt 14 and S is a solution of standard pH while || 3.5 MKCl (aq) || denotes the salt bridge. The currently recommended primary standards include a saturated solution of potassium hydrogen tartrate, which has pH =3.557 at 250C and 0.0100 mol kg-1 disodium tetraborate, which has pH=9.180 at that temperature. In practice, indirect methods are much more convenient, and the hydrogen electrode is replaced by the glass electrode. This electrode is sensitive to hydrogen ion and its potential is proportional to pH. It is filled with hydrochloric acid or phosphate buffer containing Cl − anions. Conveniently, the glass electrode has E=0 when the external medium is at pH=7.The glass electrode is much more convenient to handle than the gas electrode itself, and can be calibrated using solutions of known pH. The glass electrode is usually used in conjunction with a calomel electrode that makes contact with the test solution through a salt bridge. Fig.1. Glass electrode and its cell schematic in association with a reference electrode 15 The sensitivity of a glass electrode towards hydrogen ( H+ ) or hydronium ( H3 O + ) ion is a result of complex processes at the interface between the glass membrane and the solutions on either side of it. The membrane itself is permeable to Na+ and Li+ cations but not to H+ ions. Therefore, the potential difference across the glass membrane must arise by a mechanism that is different from that responsible for biological transmembrane potentials. A clue to the mechanism comes from a detailed inspection of tee glass membrane, for each face is coated with thin layer of hydrated silica. The hydrogen ion in the test solution modify this layer to an extent that depends on their activity or/and concentration in the solution, and the charge modification of the outside layer is transmitted to the inner layer by the Na+ and Li+ cations in the glass. The hydronium ion activity give rise to a membrane potential by this indirect mechanism. POTENTIOMETRIC TITRATION If, during a chemical reaction, there is a change in the concentration of an ion which can be sensed through the change in potential of a suitable electrode, then the progress of the reaction can be followed through this potential change. It follows the electromotive force measurements, like conductivity measurements, can serve to determine the equivalence point or end point of titration. Both conventional electrodes and the types of ion-sensitive electrodes can be used to follow the process and the change of potential in the case of acid-base, precipitation, complexation and red-ox titration. To follow an acid-base titration a hydrogen electrode or a pH-sensitive glass electrode may be used as the indicator electrode. In both cases, as the titration is carried out, for example, by addition of alkali to an acid solution, the potential difference measured will decrease at the rate of 59.1 mV per decade lowering in H3O+ concentration. As long as the acid is in excess, then the pH, as well as the electromotive force of the studied cell, will vary only slightly with addition of base. However, near the equivalence point, concentration of the H3O+ cation falls rapidly before levelling out again in excess base. Thus, the measured potential difference will show a step-like behaviour, as is seen in Figure 1, 16 in which the change in potential of the pH-electrode is calculated for titration of 100 cm3 of 0.01 M solution of strong acid, HCl, with 0.1 M solution of strong base. The end-point of the titration corresponds to the point at which the potential changes most rapidly. Fig.2. Potentiometric acid-base titration: (a) schematic representation of titration of 100 cm3 of a strong acid of concentration 0.01 M with a stronge base of concentration 0.1 M; (b) differential potential change on addition of aliquots of titrant, showing a marked peak at the end point. 17 A more precise measure of the end-point than the position of the steepest change in the potential difference, i.e. the change in the electromotive force, can be obtained by plotting the derivative of the potential difference with the volume of titrant added. This is shown as the dotted line in Figure 2, and it can be see to have a nice, sharp maximum indicating a position of the end-point. As an example of the precipitation titration, consider the determination of the chloride ions by silver nitrate, making use of the reaction Ag + + Cl − → AgCl(s) here, the equilibrium-potential of the Ag|Ag+ electrode can be followed as a function of addition of the titrant. At the beginning of the titration, the concentration of silver in solution will, in effect, be determined by the solubility product of silver chloride, and, at the end-point, the Ag+ concentration will rise very rapidly as the last of the chloride is precipitated. The height of the potential step can be further enhanced if the titrations is carried out in a water-acetone mixture, in which the solubility of silver chloride is lower. The change of potential in the case of complexation and redox titrations is very similar to that observed in case of potentiometric acid-base and precipitation titration. Potentiometric titrations have the great advantage, in common with conductometric titrations, of being possible in turbid, coloured and very dilute solutions. Further advantages of potentiometric titrations are the generally very sharp end points and the ease of automation, and a large number of commercial rigs are available. The range of applications is enormous, and accurate methods have been developed for many electroanalytical processes. 18