Patent Application: US-201314890943-A

Abstract:
a method and device for measurement is disclosed in operation , an undivided cell sensor immersed at any desirable point of the positive electrolyte circuit is constantly supplied at a controlled fixed dc bias voltage between the positive metal electrode and the porous carbon counter - electrode by an appropriate voltage regulator of adequate power capability , or cyclically at two or more different voltages , all within a range that includes the region between 0 . 35v and 0 . 45v , measuring simultaneously the current flowing across the undivided cell sensor at the fixed voltage or voltages bias . by correlating the paired voltage and current values , using a look up table compiled at calibration , estimated values of the degree of oxidation or state of charge of the redox ion couple of the positive electrolyte solution are produced .

Description:
a diagram showing the electrochemical potential characteristic curve and the open circuit cell voltages for the distinct phases of charging and discharging of an all - vanadium rfb system is depicted in fig1 . typically , operators concern focuses on preventing conditions of oxidation of vanadium ions in the positive electrolyte solution to a degree such to cause a starvation of vo 2 + ions at the wetted surface of the positive porous carbon electrodes of the battery cells to be oxidized to vo 2 + . this , in practice means that a safety maximum limit of about 1 . 45 - 1 . 50v of the ocv value is generally considered a viable full charge condition of the rfb system . however , any undetected unbalance of the respective states of charge of the negative and positive solutions , because of a progressive oxidation of the negative electrolyte solution by exposure to air and / or parasitic hydrogen evolution ( gassing ) phenomena at the negative porous carbon electrodes when functioning at elevated current densities , may shrink at its negative end the ocv to a point that even a would - be - safe 1 . 45v reading may be masking a condition of excessive oxidation degree of the vanadium ions in the positive electrolyte solution , as it may be assessed only on the basis of the ocv information . the arrows span of such a one - ended shrunk ocv traced on the diagram of fig1 shows the baffling shift to which the ocv information is subjected because of the contraction at its negative end of the ocv magnitude in case of charge unbalance between the two solutions . fig2 shows the laboratory set - up used for studying the electrochemical behaviour of a charged positive electrolyte solution of a vanadium rfb subjected to electrolysis in a undivided cell 3 having a stable electro catalytic metal anode 3 a and a porous carbon cathode 4 c . a fluid permeable plastic insulating screen 3 b prevents a short circuiting contact between the opposed electrodes . the immersed portion of the electrode assembly had a projected cell area of 18 cm 2 . the metal anode 3 a was an expanded titanium plate with a void / solid ratio of about 0 . 4 , coated with a electro catalytic ceramic coating of oxides of tantalum , zirconium , tin and iridium conferring to the anode the ability to discharge oxygen without losing in time its electro catalytic property . the porous carbon cathode 3 c consisted in a compressed bed of active carbon particles contacted by a graphite back plate , connectable to the negative terminal of a controlled power supply . when powering the test cell at a certain output voltage of the power supply vout , the voltage drop contributions are vout = e p − e n + η n + η p + η c + r i cell ( 1 ) e p is the positive electrode potential versus the electrolyte solution that is required for the following possible reactions to occur at the anode 3 a : vo 2 + + h 2 o = vo 2 + + 2h + + e − e ° =+ 1 . 0 volt in fact , this reaction requires a potential of + 1 . 0 volt ( at standard conditions ) and slightly higher or lower if the conditions are not standard ( in standard conditions the concentration of vo 2 + is identical to the concentration of vo 2 + ). this reaction will occur only if v + 4 ( i . e . vo 2 + ) is present and cannot occur any longer if the state of oxidation of the electrolyte is + 5 . 0 . h 2 o = ½o 2 + 2h + + 2 e − e °=+ 1 . 23 volt e n is the negative electrode potential that is generated by the following reaction of those theoretically possible at the carbon cathode 3 c : a ) reduction of v + 5 to v + 4 : vo 2 + + 2h + + e − = vo 2 + + h 2 o e °=+ 1 . 0 volt this reaction generates a potential of + 1 . 0 volt ( at standard conditions ) and slightly higher or lower if the conditions are not standard ( in standard conditions the concentration of vo 2 + is identical to the concentration of vo 2 + ). conventionally we attribute a positive sign to this potential because of the sign “ minus ” used in equation ( 1 ). b ) the other possible reaction of hydrogen discharge : 2h + 2e − = h 2 o e °=+ 0 . 0 volt , does not occur because the porous carbon cathode ( free of metal contaminants ) used in the test cells has a high over - voltage for hydrogen ion discharge . η n is the negative electrode over - potential for the sustained electrode reaction specified above , η p is the positive electrode over - potential for the sustained electrode reaction specified above , these over - potentials ( factors of irreversibility of the charge - discharge process ) are all a logarithmic function of the current i flowing through the test cell according to the well known tafel equation . vout = e p − e n + α n 1n i + β p 1n i + γ c 1n i + ri ( 1 ) in this equation e p and e n are the only terms that are not a function of the current “ i ”. if the test cell is driven at voltages capable of forcing a relatively high current , the terms that are function of “ i ” become predominant and much larger than e p and e n . by contrast , if the test cell is driven at relatively low voltages a condition may be reached at which the cell current becomes very low , rendering the terms other than e p and e n practically negligible . the equilibrium equation ( 1 ) becomes : fig3 shows broad - range voltage - current characteristics curves obtained with the set up of fig2 a and 2 b for positively charged vanadium electrolyte solutions of different known degrees of oxidation , forcing a current varying from 0 to 4 . 0a through the test cell of about 18 cm 2 . it is evident a cross - over region at currents of 0 . 7a - 0 . 8a preceding a region of convergence toward a voltage of about 0 . 8 mv when the current has become null , wherein the characteristics curves for different states of charge undergo a bulging of amplitude proportional to the degree of oxidation in other words to the state of charge of the positive electrolyte solution . in the interval between about 0 . 35v and 0 . 45v , such a spread out of the voltage - current characteristic curves is at maximum of amplitude and allows an excellent discrimination of the state of oxidation of vanadium by locating the point on the voltage - current plane . fig4 shows voltage - current characteristics curves obtained in laboratory with the test cell for positively charged vanadium electrolyte solutions of different known degrees of oxidation , expressed in terms of correspondent ocv values of a balanced rfb , in the region of convergence beginning below an applied voltage of about 0 . 7 v to the cell voltage . in this region of distinct spreading out by a peculiar bulging that is more and more pronounced for an increasingly charged state of the positive electrolyte solution , the characteristic curves at different known degrees of oxidation , expressed in terms of correspondent ocv values of a balanced rfb , have been recorded during a calibration work carried out on the specific undivided test cell , that may really be defined an oxidation state sensor . having expressed in terms of correspondent ocv values of a balanced rfb the known state of charge of the solutions used for calibrating the sensor , fig5 shows the correlation characteristics in a cartesian plane of the current measured at the indicated three different bias voltages applied to the test cell ( sensor ) and the known state of charge of the vanadium redox couple in the positively charged electrolyte solutions used . fig6 shows the correlation characteristics in a cartesian plane of the current measured at the indicated three different bias voltages applied to the test cell and the ocv voltage of a battery cell at the correspondent known state of charge of the vanadium redox couple in the positively charged electrolyte solutions used . fig7 illustrates an example of how the method of this disclosure may be implemented in a common rfb system , only partially and schematically traced in the drawing as a symbolic battery cell 1 the flow ( electrode ) compartments of which are traversed by the two streaming solutions , namely : the positive electrolyte and the negative electrolyte , respectively . according to a common practice , the ocv of the battery cell is commonly monitored on a minuscule scaled replica 2 of the battery cell , through the flow compartments of which proportionate streams of the circulating electrolyte solutions are diverted . a voltmeter provides an instantaneous measure that assuming perfect balanced electrolyte solutions should correspond to respective states of charge of the two electrolyte solutions . the method of this disclosure for estimating the degree of oxidation or state of charge of the sole positive electrolyte solution may be implemented , as depicted in the figure , by passing a stream of it through a stable electro catalytic positive metal electrode 3 a and a negative porous carbon counter - electrode 3 c constituting a undivided test cell 3 , i . e . without any fluid impervious membrane permeable to ions , namely a permionic membrane m as it is the case with the battery and ocv cells 1 and 2 , respectively . the test cell 3 may have an enclosure , as schematically shown in the example depicted , for flowing there through the positive electrolyte solution , or a two electrode assembly comprising an outer positive metal electrode having an open structure readily flown through by the solution ; for example an expanded metal sheet or wire mesh surrounding the porous carbon counter - electrode , insulated from one another by a fluid pervious plastic separator , adapted to be introduced inside a flow conduit of the circulating solution , or immersed in a pool of the circulating solution . suitable leads or equivalent means of electrical connections allows to connect the two electrodes to the positive output terminal and negative output terminal of a dc source 4 capable of delivering a current of up to one or more amperes though the test cell 3 , at the bias conditions of the test cell 3 of selected output voltages that are substantially held constant by a regulating loop of the dc source 4 , for the time necessary to read simultaneously the electrical current absorbed by the test cell 3 at the selected bias condition . voltage - current measurements being performed according to the method of this disclosure are indicated in the block diagram of fig7 by the respective instrument symbols v and a . preferably , output voltage and current measurements should be made without using a sense resistor in series to the test cell in order to avoid corrections of the voltage bias applied to the test cell . most preferably , the programmed output voltage and the measure of the current drawn by the test cell at the constant voltage bias are both extracted as analog signals from the dc source circuitry with commonly known circuital techniques . in particular , the output voltage signal may be drawn from a common resistive voltage divider of the output voltage that constitutes the feedback network of the control loop of a linear voltage regulator that control an output pass transistor . a signal representing the output current may be drawn starting from a commonly controlled scaled replica of the output pass transistor , the scaled current generated by which may be mirrored with the output current and thence a voltage signal proportional to the output current may be drawn from the output branch of a second mirror . of course , a specifically designed circuitry for electrically biasing the cell sensor 3 at a desired supply voltage and for simultaneously sensing the current absorbed by the sensor , may be used also for preliminarily generate a look up table of correlation of the response of the sensor to a plurality of calibration solutions of known degree of oxidation or state of charge . a circuital embodiment of the dc source 4 and of the voltage and current measurement implements , allows the realization of an electronic system capable of managing the powering of the test cell , the collection and temporary storage of voltage - current data pairs and the production of a real - time estimated value of the degree of oxidation or state of charge of a positive electrolyte solution containing a v + 4 / v + 5 redox ion couple of a working redox flow battery cell , as described herein below . as schematically illustrated in a basic exemplary block diagram of fig8 , properly scaled and buffered analog voltage signals representing the regulated output voltage of the power supply biasing the undivided cell sensor and the current absorbed by the sensor , respectively , may be sampled at clock beats and converted by common a / d converters into digital data pairs that may be stored in a work memory , for example a ram . a digital processor correlates every data pair read from the work memory to the correspondent degree of oxidation and / or to the correspondent state of charge of the redox ion couple contained in the positive electrolyte solution flowing in the battery cells , recorded in a look up table when calibrating the undivided cell sensor . the generated estimated data may be compared with one or more threshold values for eventually alerting the operator of the risk of approaching a potentially dangerous high degree of oxidation of the redox couple . data processing capabilities of modern digital processors allows real time execution of computational algorithms over a plurality of sequential voltage - current data pairs read from the ram , for making more robust , precise and reliable the identification of the point on the voltage - current plane of the response to the actual degree of oxidation or state of charge of the streaming solution provided by the biased cell sensor . a pre - filtering of disturbances by a sample data correlation algorithm , may be performed in order to filter out odd data pairs that may be accidentally acquired by the monitoring system . by processing the real time produced estimated degree of oxidation or state of charge of the positive electrolyte solution and the normally monitored ocv it is possible to indirectly estimate by subtraction the state of charge of the negative electrolyte solution and thence the degree of unbalance that may have been cumulated in running the rfb system for a long period or after many charge - discharge cycles . the availability of this information in real time fashion is an attendant important result that is made possible by the method of this disclosure . the various embodiments described above can be combined to provide further embodiments . other changes can be made to the embodiments in light of the above - detailed description . in general , in the following claims , the terms used should not be construed to limit the claims to the specific embodiments disclosed in the specification and the claims , but should be construed to include all possible embodiments along with the full scope of equivalents to which such claims are entitled . accordingly , the claims are not limited by the disclosure . 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