My hard work years. Just out that is undergraduate was doing master's in aerospace engineering I guess. So by a great way back to school here. Thank you very much Tom and I really appreciate the invitation to come to talk to you today have had a really great day. Last night I went out for to a very nice Greek restaurant and have some advice to before you if you ever go on an interview don't drink the Greek coffee the night before your interview you will. I was told not to drink the dregs but even if you stay away from the dregs it can be a challenge but I've had lots of good conversations Doc starting with Dr Lou this morning and and ing with Bill chorus this afternoon. So I've said many times today. I well talk about mention that in my talk so why don't I give you my talking see if I can mention everything the topic is mediated electrode systems who are interested in using enzymes as catalysts primarily for fuel cells which is an example of a system where the rate of electric tells us is important. This is distinguished from sensors. But there's other examples. This is my musical interlude. There are other examples of systems where high rate is important. So the. The fuel cell examples are pictured here this is sort of a classical I made this picture when I was a post-doc of a implanted fuel cell and a blood vessel where the fuel cell can be catalyzed at the cathode by an enzyme like lack ace at the end and I'm like glucose oxidase and the and the blood which contains generally glucose and oxygen can conserve as the reactance for for the system. This is a little bit far fetched from a surgical standpoint but it that it acts as a sort of an initial motivation more simple systems might include implanting a small bio fuel cell in. A fruit like this is a great this is worked on by man. What Heller and University of Texas and ultimately more near term one can imagine using the selectivity of electric catalysts in more practical direct methanol fuel cells where the cathode can be catalyzed by a selective lack a lack a sense I'm and because and the anode can be placed in the same plane as a cathode so that the feed can be a mixed feed of both fuel and an oxidant and it relies on the selective any of these devices so this is an example of a way to to intensify the the fuel cell system using the selectivity of the enzymes a more general approach might be bioreactors using enzymes to do chemical conversions from low value. Fee's like glucose using like mentality hydrogenated to format a tall which is a high value sugar one can take listener all which is a byproduct of biofuels production using. A DI hydrogenation enzyme to produce the ha. Which is done had dropsy acetone which is a tanning agent that you do use in self tanning. OK so. So we can also consider chemical conversions in addition to energy generating devices to make. You added products that are really only obtainable using catalyze reactions and we can couple these reactions so this is a and oxidation reaction this is a reduction reaction so that we can actually do these types of the conversion simultaneously in the same reactor the common themes here are that the these reactions have to be operated at high rate in order to have you know efficient production of electric electrical energy or chemical products and in order to make these devices practical stability is a big concern. So enzymes have some advantages in terms of selectivity etc but they are challenged compared to conventional catalysts by a lack of stability and a relatively low turnover rate. So a common question. In the context of using And sometimes as catalysts electric catalyst is whether they have what it takes to do what's probably the highest power density application for fuel cells which is the automotive application. And so I dressed this sort of doing a very brief analysis using a criteria that was established two thousand and five by gas starter a doll which is the the requirements for a free catalyst. So if one were to replace a precious metal such a platinum with. With a catalyst ideally that replacement would be free because that would overcome the cost issues with platinum and so the activity of a costless Cathy Cathy catalyst really is defined mostly by whether the fuel cell that one would design with this catalyst. Has sufficient energy per unit volume in other words can you put enough catalyst into the fuel cell to get the power that you want and so that the definition that the guest worker came up with is that the activity per unit volume. It's sort of quantified as current per unit volume for automotive applications needs to. About. The order of a tenth of the industrial plant and activities in other words the activity of a platinum catalysts supported on carbon as implemented in an automotive fuel cell. So here's a little table that sort of does the analysis for an enzyme catalyst as compared to platinum. The this is a supported platinum catalyst on carbon forty seven wait percent the conditions for the platinum catalyst and this is a lack ace oxygen reducing catalyst are are at their ideal conditions so the platinum is at roughly eighty degrees C. the lack a says at forty C. the PH for lack a says five the PH for Platinum is around zero at at reasonable high potentials where you want to operate a cathode the turnover frequency for a platinum catalyst in terms of electrons for sight per second is around twenty five the the enzyme itself the lack of self has a turnover frequency as measured in our experiments of around two hundred so just based on the two or frequency the lackeys looks pretty good. The problem of course is that the density of sites for Platinum around three point two So point two times ten to the twenty percent cubic centimeter is almost an order of magnitude bigger than the density for lack A So the reason there's a lack a says a hundred kill a dog molecule. It's very large so the site density is really limiting. So if you multiply these two numbers together you get more or less the current per unit volume and if we see just on a theoretical ideal basis black ace is certainly within the order of magnitude requirement for platinum. So if you if you if we can utilize black ace in an ideal way high utilization high turnover then weren't in the ballpark. However if we really look at a practical device you know this is a practical platinum catalyst we look at a practical mediated lack a system at the same condition. Same more or less same potential a little bit lower the turnover frequencies the same but the additional components that one has to add in order to really obtain high utilization of the electrode lowers the site density by about an order of magnitude which brings the current per unit volume down again by about an order of magnitude. So that sort of brings us out of the range for power application so from a power density standpoint lactase the you know what we can envision doing with like case now is not what you'd expect to do with it for automotive applications and we haven't even addressed the stability aspects which are also a big detriment. However it's easy to show this is work by Matthew and Heller from two thousand and three. It's easy to show that that enzyme electrodes have some advantages compared to platinum on the on the left or polarization curves where the current increases with a decrease in potential for platinum and the same thing for for this is for a bill ribbon oxidase also an oxygen reducing and I mean we can see that the current densities under ideal conditions can be quite high as compared to platinum and most importantly the potentials at which the cattle to tell says Can occurs. This is a minus point two versus the reversible potential of oxygen are higher than the potentials for for play platinum so there's a third a Namak advantage to using an enzyme in the sense that we can catalyze the reaction at a higher potential So there are some advantages. There is commercial interest in bio fuel cells primarily for portable power so for smaller devices where the power density is not as important and energy density becomes important. This is a system that's being developed by Sony. This is a. This is the size of the system it's you know this is an M P three player and this is the size of the system is roughly you know four or five times the size and these are for glucose oxidizing and air reducing. Fuel cells that glucose is is oxidized by an energy age based enzyme which requires additional components to do mediation which we'll talk about a moment in the same thing is true on the Oxygen side and these devices generate on the order of microwatts per cubic center right. Centimeter right now really just barely enough if you have a large device to power the M P three player and so the power density of these devices is really at issue and what is also true is that this device only works for about a minute and then it's pretty much done so. So power density instability or it's are still very much. At issue. So there's two ways that we can extract or inject electrons into an enzyme. One is direct light electron transfer and the other is mediated electron transfer in direct electron transfer one orients the enzyme as closely as possible directly on the surface of an electrode and if the active center is close enough you can have electron tunneling between the electrode surface and the enzyme and that's the most the simplest possibly the most efficient way to to achieve electron transfer. But generally speaking this is hard as I'll show in a moment and the the alternative is to introduce a mobile species a mediator that can and has good kinetics with respect electron transfer at the electrode and then can transport the the electrons to the enzyme and generally speaking at least in our hands these sorts of approaches are more effective in terms of utilization of the enzyme then the direct electron transfer approaches. Having said that there are several examples in the literature where people have used direct like trying transfer to get reasonably high current densities this is a fructose to hydrogenation. And I'm from the condo group in Japan where they have actually measured the order of six million per square centimeter at pretty high over potentials for fructose oxidation. Just to give you a reference this sort of current answer on the order of five or six millions per square centimeter for an enzyme electrode is quite high for a platinum based fuel cell if it's a less than an amp per square centimeter It's not that interesting. So those are the sorts of scales that we're working on this is a lack a scale cathode where the current increases with decreasing potential in the current densities I know you can't read this that they measured on the order of tens of millions per square centimeter quite impressive for a direct electron transfer and then this is a bilirubin oxidase electrode which has similar performance in the million percent of your squared range so it can be done but the mediated systems we've found have been more effective and this is why this is the structure of lack ace in the yellow balls represent the active centers of a lack ace and this is from the the this yellow ball is a copper center called the T one site that's responsible for electron transfer between a CO substrate and the enzyme and so the CO substrate in our case would be the electrode itself and then these three coppers are the T two T three site that's responsible for oxygen reduction all the way to water and so ideally one would immobilize these lack aces and here the coppers are in blue with respect to the electrode surface such that single copper site is oriented perfectly respect to the surface. Every time to enhance electron transfer and there are some chemistry that are being developed to do this but it's very hard and so generally when one does a random approach the orientation is not ideal and only some of the lack a sense I'm zeroing in to properly to achieve directly try to transfer. So this ends up being a less active electrode as compared to this one. Now the alternative is to not worry about orientation by introducing the mediator so what we do is we immobilize the enzyme in a and a hydrogen else so this these lines are intended to be the hydrogen. Backbone and the hydrogen also has complex to it are redux complex that I'll describe in a moment and if the concentration of the Redux complex these purple balls are significantly higher than the concentration of the enzyme then electron transfer via the mediator can can be efficient in terms of getting electrons to these a single copper site. So one it cheese a situation where the orientation of the enzyme is not important one. Also achieves a situation where the does not have to be immobilized directly on the surface and so you can have multilayer the mobilization of the enzyme and this leads to the possibility of higher utilization of the enzyme and higher loading of the enzyme on the electrode surface the challenges are the transport limitations at the electron ultimately is transported to the enzyme by electron hopping between these readouts complex sites and this hopping process is the few gentle in nature and can be characterized by diffusion coefficients on the order of ten to the minus eight to ten the minus ten which is very low especially compared to for example the diffusion coefficients of oxygen which are on the order of ten of the minus five. So the transport limitation both in terms of electrons and if this ends up being a very thick system transport of the oxygen ends up being the limiting process in these systems. So these are the Palmers the Redux polymers that we've we've synthesize in order to study the interaction between the enzyme and the mediator. These are all polyvinyl emitters all backbones to which we've complex and complex and we can choose the Libyans. These are all either by peer again or tour period leggins and sometimes there's two by purity Liggins and a chlorine leg and we can choose these these subgroups on the period eans in order to tune the potential that which this cause. Plex can oxidize So if you use chloride groups the oxidation potential is quite high. If groups X. today some potential is quite low. And so we can span the potential range of almost one full down to almost zero volts to to control the the way that that of that mediator oxidizes and we can use that parameter to study electron transfer rate kinetics between the mediator and lack a sense of. So just to give you an idea of the electrochemistry of the mediators. These are cyclical down time of Graeme's where we scan rather quickly. The potential of the of an electrode on which the this mediators are immobilized and then we return in the oxidation reduction peak sort of define the Redux potential of the electrode in these range over a broad range for each of the end of the mediators we can also use the peak of the cycle for time gram to estimate activity and we can use these sorts of measurements to also measure transport rates of electrons in the meter. The way this can be put into a fuel cell is described here. This is a bill. Reuben oxidase cathode where action is reduced to water. The electrons are transported from the electrode through the mediator to the enzyme and then to to the to the oxygen where it's reduced the water and so they're traveling up a potential gradient So the electrons like to go towards positive potentials and the rate of electron transport in this direction depends on these potential jobs. The larger the difference in potential between the mediator and the larger the jump and the same thing is true out and at the anode where our glucose is oxidized and those free electrons also travel up the potential gradient and then go to the cathode and so when you look at the system. There's a. Several different potential differences involved. There's a thermodynamic potential difference between the glucose in the oxygen the two reactance which is fairly large there's the potential difference between the two enzymes which is slightly smaller and then small Saval is a potential difference between the two mediators and this potential difference in operating fuel cell really defines the potential of the operating fuel so. So in order to drive electron transfer between the mediator and the enzyme one needs a large potential difference between the mediator in the enzyme in order to have a high of cell potential and remember power in a fuel cell is potential times current one has to have a large difference. In tension here and so there's a tradeoff between the kinetics of electron transfer and the potential of a cell which is a classic trade off and. In electro chemical solve side. Also there's other issues involved for example the mediator is competing with oxygen if it's present for the electrons glucose oxidase which is a typical glucose oxidizing and uses oxygen as its natural course substrate and so there's a natural ability for glucose oxidase to reduce oxygen to proc side which scavenge is electrons. So the difference in potential between the mediator and the glucose oxidase also controls its ability to compete with with oxygen for electrons. So these are quote unquote steady state polarisation curves these are sweeps of the potential in the presence of oxygen and the lack a C. and also mediated by the various mediators and what we can see this is for a fairly high potential mediator as we reduce the potential the current starts becoming negative which means that we're reducing oxygen and it becomes negative more or less at the potential redux potential of the mediator and then it levels off at some potential where where the. MEDIATOR is fully reduced and there is no potential dependence whatsoever. And this plateau is controlled primarily by the kinetics it can be controlled by mass transfer it can also be controlled by the kinetics of of oxygen reduction. It can be controlled by the kinetics of electron transfer between the mediator and the enzyme So this this this polarization curve is a cople pated interpretation of all the processes involved in the electrode and we can show similar results for a lower potential Palmer and we can see that for a low potential polymer generally speaking we have a higher current which indicates faster kinetics at a lower potential and we can add all of the pollers and we can see this is a fairly messy when we look at all the cycle full time grabs but if we plot the plateau current as a function of mediator potential we see a very general trend of increasing current density with decreasing mediator potential it's not a complete trend because some of the polymers. Are not really following the trend at all in the there's several reasons for that having to do with transport and other artifacts in these experiments that have to be accounted for and so the next step in this process is to start a colony for those things to do that we developed a relatively simple transport model of this and I mediator film just taking into account diffusion and transport of oxygen into the film and diffusion and transport of what Trons from the other side we use a very simple Ping-Pong Bye-Bye mechanism that involves a turnover rate and to Caylus constants and we use this to experimentally a while before we use this model we experimentally obtain the fusion coefficient for the mediator and I'll show those results next and then we use that diffusion coefficient to actually determine the kinetics of the reaction and if you look at these pla. What's the trend transport of oxygen. This is the C.S. is the concentration of oxygen coming comes in from the right it's more or less flat and so that the transport limitations do not involve oxygen in most of these experiments on the other hand the mediator which has again the lower diffusion coefficient is transport limited and sometimes the rate the reaction rate follows the meter concentration. Sometimes it does not is that it really depends on the saturation of the media in this ratio of of K.-M. to the media. Reduce mediator concentration. If that concentration is high the system is saturated and the rate is constant if it's not high then there's a dependence. So we measure the diffusion coefficient of the mediator using the control technique where we where we plot the current as a function of time after a potential step and that's just a transit measurement and connect if we plot it correctly we can extract the slope and extract the diffusion coefficient directly and generally speaking the diffusion coefficient should follow a linear model with respect to the concentration of the osmium redux complex in the readouts Palmer and so after measuring all the diffusion coefficients we can make a plot and we find that yes indeed. The diffusion coefficients do follow that linear relationship. So what that one main conclusion that is that not only does the Redux potential of Palm but also the concentration of the Redux complex in the Palmer has a significant impact on the diffusion coefficient and as you might expect on the overall rate. So having designed the model and obtained diffusion coefficients to account for transport within the electrode film we can go ahead and extract kinetic constants from the system and again we're using this simple system where we can the main constants that we can extract are the. By molecular weight constants for the mediator which is just K. Cat divide by K. M. and then the by molecular a constant for the substrate oxygen and these are plotted here as a function of mediator potential which is what one of the main parameter that were varying and you can see that as the potential decreases. There the kinetics generally increases. This is an exponential scale so they include increase exponentially and then flatten out and essentially what that means is that the kinetics reach a point as at which they are internally controlled by electron transport processes within the enzyme and in which case the potential of the mediator is not important and in contrast the by molecular weight constant for the substrate is more or less flat which is what you'd expect. So this information can be used for design purposes and just as an illustration we can we can predict the performance of a hypothetical bio fuel cell as a function of the mediator potential we can plot the current of the fuel cell just using a simple exponential rate function as a function of mediated potential and we see that as as I mentioned as a potential decreases the current increases up to the point where which is this plateau where again the kinetics are controlled by an internal mechanism in the end zone. But if we plot the power of the system which is essentially this potential multiplied by the current We see a plateau and so this hour we see an optimum and this optimum defines the mediator potential for this hype is that hypothetical cell which is is optimal for a real fuel cell. So we we've done a kinetic study and use the results of the kinetic study to actually design the mediator for this hypothetical. Electric. Also there's several prime ministers of the. Of the beater that are important that we've also studied in terms of synthesis details. For example that I mentioned that the concentration of the mediator is important to a point. It can help to a point. It starts to hurt and also the ratio of the mediator to the monomer of the backbone can also be an important and just looking at a very simple study where we've increased the concentration of the polyvinyl images all increase the concentration of the osmium and then a very at the ratio of the polymer backbone to the mediator we see that a very interesting result if we look at the cyclical Tammy tree. We see that the peak for these high concentration mediators are more or less the same and they both lead to increased current density in a complete electrode but the but where as these peak eyes are about the same would suggest that the diffusion coefficients are about the same the the plateau current density meaning the maximum current density of the electrode is different and so the indication there is that there is a and that there is an impact of swelling of this hydrogels on the kinetics of the electrode more water higher osmium concentrations lead to lower water intake into the electrode and that has seems to have no impact on. Electron transport but for some unknown reason has an impact on the the catalyst activity. So what if what have we done so far the in our interests is you know generating higher power density by generating higher current density and we've done that by first and Hansen electron transport to the enzyme we've we have this one dimensional film where we have this the hydrogels essentially the light blue air. And it contains an enzyme worth of which are the pink things and then there are purple balls which are the mediator. And we've designed the mediator to enhance electron transport. But another thing that we can do is to facilitate electron transport with composite materials and so the next step is to introduce composite supports that allow electrons to be transported via the solid phase and increase the activity of the enzyme by reducing the distance over which the mediator has to act. So that's something I'll describe next we could also introduce these carbon phases and we tend to make the electrodes a lot thicker which introduces transport limitations on oxygen and one thing that we can do to enhance oxygen transport for example is to introduce a gas phase for oxygen concentration and the defensive auction are much higher. And so we'll show a little bit of preliminary data on that but going back to the carbon materials what we like to do is to start again with this one dimensional film and what I did as post-doc is to to to introduce a carbon paper composite where we use. Roughly ten micron diameter fibers on the order of one hundred microns thickness and and immobilize the ends of hydrogen within these fibers and see that's the box. I want but just by introducing this this carbon material we increase the surface area of the electrode by a factor of fifty and the measured current density increased by a factor of five compared to this more or less one dimensional film. And then the next step is to start adding surface area so we want to maintain this the structure of the carbon fibers in order to maintain. Mass transport within the structure but. We want to enhance the surface area of the material by growing nanotubes on the structure and in doing so we increase the surface area again by a factor of one hundred and and the ultimate result in terms of current density is an increase by a factor of ten. I'll show you that in a second. So this is the way we work with the carbon materials we start with a with Tory paper which is again these ten micron carbon fibers and we've set it up in a room temperature chemical vapor deposition system or we pass a current through the carbon paper to heat it up and we Simon Taylor simultaneously send a gas precursor feed just typically carbon monoxide and hydrogen through the carbon paper in order to facilitate chemical vapor deposition of the growth and we have a catalyst which is generally in our nanoparticle we have a couple ways of delivering the particles either prior to the to the chemical vapor deposition we can deposit them from hexane or we can actually use a gas phase iron for example our input to Carbondale to mobilize the catalyst and this is the sort of growth that we get. This is the bare Tory paper that you might have seen before and as we grow for one minute understood our baseline conditions we start getting a little bit of follows on the carbon fibers and as we go for five in ten minutes the growth is is messy but at substantial we get roughly a doubling of the diameter of the fiber due to the nanotube growth. And we can take those materials and load them with an enzyme and with a mediator and measure the the kinetics of tells us and in this case we're going to use the media. We're going to use a low potential polymer. And it's going to be used to mediate tells us. Glucose oxidase So now we're going to be doing making an ode that oxidizes. So the current density will increase with increasing potential and what we have plotted here the polarization curves for an electrode immobilised on this scale material where the negatives have been growing for with zero one in twenty minutes so this is Bear Tory paper the black and we increase the current density by a factor of ten. By growing nanotubes for about twenty minutes. We can also plot the this current density as a function of growth time and we can compare it to the current density surface area measurements we can do in two ways one is using just physics Orcs and the other ways to use electric chemical capacitive measurements and those two measurements are more or less the same the the capacitive measurements at the high an attitude grosser are ninety percent of the tea which means that there is a limited electrolyte accessibility to all the surface area that we've created. But the current density jumps up very quickly at fairly low growth times and then levels off so that is an indication that the surface area that we're actually utilizing is really is relatively low compared to the total that we're growing so one of the things we're working on now is to try to improve the utilization of the surface area so that we can activate more of the enzyme. We can also immobilize a lack a sense I'm oxygen reducing enzyme and these materials these are the same these the same polymers that we showed before where these are very high. Osmium low to high P.P.I. precursor concentrations and we can get current densities just as a point of comparison the current densities for glucose oxidase are on the order of twenty million answer per square centimeter for lack a sense. We've been able to cheat on the order of ten so so it is a rather high current densities for an enzyme based electric. We can make a complete cell with combining these two electrodes and the way we do that is to use a commercially available flow through cell that has a two glassy carbon electrodes on which we can essential glue using carbon paint. The Tory paper based Aleck TROs one for the cathode and blue one for the anode in red and we can flow a mixture of oxygen and glucose solution through the cell in order to feed the cell and then polarize it using the glass to carbon electrodes. And if we use this high surface area material on both the end of the catheter we can take advantage of the high utilization. So this is a just a quick pull or there's likely to lots of data on this but here's a colorization curve for the cell the key numbers are that we can generate about a half a mil a lot per square centimeter. Using the cell and if you divide by the total extra area. It's twenty one million watts per cubic centimeters so it's a fairly active system. What's interesting is that glucose oxidase is active primarily at PH seven the lack a sense has its maximum maximum activity at PH for so I'm in order to balance these things we have to operate the system at. Intermediate ph and we used five and a half. So that's where that's where the state it was taken. Stability is an issue and just to give you an indication of. Of how unstable this sort of system is this is the two hundred fifty micron paper carbon paper. It's essentially the twenty million per square centimeter glucose oxidase electrode that I showed you and it. The decay in the current as a relative to its initial current is plot. As a function of time. This is what I hope to be exponential decay and you will see if it's exponential. But the time constant if and we usually use the half life of the electorate as a time constant is on the order of seventy sixty seventy hours which is you know roughly three days or so. So it's a it's short lived and there's a variety of sources of degradation the enzyme can unfold the mediator is as a redux active material that can that can that can easily be chemically deactivated running flow through the cell leads to chemical stress and other sorts of stresses for example oxygen present at the glucose oxidase and can generate proc side as I mention and that can lead to chemical stress so the sources of instability are myriad and we're trying to tease this sort of data apart to start looking at stability as a key issue in bio fuel cells. Some other key issues. Gas phase activity I mentioned that we'd like to deliver oxygen the substrate at for cathode in the gas phase to enhance its mass transport. This is sort of the preliminary data we have for that this is current density as a function of time for a cathode. Operating in the presence of gas phase air and gas phase oxygen and we also introduce unification to both the air feed and the oxygen feed to see how to what extent water and in the gas fee can have a stabilizing impact on the electrode. Well the answer is it has a big impact on the air electrode but we really don't know why yet but it has a negligible impact on the Oxygen electrode the current densities here are pretty comparable for both oxygen and air but the air Lector is much less stable. It has a life time of about three hours or so the oxygen electrode seems fairly. Stable and if we go out to you know longer times around ten hours it's it's reasonably flat but as you might expect we're. One rarely designed a fuel cell system to run on pure oxygen because it's not readily available so as a as enlightening as this might be actually it's really challenging because of the humidification has no impact. It's really not a useful device and we really want to be able to operate on dry air and extend the stability out to sea to at least several hours. More challenges. I've talked about power density have talked about stability. We'd also like to increase the energy density of the system and if one uses for example a high molecular weight fuel glucose is a good example has twenty four electrons. For a molecule of fuel. If you oxidise it all all the way to carbon dioxide methanol also has multiple of transfer molecule. If you oxidise it all the way to C O two and there's a no there you can extract six electrons per mile. CULE but from an enzymatic standpoint that requires multiple enzymes steps a classic methanol oxidase oxidizing and so relies on alcohol the i Drive aldehyde hydrogenation for me. Do you have drive all of which are require the any any D.H. co-factors So we're working on systems in in which we can achieve this carbon dioxide full oxidation with a system and ultimately what we'd like to do is to go after something even more complicated which would be the glycolysis cycle in the Krebs cycle which doesn't achieve that complete oxidation of glucose to carbon dioxide. This is a subset of the curb cycle that highlights that the relatively few electro chemical reaction steps the malady has drugs and a step. Situate headrush in a step there are several other steps that are not electrochemical that are required in order to go through this entire process and ultimately we'd like to add the rest of the loop at the glycol so cycle at the top and achieve complete city. Other projects. Well a collaboration with Scott pad to Columbia University in which we're looking at complete peptide based hydrogen mediators where we can take the well known Lucene zipper coil coil and use that as a way to self assemble peptide chains into a complete hydrogen. And if we take in osmium complex and attach it to the histidine the images all ring on the histidine we can take that self assembled peptide hydrogen. And turn it into a mediating hydrogen. Also we can take this super and attach it to a recumbent it ends on this is a small Lac ace or slack that we've used for our initial studies and with that we can take we can we can more or less create a fully biologically derived and sign hydrogen composite the only chemical step is the complex ation of the Hydrogen will with the osmium. And we can demonstrate this of all that the these of peptide hydrogels have redux activity by doing cyclic full time three. This is the the free complex. This is the complex attached to the to a couple of different peptide hydrogels we can add the enzyme and do cycle do electric chemistry as well. The this is the polarization is a little different that you seem because we don't see that that plateau but we do get current density at low levels at real cell potential. So just to wrap things up. I've showed you some of the results of using mediated by. Trodes for high rate electro chemical conversions primarily for fuel cells but also for chemical conversions. I've talked a little bit about the hurdles that we've been able overcome primarily in terms of activity and the challenges that we still face in terms of stability and there's multiple ways to address these problems through you know bio chemical protein and generic approaches but also in terms of the mid materials that are used to immobilize the inside. We we achieve more or less maximum power using mediated systems but we introduce complicating factors insensitivity to the environment stability are the main ones. Just last I like to acknowledge my students Josh Galloway. And you have son have all been of all graduated. Let's talk Morty and how I entered my first two students at Michigan State Jim Hall and help as a collaborated with the. Chemical vapor deposition experiments. I work with Shell and tear on the experiments and I've also mentioned Scott banter with the peptide and there's my fun. So I appreciate your attention and I'd be happy to answer any questions. You take place where you please. If you look for truth will go away the whole of looking you are more wise in comparison. So all of the experiments that I showed you were mobilized. So I think I only showed one experiment that was in solution. So the enzyme to the picture to keep. Right there is the picture to keep Is this one. So these are this is our platform. This is the hydrogen of the blues the hydrogen. The the purple is the mediator it's the redox complex that's attached to the polymer backbone. And the enzyme isn't trapped within the hydrogels well. And so this is the way we do our experiment so the question though is how do these things operate in a hydrogen as opposed to free solution. Well at the answer is that the enzyme activity is more or less the same the activities that we show or hundreds of. The turnover rates are in the hundreds very comparable to what one sees in solution that the transport the fact of the matter is that in this system these little purple balls they don't actually move. In the system and so if you have a diffusion a mediator where the molecule the complex molecule actually moves then the diffusion coefficient that one would measure would be again on the order of ten the minus six to minus five and so that that is one of the big differences is that the electron transport which is the fusion of all is slowed down dramatically by the immobilisation of the complex but if the film is thin enough and thin for us as a micron or less then even that transport limitation is not overwhelming. Yes. Yes. So we haven't done that copulation but we could these are multi-well nanotube So it's a little bit messy to to think about to to think about for example the the volume fraction of that layer that's occupied by carbon because where it. We don't know the answer to that but what we'd like to do it to answer your question in this is ongoing research we'd like to vary that density. For example by varying the catalyst site density in order to open up. That nano scale structure and. And hopefully increase the utilization of that surface area with the enzyme So we haven't done that we're working on that and that involves controlling the the Nano to growth catalyst deposition process. In addition to the growth of the negatives themselves so it's a very good question that we're working on answering right now. Now. There was a moment. That's very easily studied by just looking at the ohmic resistance of the of the system for example in the absence of stub substrate we can do cycle full time a tree and obtain the ohmic resistance of the electrode and generally speaking that resistance is very low. So that the comic to be of the nanotubes is negligible compared to all the other resistances in the system. Yes absolutely. That's a good that's a good question. I'm in the case that I showed you which was glucose oxidase immobilised on the. Nanotubes I can't give you an unequivocal answer but I'd say almost certainly not and the reason is that no one has demonstrated direct electron transfer using glucose oxidase at all. There's no literature on that you can do electron transfer between the Nano to end the enzyme centrally charge and discharge the enzyme that has been shown but getting electron to go from the glucose to the enzyme to the Nano to the direct elect. Transfer is NOT been shown. So in this case for this data I don't think that is a problem. However if we had used a different enzyme like Ace is actually an enzyme where direct electron transfer has shown to be relatively efficient then it's certainly possible that there might be a mixed mode in which there's you know we have a hydrogen that contains the enzyme that's not attached to the carbon surface and then it's tubes and then we have some enzyme that is attached and that that enzyme that is attached would probably be more or less successful in direct looked on transfer and then the stuff that's out in the middle of nowhere with just a mediator would probably be mediated. So in it with a different enzyme a system. I think you could probably have a mixed mode. Yes. I can comment on that let's see where is that. I have to go to that slide. This is. So this is one study that we used to. To quantify that. So what we have here. The main plot is just the decay in the catalytic current density as a function of time and it's more or less exponential what we have in the inset is a cycle of all time. A gram. In the absence of substrate. So this is an indication of the activity of the mediator self not the enzyme and what we see is that there's a after roughly that the half life of the electrode is reached. In other words the activity total activity then time has gone down by fifty percent. We see roughly a twenty five percent decrease in the activity of the mediator itself so one way to think of this and I think this is quantitative this point is that whereas the overall decay was fifty percent the meter decay was twenty five percent so so it roughly half of that decay can be associated with the mediator half of the decay so share with the enzyme. I think that's a qualitative answer I don't think it's a complete answer but it gives an indication that both both materials have a life time issues. So the question is Is this a function of the media that we use and the answer is I don't have that data we haven't done those studies. At least I think I haven't seen the results they might be available for my student. I'm not sure about that. Good question. But it seemed like still there was a lot of theory that we will be wrong. Actually Or simply wrong. Just now putting it in and using that paper. From the road. Sure if the. In our experience it. The answer question it depends on whether how you handle the electrode. So an obvious. And in my mind at least an obvious approach would be to skip the Tory paper skip the cart's chemical vapor deposition and just buy some nano tubes from small tubes and mix them in with the hydrogen solution that put them on an electrode and what we found is that by for example cycle full time true we can measure the surface area available surface area of the nanotubes and under those conditions and it's very low so that means that what's happening is the negatives are being compacted into a fairly dense layer and because of that the surface area availability is low and that the activity of the electrode is low so what the what growing. We're still working on that approach because it's a lot simpler than using chemical vapor deposition and it. It's much more scalable in terms of actually making electrodes so there's we're working on ways to deal with that but what this does is allows us to you know route the nanotubes on the carbon surface and and provide structure that will prevent agglomeration unpacking and the Tory paper itself. Also provides Micron scale prosody that enhances transport of substrates in and out. So if we were to grow the nanotubes completely fill. We have a mail of do that I'd love to be able to do that we're working on ways to achieve complete filling of the Tory paper with with nanotubes but the expectation is that at some point you'll run into substantial transport limitations that so that there's an optimum there that were there where we're reaching for.