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Team:Stanford-Brown/Projects/BioWires
Contents |
Introduction
Nanowires are integral to the miniaturization of computing and communication devices, and are used in everything from quantum computing to mind-machine interfaces. Limited by standard synthesis techniques, they are expensive and impractical. OUR SOLUTION IS DNA.
Imagine if nanoscale electronics could be synthesized, not by enormously expensive and over-sized lithography machines, but by factories visible only by microscope. Imagine that the machinery required were ubiquitous, and that the parts within a common gut microbe could be harvested for the nano-fabrication of electrically-active materials. Further imagine that these materials could self-assemble into highly ordered states to form coils, bundles, sheets. What could you build with a system like this?
We present BioWires, a thoroughly tested DNA-based nanowire system engineered to manufacture quasi-one-dimensional metals in PCR tubes.
Mechanism
Our system of choice is DNA, a self-replicating, self-assembling, and often self-catalyzing biomolecule that arranges itself to form long filaments. These chains are held together by hydrogen bonds, and are arranged in a sequence-specific manner. Standard DNA is not conductive enough to build useful constructs, and as such we have modified the basic structure of the molecule for the purpose of enhancing conductivity.
Drawing upon the work of the Ono group (2008, 2011), we have modified DNA by engineering C-C mismatches into short oligonucleotide duplexes. The hole left by a non-bonding pyrimidine pair is selectively filled by a single silver ion. Due to the sequence specificity of DNA, these duplexes can be patterned with varying silver distributions. We have demonstrated that this system is thermodynamically robust, and have identified and bricked sequences which intercalate silver particularly well.
Example of a 2-1-2 ion distribution pattern (BBa_K1218026):
5’ AAA CAT TTA CCA CCT CCT CCA CCT TAT AGT TT 3’ ||| ||| ||| ••| ••| ••| ••| ••| ||| ||| || 3’ TTG TTA AAT CCT CCA CCA CCT CCA ATA TCA AA 5’
We propose a variety of applications (wave generation from nanocoils, sheet design for circuit patterning) using DNA origami, and are currently testing whether our strands demonstrate increased conductivity. We have successfully established BioWires as a synthetic biology platform for nanowire assembly, and ultimately hope to show that it is more effective than other systems for nanoscale electronic arrays.
Protocols
Protocols for the various tests can be found in the document below.
Silver was added as AgNO3. We used a variety of buffers, and recommend for future teams to avoid chelating agents such as EDTA, which outcompete the DNA for silver ions. We determined that 100mM NaNO3 + 10mM MOPS at pH 7 was the ideal buffer. We also successfully utilized an ammonium acetate buffer for NMR and phosphate buffer for mass spectroscopy. We also note that the silver intercalation can survive isopropanol precipitation as well as buffer exchange.
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Lab Notebook
Our experimental progress, updated throughout the project, can be found in the BioWires Objectives document.
Our experimental notes can be found in the BioWires Lab notebook:
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Data
The BioWires system underwent rigorous testing thermodynamically, chemically, electrically and visually. The data below illustrates the success of the system.
Thermal denaturation: thermodynamic evidence of silver binding
For this experiment, we sought to unequivocally prove that there was silver uptake by our DNA. To do this, we annealed highly-mismatched oligos of 28 and 32 base pairs in two conditions: Ag+ (silver present) and Ag- (silver absent).
It is known that when double-stranded DNA is heated, it “melts,” or experiences a breakdown of its secondary structure. Beer’s law states that for a fixed volume and molecule, absorbance is proportional to concentration. As DNA melts, the concentration of nucleotides doubles, and the absorbance will increase similarly.
To show intercalation, we hypothesized that for highly-mismatched strands, annealing will only occur in the presence of silver. Conversely, those strands should only show an absorbance increase with temperature if they were annealed with silver. That which does not anneal will not melt.
We tested a variety of strands, but two were selected for their strong annealing efficiency. They were a polyC strand (28 cytosines), and a 32bp strand with 10CC mismatches (now BBa_K1218026). This test was highly successful.
The graphs below are the average of three trials, plotted for %change in absorbance over increasing temperature.
FRET analysis: further evidence of silver binding
We repeated this experimental setup with a FRET-labeled hairpin. FRET-labeling entails the placement of a fluorescent marker on one end of an oligonucleotide and a fluorescence-quenching molecule on the other. When the strand is not annealed, it will fluoresce. When annealed, it will be quenched.
We used a 42-base nucleotide that hairpins to form a 21bp duplex with 8 mismatches. This strand was also expected to melt only when silver was present. Melting is evidence that silver was intercalated, which is demonstrated by an increase in fluorescence (melted strands do not get quenched by the union of fluor and quencher).
We melted DNA that had been annealed with varying levels of silver. 900nM Ag represents a 1:1 molarity between mismatches and silver, which is the expected saturation point of the system. As with the previous test, we showed that the presence of silver allowed duplex formation in mismatch-complimentary strands. . Our error in this system was higher than we’d hope, but in conjunction with other tests adds to the richness of the data confirming the system.
PAGE: electrical analysis of duplex formation
We hypothesized that a DNA duplex with silver ions would have a different net charge than non-ionized DNA. The resolution of our gels was insufficient to resolve this charge shift, and we are using electrospray ionization mass spectrometry to help visualize instead.
Poly-acrylamide gel electrophoresis (PAGE) was, however, highly successful as producing visual representations of duplex formation, and we used this method to demonstrate that as a 1:1 molar ratio between CC mismatches and silver ions is reached, duplexing occurs. We used a variety of silver concentrations to anneal a 32bp10CC strand (BBa_K1218026).
We tested undersaturation (<1:1) and oversaturation (>1:1) of the system, and showed the duplexing point. Duplexing beame visually apparent at the 1.5:1 silver to mismatch ratio, which is slightly higher than expected. Nonetheless confirms both the role of silver in annealing mismatch-complimentary strands and that the set point of the system is near a 1:1 ratio.
Phen Green: chemical analysis of silver uptake
To further prove the uptake of silver by our system, we decided to test the presence of silver directly. We hypothesized that an increase in the number of mismatches should increase the amount of silver taken up by the DNA, which should be visible with the use of metal-sensitive dyes.
Phen Green is a fluorophore that is quenched when it chelates metal atoms. To test for the presence of silver in our strands, we annealed several sequences with varying numbers of CC mismatches (0CC, 3CC, 6CC, 10CC with silver. We then precipitated these strands out of solution using isopropanol to remove the aqueous silver. When resuspended, Phen Green was added and fluorescence was measured.
We demonstrate that as the mismatch/ion number increases, the fluorescence of Phen Green decreases. Thus, the more mismatches there are, the more silver is taken up by the DNA. This confirms that it is in fact the mismatches that govern silver uptake. There was a high degree of error in the system, though the trend is still apparent. In the future, we would like to try this test with a dye more closely suited to silver-binding, as Phen Green is not the ideal silver-chelator.
TEM: Visual analysis of particle pairing
We used transmission electron microscopy (TEM) to visualize our DNA directly. We hoped to directly identify the presence of silver in our samples. This was easier said than done, yet we used software to analyze the images that suggests that such a feat is possible.
We used a sputtering technique to coat our samples with platinum ions. This allowed for a better visualization of the DNA, though it provided no analytical data (platinum masks the silver). We were excited by the striated nature of the DNA, again confirming that we were able to form duplexes. This DNA was supercoiled due to the sample preparation procedure, but was intriguing nonetheless.
We then used a negative staining technique to visualize different samples to extract information about the structure of the strands. The high resolution images showed a mass of DNA, but we were able to analyze these images using ImageJ, an NIH-provided software for image analysis.
Under TEM, electron-dense areas such as silver are expected to shine brightly, while the low-electron DNA is expected to show up as a dark spot. We used our 32bp10CC strand (BBa_K1218026), which has a silver ion pattern of 2-1-2:
5’ AAA CAT TTA CCA CCT CCT CCA CCT TAT AGT TT 3’ ||| ||| ||| ••| ••| ••| ••| ••| ||| ||| || 3’ TTG TTA AAT CCT CCA CCA CCT CCA ATA TCA AA 5’
Thus, where silver is present inside the DNA, it should be at a known distance from other particles. With this in mind, we used ImageJ to find all particles within 30% of the silver ion size (2.4Å diameter, or 5.8Å2). We then measured the distance of the center of each particle from nearby particles. As expected, we saw local maxima at the distances representing distances of one and two base pairs (3.4Å and 6.8Å, respectively). We did this measurement manually using the software, and are in the process of using Matlab code to do the same process, albeit at a higher fidelity. Local maxima at integer multiples greater than two base pairs were not observed, likely due to the supercoiling of the DNA.
In sum, by using TEM, we were able to visually demonstrate the silver ion distribution across our samples, providing even further evidence of the robustness of our system.
Data in Progress
In addition to the tests we demonstrated above, we are in the process of running a variety of other assays on our samples. We hope that with the addition of more structural and electrical testing, we will have a fully described system. All of the following tests are currently being prepared or run.
COSY-H NMR: Bond site confirmation
Per the literature (Torigoe 2012), we want to confirm the specific bonding site of the silver as being the N3 nitrogen in the cytosine ring. This will be accomplished by testing a 25bp AT palindrome with 1 CC mismatch in the center of the strand. We have noted that this sample can anneal both in the presence and absence of silver. We will be able to see a shift in the H5-H6 cross peak under COSY-H nuclear magnetic resonance (NMR). We wanted to avoid radioisotopes of nitrogen, and thus elected to test indirectly by looking at the hydrogen atoms in the ring. This test has, however, been established in the literature, are we are certain that a shift in this hydrogen peak will be a simple solution to demonstrate that Ag+ is binding to the N3 site on cytosine.
ESI-MS: Binding efficiency and molar ratio
We are using electrospray ionization mass spectrometry (ESI-MS), a non-fractioning mass spec method for analyzing charged molecules, to directly count the number of silver ions intercalated in the DNA. We want to know what the efficiency is of silver uptake by the highly-mismatched strands. We also want to confirm that a maximum of one ion per mismatch is taken up, and that a 1:1 ratio of silver to mismatches is the idea sample prep procedure.
To do this, we prepared two different sequences. The first was a 32bp10CC strand (BBa_K1218026) with space for 10 silver ions. We will find the number of strands with 10 ions as a proportion to the total number of strands. We also prepared a 25bp AT palindrome with one CC mismatch and annealed with one, two and three equivalents of silver to determine whether a 1:1 silver to mismatch ratio was kinetically sufficient for uptake of silver.
X-ray Crystallography: Solving the structure
We further wished to know whether the intercalation of silver by DNA caused any structural differences in the duplex. We hypothesized that this event could cause either a bulge in the 3.4Å diameter due to ion size or a compression due to ionic forces from the charge shift. We also hypothesized that the intercalation event could alter the tensility of the strand and affect the 10.5bp/helical turn ratio.
To test this, we prepared a 10bp duplex with five CC mismatches and a one base AT overhang to enhance crystallization. This sample is currently being crystallized to determine the structure.
Spin-Coupling NMR: Type of transport
In order to test conductivity, we devised two tests. The first test is to use spin-coupling nuclear magnetic resonance (NMR) to determine the quantum spin state of the silver atoms in the samples, which will enable us to understand the kind of charge transport that is occurring in our strands.
We prepared three samples, each 32base pairs long: 32bpNOCC (0 mismatches), 32bp10CC (10 mismatches, BBa_K1218026), and 32bp26CC (26 mismatches). These samples were annealed with a 30 equivalents of silver, or just larger than a 1:1 silver to mismatch ratio for the strand with the most mismatches. The samples were then desalted, and all aqueous ions were removed. Results will determine both the transport that is occurring as well as how ion proximity affects this transport.
DC Testing: solving for conductivity
We ultimately want to know the conductivity of our samples with respect to standard DNA. To do so, we are devising a protocol to use vacuum filtration on DNA to produce a film, which can then be placed on a direct current (DC) chip that will measure impedance. With this, we will be able to solve for conductivity. We have prepared samples in the same de-ionization method as for spin-coupling NMR, and are experimenting with film production. With this, we will be able to conclusively test the conductivity of our strands. As the conductivity of DNA is a volatile subject, we are taking the utmost care to ensure our method will be immune to confounding variables such as salt charges, strand bundling and extra-DNA silver.
