Open Access Article
Anand Bala
Subramaniam
a,
Mathieu
Gonidec
a,
Nathan D.
Shapiro
a,
Kayleigh M.
Kresse
a and
George M.
Whitesides
*abc
aDepartment of Chemistry & Chemical Biology, Harvard University, 230 Mallinckrodt Bldg., 12 Oxford St., Cambridge, MA 02138, USA. E-mail: gwhitesides@gmwgroup.harvard.edu; Tel: +1 617 495 9430
bWyss Institute for Biologically Inspired Engineering, Harvard University, 230 Mallinckrodt Bldg., 12 Oxford St., Cambridge, MA 02138, USA
cThe Kavli Institute for Bionano Science, Harvard University, 230 Mallinckrodt Bldg., 12 Oxford St., Cambridge, MA 02138, USA
First published on 4th December 2014
This paper reports the development of Metal-amplified Density Assays, or MADAs – a method of conducting quantitative or multiplexed assays, including immunoassays, by using Magnetic Levitation (MagLev) to measure metal-amplified changes in the density of beads labeled with biomolecules. The binding of target analytes (i.e. proteins, antibodies, antigens) to complementary ligands immobilized on the surface of the beads, followed by a chemical amplification of the binding in a form that results in a change in the density of the beads (achieved by using gold nanoparticle-labeled biomolecules, and electroless deposition of gold or silver), translates analyte binding events into changes in density measureable using MagLev. A minimal model based on diffusion-limited growth of hemispherical nuclei on a surface reproduces the dynamics of the assay. A MADA – when performed with antigens and antibodies – is called a Density-Linked Immunosorbent Assay, or DeLISA. Two immunoassays provided a proof of principle: a competitive quantification of the concentration of neomycin in whole milk, and a multiplexed detection of antibodies against Hepatitis C virus NS3 protein and syphilis T. pallidum p47 protein in serum. MADAs, including DeLISAs, require, besides the requisite biomolecules and amplification reagents, minimal specialized equipment (two permanent magnets, a ruler or a capillary with calibrated length markings) and no electrical power to obtain a quantitative readout of analyte concentration. With further development, the method may be useful in resource-limited or point-of-care settings.
Bead-based assays are typically read out by fluorimetry,6 chemiluminescence,21 or colorimetry.22,23 These methods rely on measuring the intensity of light, and require electronics and signal processing to obtain a quantitative readout. Qualitative colorimetric readouts that use the naked eye are subjective, and thus subject to error. They may also be biased due to variations in the intensity or the quality of the ambient light.21 Alternatively, an electrochemical method, which requires electrical power, can be used to read out a bead-based assay quantitatively.20 A fundamentally new technique of reading bead-based assays – one that provides an alternative to electrochemical methods, and that does not measure the intensity of light – has the potential to be useful, especially if it offers a means of quantitation that does not require electronics or electricity.
This paper reports a bead-based assay – a Metal-amplified Density Assay (MADA) – that is based on detecting a change in the density of a bead; it is read by monitoring the levitation height of polystyrene beads presenting biomolecules (e.g. proteins, antigens, antibodies, or nucleic acids) on their surfaces in a Magnetic Levitation (MagLev) device, following a step in which analyte binding-events cause electroless deposition of metal on the bead.
The MagLev device consists of two permanent magnets arranged coaxially with like-poles facing.24 Due to opposing buoyant and magnetic forces, diamagnetic beads – when suspended in a paramagnetic solution in the MagLev device – levitate at a static ‘levitation height’ against gravity.24–34 The binding of target analytes (i.e. proteins, antibodies, antigens) to their cognate ligands immobilized on the surface of the beads causes a change in density that is too small to be detected conveniently. Chemical amplification of the binding in a form that changes the density of the bead (achieved by using gold nanoparticle-labeled proteins and electroless deposition of gold or silver on these nanoparticles), translates analyte binding events into measurable changes in the levitation height of the bead. This change in levitation height (the signal of the assay) depends on the concentration of analyte that was present in the sample.
To understand the processes that lead to the changes in density, we examined a model system comprising of gold-labeled streptavidin (as analyte) and polystyrene beads with biotin on their surfaces. A minimal mathematical model, based on the diffusion-limited growth of independent hemispherical nuclei (i.e. the gold nanoparticles) on a surface, adequately described the kinetics of the change in density. Measurements of the number of adsorbed gold-labeled streptavidin molecules on the surfaces of the beads using inductively-coupled plasma mass spectrometry (ICP-MS) confirmed matched the predictions of the minimal model. The addition of free gold nanoparticles in solution modified the kinetics of deposition of gold on the beads, and suggests a design for these assays in which the results would be independent of the time of development.
We use the description Density-Linked Immunosorbent Assay, or DeLISA, when those assays are performed with antigen and antibodies. As proof-of-concept experiments, we chose two different immunoassay formats – a competitive immunoassay to quantify the concentration of neomycin (an aminoglycoside antibiotic) in whole milk, and a multiplexed indirect immunoassay (including a positive and negative control) to detect antibodies against Hepatitis C virus NS3 protein and syphilis T. pallidum p47 protein in serum.
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In this equation, ρbead (kg m−3) and ρbuffer (kg m−3) are the densities of the bead and the buffer, χbead (χbead ~ −1 × 10−5 for diamagnetic objects) and χbuffer (χbuffer ~ 1.8 × 10−4 for 1.00 M MnCl2 (ref. 24)) are the magnetic susceptibilities (dimensionless) of the bead and the buffer, d (m) is the separation between the magnets, Bo (T) is the magnitude of the magnetic field at the surface of the magnets, μ0 = 4π × 10−2 (N A−2) is the magnetic permeability of free space, and g (m s−2) is the acceleration due to gravity.
We have used MagLev to measure the binding and release of bovine carbonic anhydrase (BCA) to (aryl)sulfonamide ligands on porous beads.30,35 In one version of these assays, BCA diffuses into the beads and binds to the immobilized ligands. The accumulation of protein in the beads due to this process results in a change in their density and levitation height. Although the use of gel-immobilized ligands in MagLev provides a label-free method to detect the concentration of protein in solution, the method worked best with small (<60 kDa) proteins having high diffusion constants in the pores of the beads, and required relatively long reaction times (hours to days). These limitations made the method, without modification, unsuitable for most applications of immunoassay. In this paper, we use a chemical reaction on the surface of non-porous beads to measure the concentration of proteins in solution. As we describe in the next section, the general principles of DeLISA use some procedures developed for existing immunoassays,21 and thus allow the adoption of established protocols and reagents.
After the primary and secondary incubation steps, the beads are then loaded into a capillary containing an aqueous solution of a paramagnetic salt (MnSO4) dissolved in a commercial gold amplification solution (the developing buffer). The gold amplification solution, which contains gold ions, a reducing agent, and various proprietary stabilizers, causes gold ions in solution to be reduced to elemental gold on the surface of the gold nanoparticles.39 Gold and silver amplification solutions are used, conventionally, to increase the size, and hence the scattering cross-section, of gold nanoparticle labels in tissue slices for optical and electron microscopy,39–41 and to conduct assays with optical readouts.42–44 We reasoned that the deposition of elemental gold onto the surface of a polymeric bead would also increase the density of the bead.
The rate at which gold is deposited on the bead (and hence the change in density and levitation height of the bead) depends on the number of bound gold nanoparticles on the surface of the bead, and the kinetics of the electroless deposition. This dependence allows a density-based assay for the quantitation of a target analyte in the sample.
Fig. 2A shows time-lapse photographs of a single bead in the developing buffer in the MagLev device. The bead had previously been exposed to a buffer solution containing 3000 pM gold-labeled streptavidin (see Materials and methods for the detailed procedure). The bead, which was initially colorless, turned black, and then golden, and decreased in levitation height before reaching the bottom of the capillary after 21 minutes. The change in levitation height of the bead corresponded to an increase in the density of the bead from 1.050 g cm−3 to over 1.055 g cm−3. A bead previously exposed to a 30 pM solution of gold-labeled streptavidin also changed color and decreased in levitation height. The decrease in levitation height, however, was slower (Fig. 2B): at 21 minutes its levitation height was 27 mm and after one hour its levitation height was 7 mm, i.e. 3 mm above the bottom of the capillary.
The change in the color of the beads is characteristic of the growth of the nanoparticles on the surfaces of the beads. The appearance of the beads in reflection depends of the ratio of their scattering cross-section and their optical density in the visible spectrum. Despite their strong optical density in the visible spectrum, the initial 10 nm gold nanoparticles immobilized on the polymeric beads have a small scattering cross-section, and therefore have a small albedo, which makes them nearly undetectable with the naked eye (hence the beads appear colorless). As they grow in size, they maintain a high optical density in the visible and their cross-section increases which makes the beads appear darker and darker. After some time, a continuous film is formed that does not significantly absorb in the visible and the scattering of the gold-covered beads is reminiscent of that of bulk gold (i.e. the beads appear golden).
Scanning electron micrographs of the surface of a bead exposed to 3000 pM of gold-labeled streptavidin at 0, 30 and 60 minutes confirmed that the nanoparticles on the surfaces of the beads, which were not visible prior to amplification, increased in size and eventually coalesced to form a film (Fig. 2C). Both these observations confirm that the amount of gold that was deposited on the surface of the bead increased with time in the developing buffer.
Fig. 3A shows the evolution with time of the levitation height of the beads exposed to 3000 pM, 300 pM, 30 pM, and 3 pM of gold-labeled streptavidin. The rate of change of the levitation height of the beads depended on the concentration of the gold-labeled streptavidin in solution. This dependence is seen clearly in the dose-response plot in Fig. 3B which shows the levitation height of beads (averaged over seven replicates) plotted against the concentration of gold-labeled streptavidin in the samples, at 30 and 60 minutes.
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| Fig. 4 Model of a MADA. A) Schematic of the three growth regimes of the gold nanoparticles on the surface of the bead in the developing buffer. When t ≪ τ (regime 1), the nanoparticles are far apart and the mass of gold on the bead, m ∝ Nt3/2. When t ~ τ (regime 2) m can be obtained by integrating eqn (2) numerically. When t ≫ τ (regime 3) the gold has fused to form a continuous layer; m ∝ t1/2. B) Plot of the levitation height, h (Fig. 3A) versus rescaled time, x = t3/2. The black lines are linear fits to the data. C) Table showing the concentration of free gold-labeled streptavidin that the beads were exposed to ([y]), the coefficients of the linear fit, and the values of the coefficient of determination, R2. The fits are good, indicating that the MADA can be modeled in the regime where t ≪ τ. The two leftmost columns report the ratio of the slope relative to the slope for the 3000 pM line, and the ratio of the number of nanoparticles on the surface of the beads relative to the number of nanoparticles for beads exposed to 3000 pM of gold-labeled streptavidin. The values are in good agreement. | ||
Eqn (2) describes the rate of deposition of metal, dm/dt (kg s−1), on a flat (electrode) surface of area S (m2) due to the diffusion-limited growth of N surface-adsorbed hemispherical nuclei (nanoparticles) per unit area (number m−2) with an initial radius, r = 0 (m) at t = 0 (s).51–53
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In this equation, C1 is a constant that depends on experimental conditions and
is the ‘characteristic time’ of the process, D is the diffusion coefficient (m2 s−1), and k is a unitless numerical constant (see ESI† for full discussion and derivation). Integrating eqn (2) with respect to time gives the mass of gold deposited on the bead, i.e.
. This integral is readily solved numerically for all t.
Simplified analytical expressions of eqn (2), obtained by considering limiting cases, provide physical insight. We divided the process of the growth of the nanoparticles on the surface of the bead into three regimes. When t ≪ τ (regime 1), the nanoparticles are sufficiently far apart that they grow independently of each other (i.e. the nanoparticles do not know that they are surrounded by neighbors on the surface). When t ~ τ (regime 2) the nanoparticles have grown to a size that their growth rate is influenced by their neighbors, which are also consuming reactants. When t ≫ τ (regime 3) the nanoparticles have coalesced to form a continuous layer. In regime 1, eqn (2) simplifies to
and m(t) ∝ t3/2. In regime 3, eqn (2) simplifies to
and m(t) ∝ t1/2. There is no closed-form expression for m(t) in regime 2. Note that the transition from regime 1 to the other regimes is controlled by the characteristic time, τ. Since τ ∝ 1/N, a higher density of adsorbed nanoparticles on the surface results in an earlier transition from regime 1 to the other regimes.
Substituting the expression for m(t) in regime 1 into eqn (1) and collecting the constants leads to a (relatively) simple expression for the change in levitation height of the bead as function of time
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In eqn (3),
is the surface-to-volume ratio of the bead, M is the molar mass (kg mol−1) of the metal and c (mol m−3) is the concentration of reactants. Inspecting eqn (3) the levitation height, h is linearly related to the surface-to-volume ratio, everything else being equal, the use of beads with higher surface-to-volume ratio should lead to a change in levitation height in the developing buffer that is greater than when beads with a lower surface to volume ratio are employed.
Fig. 4B shows the levitation height of the beads plotted versus the rescaled time, t3/2. The continuous black lines are linear regressions to the rescaled data. Fig. 4C shows a table with the equations for the linear regression and the coefficient of determination, R2. The linear fits are generally good, with the exception of the beads that were exposed to 3000 pM solution of gold-labeled streptavidin. We presume that N was sufficiently high in this case that the system transitioned to regime 2 or 3 during the course of the experiment.
Since the experiments were carried out under similar conditions, the ratio of the slopes of the lines should correspond to the ratio of the number of nanoparticles, N, that were adsorbed on the surface of the beads (eqn (3)). We used ICP-MS to measure quantitatively the amount of metallic gold on the beads (Fig. S1†). ICP-MS is sufficiently sensitive to detect the presence of gold on the beads due to the binding of gold-labeled proteins57,58 prior to amplification. This exquisite sensitivity allowed us to obtain the binding isotherm of gold-labeled streptavidin to the biotin-labeled beads (i.e. N vs. [free gold-labeled streptavidin]). Fig. S2† shows the equilibrium binding of gold-labeled streptavidin to the surface of the biotin-labeled beads versus the concentration of free gold-labeled streptavidin. Each datum is an average of seven beads. We assumed that due to sterics, there is one available streptavidin molecule per gold nanoparticle, we obtain a dissociation constant, Kd = 1.3 × 10−10 M−1 (we can also use the average number of streptavidin molecules on the gold nanoparticles specified by the manufacturer ~6.5. In that case, we find Kd = 8.0 × 10−10 M−1). This value compares favorably with measurements of the surface binding of biotin to streptavidin modified surfaces48,49 in other systems. The ratio of the number of gold nanoparticles adsorbed on the surfaces of the beads obtained through ICP-MS, N/N3000 pM agrees with the ratio of the slopes from the linear regression, m/m3000 pM (Fig. 4C).
We hypothesized that AuMADA might be made less dependent on time by adding free gold nanoparticles in the developing buffer. These free nanoparticles would compete for gold ions in the solution, and serve as sinks for unreduced metal ions. Once all the gold ions are depleted from the developing buffer, the levitation height of the beads should stop changing. Fig. 5A and B shows the evolution of the levitation height of beads that had been previously exposed to 3000 pM of gold-labeled streptavidin (similar to the bead in Fig. 2A). The developing buffer in Fig. 5A was doped to a final concentration of 1 × 1010 gold nanoparticles mL−1 and the buffer in Fig. 5B was doped to 2 × 1010 20 nm diameter gold nanoparticles mL−1. As expected, with larger concentrations of free nanoparticles in solution, the change in levitation height slowed after a shorter time (Fig. 5B). The levitation height of the bead, however, does not stop changing completely, at least within the timescale of a 2 hour experiment. We attribute these observations to residual low concentrations of reactants that continue the deposition process on the surfaces of the beads. For example, free gold nanoparticles that increase in size sufficiently that they sediment to the bottom of the capillary (black arrow in Fig. 5A) effectively stop acting as sinks. Further optimization of the procedure demonstrated here, which would require a study of the interaction between free and surface-bound gold nanoparticle catalysts and the concentrations of various reactants on the kinetics of electroless deposition, could eventually lead to the development of time-independent assays. Such a study is beyond the scope of this work.
The first assay was a quantitative competitive assay for the concentration of the small molecule antibiotic neomycin (an aminoglycoside) in milk (Fig. 6A). In this assay, the antigen was neomycin, the primary antibody was a monoclonal mouse anti-neomycin immunoglobulin G (IgG), and the secondary antibody was a polyclonal goat anti-mouse-IgG conjugated to 10 nm diameter gold nanoparticles. In a competitive immunoassay for neomycin, a fixed concentration of mouse anti-neomycin IgG was added to the samples of milk before the addition of polystyrene beads with neomycin on their surfaces. Free neomycin, if present in the milk, binds to the anti-neomycin IgG, and thus reduces the amount of anti-neomycin antibody available for binding to the neomycin on the surfaces of the beads. The higher the concentration of free neomycin in the sample of milk, the less anti-neomycin IgG is available to bind to the neomycin on the beads. Hence, the strength of the signal that is generated from the bound molecules on the beads correlates inversely with the concentration of free neomycin in the sample of milk, that is a sample with no neomycin will generate the strongest signal, and samples with higher concentrations of neomycin will generate weaker signals.
The second assay was a multiplexed indirect immunoassay for antibodies against syphilis and Hepatitis C (HepC) in serum (Fig. 6B). The antigens were Treponema pallidum p47 protein on polystyrene beads (which were colored blue), and Hepatitis C virus NS3 protein on polystyrene beads (which were colored pink). These experiments include two controls: bovine serum albumin (BSA) on polystyrene beads (which were colored red) as a negative control, and human IgG on polystyrene beads (which were colored yellow) as a positive control. The primary antibodies were the targeted analytes assayed in the human serum. In a sample of serum, they consist of polyclonal antibodies with a range of avidities and affinities.21 The secondary antibody was polyclonal goat anti-human IgG (γ-chain specific) conjugated to 10 nm gold nanoparticles. The presence of the primary antibody is – in the absence of non-specific adsorption – required for binding of the gold-labeled secondary antibody to the beads. Thus, in this assay, the signal (i.e. the electroless deposition of gold and the change in levitation height) correlates positively with the concentration of primary antibody in a sample of serum.
Fig. 7A shows a photograph of seven beads that were exposed to a sample of milk containing no neomycin (left), and a sample of milk spiked with 500 ppb of neomycin (right), after 30 minutes in the developing buffer. Fig. 6A shows the steps of the assay; the details are in the materials and methods section. To reduce the amount of reagents consumed, and to allow parallelization, we loaded the beads into cylindrical capillaries with an inner diameter of 1 mm. Since we performed a competitive assay, we expected an inverse relationship between the levitation height and concentration of free antibiotic in the milk. Indeed, beads that were exposed to the antibiotic-free milk had a levitation height of 27 mm, while the beads exposed to the sample with 500 ppb of neomycin levitated at 35 mm (that is, they did not change levitation height). Fig. 7B shows a plot of the levitation height of beads exposed to a range of neomycin concentrations. At 30 minutes, milk samples with residues above the MRL can be distinguished from samples with residues below the MRL. The sample of milk that was at the MRL could not be distinguished from those that were above the MRL. After a further 30 minutes in the levitation buffer (i.e. after a total time of 60 minutes), the beads decreased in levitation height further (Fig. 7C) and the sample of milk that was at the MRL could be distinguished from the samples with antibiotic residues above the limit (Fig. 7D).
Fig. 8 shows photographs of a set of the red, pink, blue, and yellow beads exposed to two simulated diseased serum samples and one simulated normal serum sample. The steps for carrying out the assays are shown schematically in Fig. 6B and provided in detail in the materials and methods section. Sample 1, the normal sample, was negative for HepC and syphilis. Sample 2 was positive for HepC and sample 3 was positive for both HepC and syphilis. Fig. 8A shows the configuration of the beads at the start of the developing period. Each of the colored beads levitated at approximately the same height in the capillaries. Fig. 8B–D shows beads after 30 minutes in the developing buffer. We observed that for the set of beads that were exposed to sample 1, only the yellow bead (human IgG, positive control) decreased in levitation height (Fig. 8B). For the beads exposed to sample 2, the pink (HCV NS3) and yellow bead (human IgG) decreased in levitation height (Fig. 8C). For beads exposed to sample 3, the pink (HCV NS3), blue (T. pallidum p47) and yellow (human IgG) beads changed levitation height (Fig. 8D). As expected, the red beads (BSA) which served as negative controls did not change levitation height for all the assays. Thus, the beads only changed levitation height when their cognate antibody was present in the serum sample. The positive and negative controls assured that the assay conditions were appropriate and served as an additional check that the deposition of gold and the change in levitation height were specific to the presence of the disease antibodies in the samples.
DeLISA, like other bead-based assays, has three advantages over typical plate-based assays. i) It requires a small volume of reagents and sample. ii) The high ratio of surface area to volume allows short (<1 h) incubation times. iii) Multiplexing can be carried out by using distinguishable (for example, differently colored) beads. DeLISA at its present level of development also has several limitations. i) The assay still requires multiple steps, including washing steps, to obtain a result. ii) The gold amplification reagents and processes might be sensitive to large variations in temperature or to other factors (such as decomposition at tropical temperatures, T ≥ 35 °C). We have not characterized these sensitivities. Use of antibodies with higher avidity and specificity, and incorporation of centrifugation16 or other automation14,15 may circumvent some of these limitations.
:
1 toluene
:
ethanol. After ten minutes, the dye solutions were passed through cotton filters to remove any remaining particulates. Approximately 300 mg of polystyrene beads were then added to the dye solution and gently rocked for one hour. The beads were then thoroughly rinsed with ethanol and dried in vacuo for at least four hours (typically overnight).
We then proceeded with grafting the proteins of interest (a BSA–biotin conjugate for the MADA for gold-labeled streptavidin, a BSA–neomycin conjugate for the quantitative detection of neomycin in milk, and the proteins Treponema pallidum p47, Hepatitis C NS3, BSA, and human IgG for the multiplex immunoassays) following the procedure from the technical note from Bangs Labs.63 Briefly, we washed the beads twice with 10 mL of 200 mM 2-(N-morpholino)ethanesulfonic acid (MES) buffer at pH 6.0, and resuspended them in 10 mL of the same. We added 1-cyclohexyl-3-(2-morpholinoethyl) carbodiimide metho-p-toluenesulfonate (100 mg) while mixing and allowed the mixture to react at room temperature for 15 minutes with continuous mixing. We then washed the beads with a 50 mM borate buffer at pH 8.3 (2 × 10 mL) and resuspended them in 10 mL of the same. We added an aqueous solution of the proteins of interest (200 μL of the stock solutions containing 1 mg mL−1 of protein) to this suspension, and incubated it at room temperature for 4 hours with constant mixing. We then washed the beads with phosphate-buffered saline (PBS) and allowed the beads to react with a solution containing 0.05 w/V% of BSA (to reduce non-specific adsorption of protein onto the surface of the beads) in 10 mL of a 40 mM aqueous solution of hydroxylamine (to react with the remaining activated carboxylic acids on the beads) at room temperature with continuous mixing for 30 minutes. Finally, we washed the protein-functionalized beads with PBS (3 × 10 mL) and stored the functionalized beads in PBS containing 0.05 w/V% of BSA.
000 ppb. We then diluted this stock solution with milk to 1000 ppb, and serially diluted the 1000 ppb solution to obtain a range of neomycin concentrations from 250 ppb to 1000 ppb. The MRL of neomycin is 500 ppb, and samples with concentrations far from this value are not relevant practically. We performed the competitive assay by following the manufacturer's (Silver Lake Research) protocol with minor modifications. Briefly, we diluted the monoclonal murine anti-neomycin antibodies 1
:
1500 times in PBS from the stock obtained from the manufacturer. We added 25 μL of the milk sample and 25 μL of the diluted antibody to an Eppendorf tube. We added seven beads functionalized with a BSA–neomycin conjugate to the Eppendorf tube and incubated for 30 minutes at room temperature. We removed the milk sample from the Eppendorf, added 100 μL of PBS and agitated the beads gently for less than 1 min before removing the buffer with a pipette. We then added 50 μL of 10 nm gold-labeled goat anti-mouse-IgG that was diluted 1
:
100 times in PBS as recommended by the manufacturer. We incubated the mixture for 30 minutes at room temperature. We removed the gold-labeled antibody, and washed the beads briefly by adding 100 μL of deionized water, and immediately transferred the beads (with a minimal amount of liquid) into an Eppendorf with developing buffer. We loaded the beads into capillaries through capillary action and placed them in the MagLev device.
:
3
:
2 ratio. Seven beads exposed to samples of differing concentrations of gold-labeled streptavidin were placed in 0.87 mL of freshly prepared dilute aqua regia for 20 minutes. To each sample, we added 50 μL of a 1000 ppb solution of bismuth (prepared by a dilution of a 1000 ppm ICP grade standard, which was prepared by dissolving high purity bismuth metal in 5% nitric acid) in MilliQ water to serve as an internal standard. We diluted our samples to a total volume of 5 mL with MilliQ water before analyzing the samples with ICP-MS. To obtain a calibration curve we also conducted ICP-MS measurements on serially diluted gold standards (ICP grade) from (0.01–10
000 ppb).
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c4lc01161a |
| This journal is © The Royal Society of Chemistry 2015 |