Gong Cheng1, Ming-Da Zhou, Si-Yang Zheng. 1. Department of Biomedical Engineering, The Pennsylvania State University , University Park, Pennsylvania 16802, United States.
Abstract
Mesoporous and hollow carbon microspheres embedded with magnetic nanoparticles (denoted as MHM) were prepared via a facile self-sacrificial method for rapid capture of low-abundant peptides from complex biological samples. The morphology, structure, surface property, and magnetism were well-characterized. The hollow magnetic carbon microspheres have a saturation magnetization value of 130.2 emu g(-1) at room temperature and a Brunauer-Emmett-Teller specific surface area of 48.8 m(2) g(-1) with an average pore size of 9.2 nm for the mesoporous carbon shell. The effectiveness of these MHM affinity microspheres for capture of low-concentration peptides was evaluated by standard peptides, complex protein digests, and real biological samples. These multifunctional hollow carbon microspheres can realize rapid capture and convenient separation of low-concentration peptides. They were validated to have better performance than magnetic mesoporous silica and commercial peptide-enrichment products. In addition, they can be easily recycled and present excellent reusability. Therefore, it is expected that this work may provide a promising tool for high-throughput discovery of peptide biomarkers from biological samples for disease diagnosis and other biomedical applications.
Mesoporous and hollow carbon microspheres embedded with magnetic nanoparticles (denoted as MHM) were prepared via a facile self-sacrificial method for rapid capture of low-abundant peptides from complex biological samples. The morphology, structure, surface property, and magnetism were well-characterized. The hollow magneticcarbon microspheres have a saturation magnetization value of 130.2 emu g(-1) at room temperature and a Brunauer-Emmett-Teller specific surface area of 48.8 m(2) g(-1) with an average pore size of 9.2 nm for the mesoporous carbon shell. The effectiveness of these MHM affinity microspheres for capture of low-concentration peptides was evaluated by standard peptides, complex protein digests, and real biological samples. These multifunctional hollow carbon microspheres can realize rapid capture and convenient separation of low-concentration peptides. They were validated to have better performance than magnetic mesoporous silica and commercial peptide-enrichment products. In addition, they can be easily recycled and present excellent reusability. Therefore, it is expected that this work may provide a promising tool for high-throughput discovery of peptide biomarkers from biological samples for disease diagnosis and other biomedical applications.
In the past decade, carbon nanomaterials
(e.g., carbon spheres, graphene, carbon nanotubes, etc.) have drawn
intensive interest due to their remarkable chemical and physical properties
such as chemical inertness, structural regularity, mechanical stability,
electrical conductivity, and biocompability.[1−3] Carbon materials
with porous structures and hetero components can provide enhanced
properties and multifunctional capabilities by combining the merits
of large surface area and the synergistic effects between multiple
discrete components, thereby showing high potential in various fields
including functional object support, biofuel cell and energy storage,
and fluorescent or electronic biosensors, etc.[4−7] Recently, carbon nanomaterials
with porous structure and multifunctional components have also been
designed and constructed for biomedical applications. For example,
biomolecule-functionalized carbon nanotubes, mesoporous carbon nanovectors,
and carbon–silica hybrids were explored for targeted delivery
of water-insoluble anticancer drugs,[8,9] in virtue of
the unique hydrophobic interactions and the supramolecular π
stacking between drug molecules and the carbonaceous structures. In
addition, by taking advantage of their multifunctional capabilities,
graphene and mesoporous carboncomposites attached by nanostructures
or modified by functional molecules were widely investigated as electrode
materials, enzyme mimics, and platforms for the detection of biological
targets in medical diagnosis.[10−12] Despite these burgeoning achievements,
facile preparation of composite and multifunctional carbon nanostructures
remains a great challenge, and it is highly desirable to further develop
and adequately utilize their unique nanostructure and remarkable physiochemical
properties in extending their use in demanding biomedical applications.With the advent of the postgenomic era, proteomics has been developing
for disease diagnosis and treatment, because it can provide a global
perspective on protein expression changes for detailed descriptions
of the structure, function, and control of biological systems.[13,14] It is well-documented that some bioactive peptides play a pivotal
role in a broad range of physiological conditions (e.g., pain sensation,
blood pressure, and energy homeostasis),[15,16] and some endogenous peptides in body fluids or tissues could be
biomarkers with higher clinical sensitivity and specificity.[17,18] With the development of modern analytical technologies, mass spectrometry
(MS) has become a powerful tool for the inspection of peptide biomarkers,
as it can provide direct and intrinsic information on the peptides
and screen multiple peptides simultaneously.[19,20] However, direct analysis of peptides extracted from biological samples
by MS is a great challenge, owing to the low concentrations of the
target peptides, strong interference, and suppression of high-abundance
biomolecules as well as other impurities (e.g., salts and surfactants).
A number of nanostructures for the capture and purification of low-concentration
peptides, such as silanized silica microspheres, polymer reverse micelles,
metal–organic frameworks, and hybrid materials,[21−25] have been explored to capture and purify the low-concentration peptides
from biosamples. Although these materials have shown interesting performance,
they are compromised by their complex fabrication strategies, limited
affinity sites, poor stability, and poor recyclability.Mesoporous
carbon nanostructures have a high potential to enrich low-concentration
peptides due to their chemical stability, high surface area, unique
hydrophobic interactions and similar pore size to peptides.[26] On the other hand, further optimization of the
materials’ structures and integration with other functional
composites would provide new opportunities to improve the capture
efficiency and facilitate the separation process. Recently, functionalized
magnetic nanostructures have become extremely favorable materials
for the convenient and fast transport and separation of the targets,
owing to their chemical durability, unique magnetic response, high
separation efficiency, and convenient operation.[27−32] Therefore, the design and synthesis of magnetic affinity material
combining the merits of its magnetic property and the special affinity
of mesoporous carbon is of particular interest in proteomic applications
requiring fast and convenient enrichment of low-abundance peptides.
Hard and soft template-based synthetic methods are always used to
prepare the mesoporous or hollow carbon nanostructures first and then
load the precursors of magnetic materials to further produce embedded
magnetic nanoparticles.[3,33] Nonetheless, it is well-known
that complicated, high-cost, and time-consuming multistep procedures
are required to prepare mesoporous or hollow carbon nanostructures
via template-based methods, not to mention the additional step to
introduce the magnetic nanoparticles into mesoporous carbon nanostructures.
As an alternative, herein we designed and constructed a novel magnetic,
hollow, and mesoporous carbon nanostructure (denoted as MHM microspheres)
via a facile method combining biomimetic formation of a polymer shell,
carbonization of an organic shell, and sacrifice of an inorganiccore,
and we also demonstrated that the MHM microspheres are effective affinity
materials for rapid enrichment and separation of low-concentration
peptides.
Experimental Section
Materials
Ferricchloride (FeCl3·6H2O), ethylene glycol
(EG), trisodium citrate (H3Cit), tris(hydroxymethyl)aminomethane
hydrochloride (Tris-HCl), ethanol (EtOH), sodium acetate (NaAc), ammonium
bicarbonate (NH4HCO3), acetonitrile (ACN), trifluoroacetic
acid (TFA), hexadecyltrimethylammonium bromide (CTAB), and ammonium
hydroxide (NH3·H2O) were obtained from
Alfa Aesar. Dopamine hydrochloride (DA), tetraethyl orthosilicate
(TEOS), 2,5-dihydroxybenzoic acid (2,5-DHB), angiotensin II, myoglobin
from equine heart (MYO), cytochrome C (Cty-C), bovineserum albumin
(BSA), and trypsin (from bovine pancreas, l-1-tosylamide-2-phenylethyl
chloromethyl ketone-treated) were purchased from Sigma-Aldrich (St.
Louis, MO, USA). All the chemical agents were used without further
purification. Human urine samples were collected from a healthy volunteer.
All procedures involving samples obtained from human subjects were
approved by the Institutional Review Board (IRB) of The Penn State
University.
Preparation of Fe3O4 and Fe3O4@PDA Microspheres
The magneticFe3O4 particles were prepared according to a
reported solvothermal approach with minor modification.[34] Typically, FeCl3·6H2O (0.81 g) and trisodium citrate (0.20 g) were first dissolved in
ethylene glycol (20 mL). Then, NaAc (1.20 g) was added, and the mixture
was vigorously stirred to form a transparent solution. Afterward,
the solution was transferred to a 50 mL Teflon-lined stainless-steel
autoclave. The autoclave was sealed and heated at 200 °C and
maintained for 8 h, and then it was allowed to cool to room temperature.
The products were washed with ethanol and deionized water several
times and dried at 60 °C for 12 h.For preparation of Fe3O4@PDA (PDA = polydopamine) core–shell microspheres,
the as-synthesized Fe3O4 particles (25 mg) were
fully dispersed in 25 mL of 20 mM tris-HCl (pH = 8.0) by ultrasonication
for 30 min. DA (50 mg) was dissolved in 25 mL of deionized water.
The dopamine solution was quickly injected into the Fe3O4 dispersion under continuous magnetic stirring at room
temperature for 8 h. After that, the products were collected, separated
by sorting using a magnet, and then washed several times with deionized
water. For preparation of pure PDA microspheres, 20 mg of DA dissolved
into 10 mL of 20 mM tris-HCl (pH = 8.0), the mixture were stirred
for 12 h at room temperature. After that, the PDA microspheres were
collected by centrifugation at 8000 rpm. The precipitates were washed
with water and ethanol several times and then dried at 60 °C
for 12 h.
Preparation of MHM Microspheres
MHM microspheres were
obtained by carbonizing the Fe3O4@PDAcore–shell
microspheres at 700 °C for 1 h in Ar at a rate of 5 °C min–1. For comparison, Fe3O4@PDAcore–shell microspheres were also calcined at 550 °C for
1 h in Ar at a rate of 5 °C min–1, and the
products are denoted as Fe3O4@C. The pure PDA
microspheres were also carbonized at 700 °C for 1 h in Ar at
a rate of 5 °C min–1 to obtain the pure carbon
microspheres. For comparison, magnetic mesoporous silica particles
were also prepared according to the previous report with slight modification.[35] Typically, 50 mg of the as-prepared Fe3O4 particles was fully dispersed in a solution containing 0.5 g of
CTAB and 200 mL of deionized water. Then, 5 mL of NaOH solution (0.1
M) and 195 mL of deionized water were added to the solution, after
which it was mechanically stirred for 30 min at 60 °C. Next,
2.5 mL of a TEOS/ethanol solution (v/v = 1/4) were injected into the homogeneous
solution, with intense agitation applied. The mixture obtained was
heated at 60 °C for 12 h. The resulting particles were separated
using the magnet and then washed with deionized water and ethanol.
Finally, the CTAB template was removed by a solvent extraction method
by using NH4NO3/ethanol solution (6 g L–1) refluxed at 60 °C for 10 h. This extraction
process was repeated twice. The products were denoted as Fe3O4@mSiO2.
Materials Characterization
Scanning electron microscopy (SEM) images were performed on a field
emission scanning electron microscope (FESEM; NanoSEM 630, NOVA) equipped
with an energy-dispersive X-ray analysis system (EDXA). Transmission
electron microscopy (TEM) and high-resolution TEM (HRTEM) images were
taken with a JEOL-2010 microscope at the accelerating voltage of 200
kV. Powder X-ray diffraction (XRD) patterns were collected on a PANalytical
Empyrean X-ray powder diffractometer (Cu Kα radiation, 45 kV,
40 mA) with the detection range from 5 to 80 degree. Raman spectra
were recorded on a WITecConfocal Raman instrument with a 514 nm laser
wavelength. Zetal potential of the particles were examined using a
Malvern Zetasizer ZS. Fourier transform infrared (FT-IR) spectra were
determined on a Bruker Vertex V70 FTIR spectrometer over a potassium
bromide pellet and then scanned from 400 to 4000 cm–1 at a resolution of 6 cm–1. Nitrogen adsorption
isotherms were measured at liquid nitrogen temperature (77 K) with
a Micromeritcs ASAP 2020 apparatus. The specific surface area was
determined by the Brunauer–Emmett–Teller (BET) method.
The total pore volume was evaluated by the t-plot method, and pore
size distribution was analyzed with the supplied BJH software package
from the adsorption branches of the isotherms. Magnetization measurement
was carried out with a superconducting quantum interface device (SQUID)
magnetometer at 300 K.
Preparation of Protein Digests
Proteins
(1 mg of Cyt-C or BSA) were dissolved in 1 mL of 50 mM NH4HCO3 solution, and then trypsin was added into the solution
with a molar ratio of 50:1 (protein/trypsin) at 37 °C for 16
h. Finally, the obtained tryptic digests were diluted to the target
concentrations and stored at −20 °C refrigerator before
use.
Low-Concentration Peptide Enrichment
A solution of
a standard peptide (angiotensin II) was first used to investigate
the possibility of the MHM affinity microspheres for enrichment of
trace peptides. 500 μL of angiotensin II solution (2.5 nM) was
mixed with 2.5 μL of 20 mg mL–1 well-dispersed
MHM microsphere suspension and then shaken for 5 min. Subsequently,
the particles trapped target peptides were collected and isolated
from the mixture using a permanent magnet. After that, the enriched
peptides were eluted with 5 μL of 0.5% TFA and 80% ACN solution,
and the supernatant was collected for MS detection after magnetic
separation.Protein digests were diluted to 2.5 nM before enrichment.
500 μL of protein digest was mixed with 2.5 μL of 20 mg
mL–1 well-dispersed MHM microsphere suspension and
then shaken for 5 min. Subsequently, the particles with captured target
peptides were collected and isolated from the mixture with the help
of a permanent magnet. After that, the enriched peptides were eluted
with 5 μL of 0.5% TFA and 80% ACN solution, and the supernatant
was collected for MS detection after magnetic separation. For comparison,
a commercial ZipTipC18 pipet tip and homemade Fe3O4@mSiO2 microspheres were also used to capture target peptides
from the above model samples. The sample preparation of peptides prior
to matrix-assisted laser desorption ionization time-of-flight mass
spectrometry (MALDI-TOF MS) using ZipTipC18 pipet tips was according
to the standard procedure provided by Millipore Corporation. The procedure
of peptide enrichment using Fe3O4@mSiO2 was similar to that of MHM microspheres.
Enrichment of Peptides
from Human Urine
Five microliters of 20 mg mL–1 well-dispersed MHM suspension was added into 1 mL of freshly collected
urine and then shaken for 15 min. After that, the microspheres with
captured targets were sorted by a magnet and washed with pure water
(200 μL). Then the MHM affinity microspheres with captured peptides
were eluted with 5 μL of 0.5% TFA and 80% ACN solution. After
magnetic separation, the supernatant was collected for MS detection.
MALDI-TOF MS Analysis
One microliter of sample solution
was mixed with 1 μL of matrix solution containing 20 mg/mL DHB
(in 50% acetonitrile aqueous solution, v/v) and 1% H3PO4 aqueous solution (v/v) by pipetting, and 0.5 μL of
mixture was deposited onto the MALDI target. MALDI-TOF MS analysis
was performed on an AB SCIEX MALDI-TOF/TOF 5800 mass spectrometer
(Foster City, CA, USA) in positive ion mode with 355 nm Nd:YAG laser,
200 Hz repetition rate, and 20 kV acceleration voltage. Fragment ion
spectra were submitted to MASCOT (http://www.matrixscience.com/) for database search and identification of corresponding peptides
using the following search parameters: Date base: SwissProt; Enzyme:
Trypsin; Number of missed cleavages allowed: 1; Taxonomy: Mammals;
Peptide tolerance: 0.5.
Results and Discussion
Synthesis and Characterization
of MHM Microspheres
Scheme 1a illustrates
the synthesis strategy of the MHM microspheres. First, well-dispersed
Fe3O4 microspheres prepared by a solvothermal
method were used as the sacrificial template and the magnetic precursor.
Then, a biomimetic adhesive method was used to coat the magneticcore
with a highly uniform polymeric shell by self-assembly of dopamine
(DA) molecules on the surface of Fe3O4 in alkaline
aqueous solution, leading to formation of the PDA shell as the carbon
resource. After thermal treatment of the magnetic PDA microspheres
(denoted as Fe3O4@PDA) at high temperature under
the argon atmosphere, the magnetic, hollow and mesoporous carbon microspheres
were prepared.
Scheme 1
Schematic Illustration of the (a) Synthesis Strategy
for MHM Microspheres and (b) Rapid Capture and Magnetic Separation
of Peptides for MS Analysis
In the Supporting Information, Figure S1a,b shows the scanning electron microscopy (SEM) images
of the prepared Fe3O4 microspheres with different
magnification. The Fe3O4 microspheres have the
relatively coarse surface and regular spherical shape with an average
size of 200 nm, and they consist of numerous aggregative small Fe3O4 nanoparticles. After encapsulation with PDA,
as shown in the Supporting Information,
Figure S1c,d, the surface of t he resulting microspheres becomes smoother
compared with the Fe3O4 microspheres, and the
size of the microspheres increased to around 280 nm. As revealed by
the TEM images, the obtained Fe3O4@PDA microspheres
possess a well-defined core–shell structure, and the thickness
of the PDA is ∼40 nm. As shown in Figure 1a,b, the MHM products still keep the sphere-like morphology after
high-temperature carbonization under inert gas protection. However,
the size of the MHM microspheres decreased slightly, and they present
a porous and rough surface, which could be ascribed to the pyrolysis
of PDA layer (Figure 1b). According to the
SEM image of broken MHM microspheres, a large cavity is apparent,
and the core particles have disappeared partially, indicating the
hollow and mesoporous structure of MHM microspheres (Figure 1c). The TEM images further authenticate the mesoporous
structure of the MHM microspheres and the disappearance of Fe3O4cores (Figure 1d). Note
that the hollow structure can only be observed indistinctly, due to
the low contrast of carbon material and the nonuniform surface of
the hollow shell.[36,37] Interestingly, many nanoparticles
with size of 10–30 nm were decorated on the shell of the MHM
microspheres. According to the HRTEM image (Figure 1e), the pore wall is composed of graphiticcarbon, because
of the presence of the curved lattice fringes of graphitic (002) layers
with an interplanar spacing of 0.35 nm. Furthermore, the lattice fringe
spacing of the nanoparticles that decorate the hollow shell can also
be clearly observed, and the lattice fringe spacing is ∼0.20
nm (Figure 1f), which agrees well with the
(110) crystal plane of iron (JCPDS Card No. 06–0696). These
results indicate that Fe nanoparticles were formed by conversion of
Fe3O4 phase during the thermal treatment, leading
to the fracturing and disappearance of magneticcores.
Figure 1
SEM images of MHM microspheres
with different magnification (a, b) and some broken MHM microspheres
(c); TEM image of a typical MHM microsphere (d), and the dotted circle
represents the obscure hollow structure; HRTEM images of the pore
(e) and nanoparticle (f) in the MHM microspheres.
SEM images of MHM microspheres
with different magnification (a, b) and some broken MHM microspheres
(c); TEM image of a typical MHM microsphere (d), and the dotted circle
represents the obscure hollow structure; HRTEM images of the pore
(e) and nanoparticle (f) in the MHM microspheres.The difference of elemental composition of prepared microspheres
corresponds to the phase transformation, as a cause of the dramaticchange in morphology, which was investigated by the energy-dispersive
X-ray (EDX) analysis. Figure 2 shows the EDX
spectra of the Fe3O4, Fe3O4@PDA, and MHM microspheres. Apparently, the Fe3O4 microspheres are mainly composed of the elements Fe and O. For the
Fe3O4@PDA microspheres, besides all the elements
observed in the Fe3O4 microspheres, the presence
of the new element N and the increase of the relative intensity for
element C demonstrate the successful addition of PDA shell. However,
after thermal treatment at high temperature, the element Fe possessed
the highest peak intensity, while the relative content of the elements
C, N, and O dramatically decreased. These results indicate that the
corresponding phase transformation has taken place during the thermal
process.
Figure 2
EDX spectra of the prepared Fe3O4, Fe3O4@PDA, and MHM microspheres.
EDX spectra of the prepared Fe3O4, Fe3O4@PDA, and MHM microspheres.Note that the temperature of the thermal treatment is critical
for the formation of mesoporous and hollow structure for the MHM microspheres.
As shown in the SEM image (Figure 3a), in contrast
to the MHM microspheres, the resulting products (denoted as Fe3O4@C) after thermal treatment at 550 °C under
inert gas protection still remain a relatively smooth surface when
compared to their precursor microspheres. Furthermore, the well-defined
core–shell structure can be obtained in the TEM images, the
Fe3O4cores still keep their original morphology,
and no porous structure is apparent on the carbon shell (Figure 3b). Compared to the EDX spectrum of MHM microspheres,
the abundance of element O in the EDX spectrum of Fe3O4@C (Figure 3c) also demonstrates that
the integrity of Fe3O4core is almost unaffected
during the thermal treatment. To investigate the role of Fe3O4core in formation of the mesoporous and hollow carbon
nanostructures, a control experiment of thermal treatment of pure
PDA microspheres without magneticcores at 700 °C was conducted.
Figure 3d shows the TEM image of the carbonized
microspheres. It is apparent that only dense carbon microspheres could
be obtained without incorporation of the magneticcores. These results
reveal that both the high temperature of the thermal treatment and
the Fe3O4cores play important roles in generation
of magnetic hollow and mesoporous carbon microspheres.
Figure 3
SEM image (a), TEM image
(b), and EDX spectrum (c) of Fe3O4@C and TEM
image of carbon microspheres (d).
SEM image (a), TEM image
(b), and EDX spectrum (c) of Fe3O4@C and TEM
image of carbon microspheres (d).To further demonstrate the phase transformation for formation
of magnetic mesoporous carbon microspheres, the microspheres were
characterized by powder X-ray diffraction (XRD). Figure 4a displays the powder XRD patterns of the Fe3O4, Fe3O4@PDA, and MHM products, and all
the products show well-defined diffraction peaks. The XRD patterns
of the Fe3O4can be assigned to the characteristic
diffraction peaks from magnetite (JCPDS Card No. 19–0629).
Similar XRD patterns can also be observed in the results of Fe3O4@PDA microspheres, further revealing that the
main magnetite phase of magneticcores was not destroyed during the
fabrication procedure. However, after thermal treatment at high temperature,
the characteristic diffraction peaks from magnetite disappeared, while
new strong diffraction peaks become present and could be assigned
to the iron phase (JCPDS Card No. 06–0696), which is consistent
with the previous TEM results.
Figure 4
XRD patterns (a) and Raman spectra (b)
of Fe3O4, Fe3O4@PDA, and
MHM microspheres.
XRD patterns (a) and Raman spectra (b)
of Fe3O4, Fe3O4@PDA, and
MHM microspheres.The nature of the composition
and interface changes of the samples was also investigated by Raman
spectroscopy, as shown in Figure 4b. The Raman
spectrum of bare magneticcores shows two strong bands around 489
and 681 cm–1, which correspond to the T2g and A1g
modes of symmetry, which indicate the presence of Fe3O4.[38,39] In comparison to the Fe3O4 microspheres, two new broad characteristic bands around 1355
and 1577 cm–1 are present in the Raman spectrum
of Fe3O4@PDA microspheres, which are attributed
to the deformation of the catechol group in the PDA shell.[40] After thermal treatment, the Raman spectrum
of the microspheres is greatly changed, due to the loss of PDA shell
and generation of new carbon species. In particular, the Raman spectrum
of MHM microspheres shows two typical peaks between 1200 and 1800
cm–1. The strong peak at around 1595 cm–1 could be assigned to G-bands of the characteristic ordered graphitic-like
carbon, while the other peak of D-band at around 1346 cm–1 could be ascribed to the presence of defects within the hexagonal
graphitic structure. Notably, the G-band shifted to higher wavenumbers,
compared with the spectra of pure graphitecrystals, because of the
presence of some structural imperfections of the carbon.[41] In addition, a weak characteristic peak can
also be observed around 2716 cm–1, which could be
attributed to the two-dimensional mode of graphitic-like carbon. The
above results demonstrate the formation of graphiticcarbon, which
agrees well with the TEM observation.Surface properties of
prepared microspheres were characterized using the zeta-potential
analysis (Figure 5a). The prepared Fe3O4 appears to show a positive zeta-potential value (7.59
± 0.34 mV). However, after coating of PDA shell, the microspheres
present a negative zeta potential of −34.73 ± 0.74 mV,
indicating formation of PDA layer on the Fe3O4. The negative zeta-potential value of the Fe3O4@PDA microspheres should be assigned to the deprotonation of the
phenolic group on the PDA shells.[42] After
carbonization, the zeta-potential value of MHM microspheres increased
to −17.70 ± 0.66 mV, implying the surface transformation
of the prepared microspheres. Furthermore, FT-IR spectra were also
recorded to analyze the surface property and manifest the transformation
of prepared microspheres. As shown in Figure 5b, the characteristic absorption peak at ∼590 cm–1 in Fe3O4 microspheres can be assigned to the
stretching vibration of Fe–O from the Fe3O4. After coating of PDA shell, besides the absorption band of Fe–O
bond, the presence of new absorption bands between 1800 and 1000 cm–1 evidence the successful modification of the magneticcore. The characteristic absorption peaks at 1622 and 1289 cm–1 can be attributed to the stretching vibration of
the aromatic rings and the C–O stretching of phenolcompounds,
respectively, while the enhanced absorption bands at 3374 and 3243
cm–1 can be assigned to the stretching vibration
of O–H and N–H.[43−45] After carbonization, most of
the characteristic peaks of the organic groups disappeared, and the
absorption bands of Fe–O stretching vibration dramatically
decreased. These results further demonstrate the carbonization of
PDA and the dramatic transformation of magneticcore under high temperature.
Figure 5
Zeta potentials
(a) and FTIR spectra (b) of Fe3O4, Fe3O4@PDA, and MHM microspheres.
Zeta potentials
(a) and FTIR spectra (b) of Fe3O4, Fe3O4@PDA, and MHM microspheres.The surface area and porous structure of the MHM microspheres
was characterized by N2-sorption measurement at 77 K. As
displayed in Figure 6a, the adsorption/desorption
isotherm of the MHM microspheres possesses type IV curve with a distinct
hysteresis loop at relatively high P/P0 according to the
IUPACclassification,[46] suggesting a mesoporous
structure. The average BET specific surface area, the average pore
diameter, and the total pore volume of MHM microspheres were calculated
to be 48.8 m2 g–1, 9.2 nm, and 0.11 cm3g–1, respectively. The pore-size distribution
derived from the adsorption curve in Figure 6a using the Barrett–Joyner–Halenda (BJH) method is
shown in the inset. As is apparent, besides a relatively narrow and
high peak in the mesoporous range around 2.0 nm, a broad band range
from 5 to 50 nm was also present in the MHM microspheres. The distribution
of multiple pore sizes agrees well with the previous TEM results,
which is possibly attributable to the cavity and interspace produced
by corrosion of Fe3O4cores and graphitization
of amorphous carboncatalyzed by reduced Fe metal during the high-temperature
thermal treatment.[47] Note that the unique
porous structure of the affinity microspheres would promote their
performance in the following application of enriching target biomolecules,
due to their high surface areas and pure affinity surface. More importantly,
because of their hollow structure, the affinity carbon shells of the
MHM affinity microspheres have numerous relatively large but shallow
open pores, which would facilitate the mass transport and diffusion
of target biomolecules. Therefore, the targets can not only be effectively
adsorbed into the affinity shell, but also be rapidly released and
diffused out of the shell in the elution step.[48−50]
Figure 6
N2 adsorption–desorption
isotherm and pore size distribution (inset) of the MHM microspheres
(a); room-temperature magnetization curves (b) of Fe3O4, Fe3O4@PDA, and MHM microspheres, and
inset shows an example of the magnetic response of MHM microspheres.
N2 adsorption–desorption
isotherm and pore size distribution (inset) of the MHM microspheres
(a); room-temperature magnetization curves (b) of Fe3O4, Fe3O4@PDA, and MHM microspheres, and
inset shows an example of the magnetic response of MHM microspheres.The magnetism of nanostructures
would contribute to the fast and convenient separation of nanostructures
via an external magnetic field, thereby being free of tedious and
time-consuming centrifugation in practical applications. As shown
in Figure 6b, the magnetic hysteresis curves
of the MHM microspheres were recorded at 300 K via a SQUID magnetometer.
The Fe3O4 and Fe3O4@PDA
microspheres show relative superparamagnetism with saturation magnetization
values of 66.6 and 35.7 emu g–1, respectively. Interestingly,
MHM have stronger magnetism than their precursor particles, with a
saturation magnetization value of 130.2 emu g–1,
which can be ascribed to the weight loss of nonmagnetic species because
of the reduction of the Fe3O4core to iron nanoparticles.
Figure 6b inset shows an example of drawing
the MHM microspheres by a magnet. As expected, in the presence of
the magnet, the well-dispersed MHM microspheres can be rapidly separated
from the mixture in less than 1 min. The above results demonstrate
that the MHM affinity microspheres have a good magnetic response that
would contribute to their facile and rapid separation in practical
applications.
Enrichment of Low-Concentration Peptides
Using MHM Microspheres
By taking advantage of their unique
nanostructure, distinct hydrophobicity, and rapid magnetic response,
the MHM microspheres can be applied to extract low-concentration peptides
from complex biological samples. Scheme 1b
displays the typical enrichment procedure. The MHM microspheres were
mixed in the sample solution for interaction with the peptides. Then,
the microspheres with captured peptide were easily isolated by a magnet.
After further purification and elution, the enriched peptides were
ready for MS analysis.To investigate the possibility of the
MHM affinity microspheres for enrichment of low-concentration peptides,
a solution of diluted standard peptides, angiotensin II (molecule
weight: 1046.2 Da, sequence: DRVYIHPF, concentration: 2.5 nM), was
used as a model sample. As displayed in Figure 7a, the target peptidescan be detected by MALDI-TOF MS; however,
the intensity and signal-to-noise ratio (S/N) are very low, due to
the extremely low concentration of target peptides. After treatment
using the MHM affinity microspheres via above-mentioned procedure,
the supernatant was also analyzed using MS. It is of particular interest
that no clear peptide signal can be detected in the supernatant (Figure 7b), revealing that the target peptides were captured
by the affinity microspheres. Figure 7c shows
the MS of the enriched peptides. As expected, the target peptides
were detected with strong intensity and high S/N. These results demonstrate that the MHM affinity microspheres
can effectively enrich low-concentration peptides.
Figure 7
MALDI-TOF mass spectra
of 2.5 nM angiotensin II solution: direct detection (a), the supernatant
(b), and the eluent (c) after enrichment using MHM affinity microspheres,
respectively. The number in the top right corner is the highest peak
intensity.
MALDI-TOF mass spectra
of 2.5 nM angiotensin II solution: direct detection (a), the supernatant
(b), and the eluent (c) after enrichment using MHM affinity microspheres,
respectively. The number in the top right corner is the highest peak
intensity.To further evaluate the effectiveness
of the MHM affinity microspheres for the capture of various peptides
from the low-concentration and complex peptide samples, protein digestions
of BSA and Cyt-c were used. Figure 8a displays
the MS of direct analysis of diluted BSA tryptic digest (2.5 nM).
Because of the extremely low concentration of the peptide mixture
and possible interference from salts, only three peptides from BSA
can be detected, and the intensity and S/Nare very low. Notably,
it is hard to identify the target protein in proteomics via peptide
mass fingerprint (PMF)-based online database search according to the
present MS of poor quality. However, after enrichment using the MHM
affinity microspheres, many peptides with high intensity and S/Ncan
be observed with a clean background (Figure 8b), indicating most of the peptides were enriched and purified. More
importantly, the BSA protein can be successfully identified based
on the high-quality MS, and 34 peptides with sequence coverage of
37% can be effectively matched (Supporting Information,
Table S1). This result is much better than that of the magnetic
mesoporous silicacounterpart in previous reports.[51] For further comparison, the commercial product (ZipTip
C18 pipet tip) and homemade mesoporous magneticsilica were also applied
to the same sample. As shown in Figure 8c,d,
although the ZipTip C18 pipet tip and mesoporous magneticsilicaare
effective to enrich peptides from the peptide mixtures, fewer target
peptidescan be detected, and the intensity is relatively low. Furthermore,
only 16 peptides with sequence coverage of 20% and 19 peptides with
sequence coverage of 22% can be identified via PMF-based online database
search for ZipTip C18 pipet tip and mesoporous magneticsilica, respectively
(Supporting Information, Table S1). A similar
phenomenon can also be observed in MS results collected from the enrichment
of low-concentration Cyt-C digests (Supporting
Information, Figure S2), indicating the universality of the
MHM affinity microspheres for efficient enrichment of low-concentration
peptides. Supporting Information, Tables S1 and
S2 list the detailed information on the identified peptides
from BSA and Cyt-c digests by MALDI-TOF MS analysis, respectively.
The above results clearly demonstrate the advantages of MHM affinity
microspheres for enrichment of low-concentration peptides from a complex
peptide mixture.
Figure 8
MALDI-TOF mass spectra of the diluted BSA digest (2.5
nM): direct detection (a) and after enrichment with the MHM affinity
microspheres (b), the magnetic mesoporous silica microspheres (c),
and the ZipTip C18 pipet tip (d), respectively. The number in the
top right corner is the highest peak intensity.
MALDI-TOF mass spectra of the diluted BSA digest (2.5
nM): direct detection (a) and after enrichment with the MHM affinity
microspheres (b), the magnetic mesoporous silica microspheres (c),
and the ZipTip C18 pipet tip (d), respectively. The number in the
top right corner is the highest peak intensity.Because of the high stability of their carbon shells and
the fast magnetic separation possible because of their magneticcores,
the affinity microspheres can be regenerated by washing with buffer
several times after use. Highly diluted BSA digests (2.5 nM) were
used to investigate the reusability of the affinity microspheres.
Figure 9a,b displays the typical mass spectra
of the low-concentration BSA digests after enrichment using the regenerated
affinity microspheres after three and five times, respectively. Notably,
many peptides with high intensity and clean background can be detected,
indicating the excellent performance of the reused affinity microspheres.
Furthermore, the same conclusion can also be drawn from the PMF-based
online database search. As shown in Figure 9c, the model protein can still be effectively identified with high
peptide matched number and sequence coverage, even after being reused
five times, verifying the excellent reusability of the MHM affinity
microspheres.
Figure 9
MALDI-TOF mass spectra of the diluted BSA digest after
enrichment with the recycled MHM affinity microspheres used three
(a) and five (b) times. The number of matched peptides and sequence
coverage of the diluted BSA digest after enrichment using the recycled
MHM affinity microspheres (c).
MALDI-TOF mass spectra of the diluted BSA digest after
enrichment with the recycled MHM affinity microspheres used three
(a) and five (b) times. The number of matched peptides and sequence
coverage of the diluted BSA digest after enrichment using the recycled
MHM affinity microspheres (c).Human urine is a common biological sample in clinical diagnostics,
and it contains various informative endogenous peptidescorrelating
well with the pathophysiology, which are potential biomarkers to diagnose
and monitor many diseases.[52,53] However, it is still
a great challenge to detect these peptides directly by MS, because
the urine contains a high saltconcentration and other solid residuals
that would severely interfere with MS analysis. Thus, it is imperative
to enrich the target peptides before MS analysis. Herein, human urine
was used to evaluate the effectiveness of the MHM affinity microspheres
for enrichment of peptides from the complex biological sample. Figure 10a presents the mass spectrum of direct analysis
of a urine sample, indicating no effective peptide peaks can be detected.
However, as shown in Figure 10b and Supporting Information, Table S3, after enrichment
and purification using the MHM affinity microspheres, many peptidescould be detected with strong intensity and clean background. These
results further prove the capability of the MHM affinity microspheres
for enrichment of target peptides from complex biological samples.
Figure 10
MALDI-TOF
mass spectra of human urine: direct detection (a) and after enrichment
(b) with the MHM affinity microspheres.
MALDI-TOF
mass spectra of human urine: direct detection (a) and after enrichment
(b) with the MHM affinity microspheres.
Conclusion
In summary, magnetic hollow and mesoporous
carbon microspheres were prepared via a facile method, and they have
been applied for the rapid enrichment and separation of low-concentration
peptides. The MHM affinity microspheres possess the unique nanostructure,
high surface area, magnetic properties as well as characteristic affinity,
thereby having high potential in rapid extraction and enrichment of
peptides from the complex biological samples. The effectiveness of
these MHM affinity microspheres has been evaluated with standard peptides,
complex protein digests, and real biological samples, and they show
better performance than the commercial product and conventional polypeptide
enrichment material mesoporous magneticsilica. In addition, MHM affinity
microspheres can be reused several times. Therefore, this work may
provide a promising tool for high-throughput discovery of biomarkers
from biological samples for disease diagnosis in biomedical applications.