Characterization techniques of nanoparticles

29,483 views

Published on

Advancement of characterization techniques of nanoparticles and sophisticated instruments

Published in: Technology, Business
9 Comments
44 Likes
Statistics
Notes
No Downloads
Views
Total views
29,483
On SlideShare
0
From Embeds
0
Number of Embeds
23
Actions
Shares
0
Downloads
3,583
Comments
9
Likes
44
Embeds 0
No embeds

No notes for slide

Characterization techniques of nanoparticles

  1. 1. Welcome 1
  2. 2. Advancements in Characterization Techniques of Nanoparticles Prithusayak Mondal Division of Agricultural Chemicals Chairperson : Dr. Anupama Singh Seminar Leader : Dr. Suman Gupta 2
  3. 3. Characterization refers to the study of material‟s features such as its composition, structure,& various properties like physical, electrical, magnetic etc. Nano = 10-9 (extremely small) Particle = Small piece of matter Nanoparticle is a microscopic particle whose size is measured in nanometers (nm). These particles can be spherical, tubular, or irregularly shaped and can exist in fused, aggregated or agglomerated forms. (PAS71: 2005,UK) 3
  4. 4. Size ranges of nanoparticles Nanoparticles are defined as particles that have at least one dimension in the nanorange (1 to 100nm). (Maurice & Hochella, 2008) 4
  5. 5. “To understand the very large, we must understand the very small.” - Democritus (400 BC) 5
  6. 6. Classification Nanoparticle Organic nanoparticle Inorganic nanoparticle 6
  7. 7. Novel Properties of nanoparticles • Small size • High surface area • Ease to suspend in liquids • Deep access to cells and organelles • Improved physical, chemical & biological properties  Properties of nanoparticles are different from their bulk counterparts.  Extremely high surface area to volume ratio results in surface dependent material properties. 7
  8. 8. Medical Agriculture Information technology Energy Uses Of Nanoparticles Ecology & environment Industry Defence & security Consumer goods 8
  9. 9. Enhanced catalytic properties of surfaces of nano ceramics or those of noble metals like platinum and gold are used in the destruction of toxins and other hazardous chemicals. (Salata, 2005) Synthesis and characterization of collagen/hydroxyapatite: magnetite nanocomposite material for bone cancer treatment. (Ecaterina et al., 2010) Antimicrobial effects of silver nanoparticles. (Kim et al.,2007) Removal of arsenic (III) from groundwater by using different concentration of nanoscale zero-valent iron (Kanel., 2005).
  10. 10. Targeted drug delivery
  11. 11. Silver nanoparticles inhibited the binding of the virus to the host cells in vitro (Elechiguerra et al., 2005). Cells and S layer protein nanoparticles of Bacillus sphaericus JG A12 have been found to have special capabilities for the clean up of uranium contaminated waste waters (Duran et al., 2007). Magnetosome particles isolated from magnetotactic bacteria have been used as a carrier for the immobilization of bioactive substances such as enzymes, DNA, RNA and antibodies (Mohanpuria et al., 2007). The gold nanoparticles synthesized from E. coli may be used for realizing the direct electrochemistry of haemoglobin (Du et al., 2007). Metal nanoparticle embedded paints have been synthesized using vegetable oils and have been found to have good antibacterial activity (Kumar et al., 2008). 11
  12. 12. Nanoparticles in agrochemicals Nano-encapsulated and solid lipid nanoparticles have been explored for the delivery of agrochemicals . (Frederiksen et al., 2003) The development of organic–inorganic nanohybrid material for controlled release of the herbicide 2,4-dichlorophenoxyacetate. (Bin Hussein et al., 2005) Porous hollow silica nanoparticles, developed for the controlled delivery of the water-soluble pesticide validamycin with a high loading capacity (36 wt%), have been shown to have a multistaged release pattern. (Liu et al., 2006) The development of a nano-emulsion (water/poly-oxyethylene) non-ionic surfactant (methyl decanoate) containing the pesticide betacypermethrin. (Wang et al., 2007) 12
  13. 13. Characterization Techniques 13
  14. 14. Optical(Imaging) Probe Characterization Techniques T Y P E S Electron Probe Characterization Techniques Scanning Probe Characterization Techniques Photon(Spectroscopic) Probe Characterization Techniques Ion-particle probe Characterization Techniques Thermodynamic Characterization Techniques 14
  15. 15. Optical(Imaging) Probe Characterization Techniques Acronym Technique Utility CLSM Confocal laser-scanning microscopy Imaging/ultrafine morphology SNOM Scanning near-field optical microscopy Rastered images 2PFM Two-photon fluorescence microscopy Fluorophores/biological systems DLS Dynamic light scattering Particle sizing BAM Brewster angle microscopy Gas-liquid interface Imaging 15
  16. 16. Dynamic light scattering 16
  17. 17. Basic principle Particles, emulsions & molecules in suspension undergo Brownian motion. If the particles are illuminated with laser, the intensity of scattered light fluctuates. Analysis of these intensity fluctuations yields the particle size(radius, rk) using Stokes- Einstein relationship, rk =kT/6πηD where k = Boltzmann‟s constant T = Temperature η = Viscosity D = Diffusion coefficient (Movie courtesy of Dr. Eric R. Weeks, Physics Department, Emory University.) 17
  18. 18. What does Dynamic Light Scattering measure? The diameter measured in DLS is called the hydrodynamic diameter and refers to how a particle diffuses within a fluid. The diameter obtained by this technique is that of a sphere that has the same diffusion coefficient as the particle being measured. The diffusion coefficient will depend not only on the size of the particle “core”, but also on any surface structure, as well as the concentration and type of ions in the medium. 18
  19. 19. Instrumentation Optical system Detector system DLS Light source Digital correlator 19
  20. 20. Light source Practical requirements for a sufficiently intense light source demand a narrow-band, polarized, monochromatic, CW laser. Type Wavelength Power Size HeNe 632.8 nm 5-35 mW 0.40- 1.5m Laser diodes 635-780 nm 5-100mV 0.05-0.15 m Ar+(air cooled) 488-514.5 nm ~100mW 1m Ar+(water cooled) 488-514.5 nm ~1.7W 1.5-2m DPSS (Frequ. Doubled) 10mV-4W 0.2 -0.5m 532 nm 20
  21. 21. Optical system A lens focuses the laser beam down into the sample which is enclosed in a temperature-controlled scattering cell surrounded by a refractive index matching liquid. The scattered light is focused onto a PMT at an angle 60 by another lens. Systems like this are constructed on a precision turntable with a stepper motor, and typically allow experiments to be conducted over a 10 -160 angular range. 21
  22. 22. Detector system PMTs are almost universally used as detectors in DLS experiments. Single photon counting mode (SPCM) which incorporates an avalanche photo diode (APD), active reset and quenching electronics and a Peltier-type temperature controller in a small package. 22
  23. 23. Digital correlator The ACF is formed by recording the number of photons arriving in each sample time, maintaining a history of this signal over a large range of sample times (time series), multiplying the instantaneous and the delayed signal for a range of time delays & accumulating these products. 23
  24. 24.  Optical mixing mode : Self beating, homodyning & heterodyning The typical measurement duration is from 1 to 10 minutes.  The DLS technique is commonly employed in the range of 0.002 to 2 microns.  The sample must be a liquid, solution or suspension & very dilute too, otherwise scattering of light can be unclear. 24
  25. 25. Advantages • Measurements are fast, from seconds to minutes. • Very small quantities of sample can be measured. • Any suitable suspending liquid (non-absorbing, relatively clear and not too viscous) can be used. • The technique is applicable from about 0.001 to several microns. 25
  26. 26. Disadvantages • It does not produce a high-resolution histogram of the size distribution. • Shape information is not easily obtained. • Multiple scattering affects the data analysis. • Dust can make measurement and interpretation difficult. 26
  27. 27. Electron Probe Characterization Techniques Acronym Technique Utility SEM Scanning electron microscopy Raster imaging/topology morphology EPMA Electron probe microanalysis Particle size/local chemical analysis TEM Transmission electron microscopy Imaging/particle size-shape HRTEM High-resolution transmission electron microscopy Imaging structure chemical analysis STEM Scanning transmission electron microscopy Biological samples LEED Low-energy electron diffraction Surface/adsorbate bonding EELS Electron energy loss spectroscopy Inelastic electron interactions AES Auger electron spectroscopy Chemical surface analysis 27
  28. 28. Scanning Electron Microscopy 28
  29. 29. Basic principle When the beam of electrons strikes the surface of the specimen & interacts with the atoms of the sample, signals in the form of secondary electrons, back scattered electrons & characteristic X-rays are generated that contain information about the samples‟ surface topography, composition etc. 29
  30. 30. Operation modes There are 3 modes – Primary: High resolution (1-5 nm); secondary electron imaging Secondary: Characteristic X-rays; identification of elemental composition of sample by EDX technique Tertiary: Back-scattered electronic images; clues to the elemental composition of sample 30
  31. 31. The typical SEM, the beam passes distribution of scanning Electronic displayed used to detect & amplify the signals & In a imagedevices are is therefore athrough pairs map of the intensity of the deflector on a in from the scanned to display pairs of an image platescathode ray tube in which of coils or them as signal being emittedthe electron columnareathe raster scanning deflect the beam horizontally & vertically. final lens, whichis synchronized with that of the microscope. the specimen. 31
  32. 32.  The sample must be electrically conductive at the surface.  Time consuming & expensive.  Sometimes it is not possible to clearly differentiate nanoparticle from the substrate.  SEM can‟t resolve the internal structure of these domains.  SEM can yield valuable information regarding the purity as well as degree of aggregation. 32
  33. 33. Environmental SEM In ESEM, samples can be looked at in a low pressure gas environment While using ESEM it is not necessary to make nonconductive positive as opposed to a vacuum. GSED posseses as much as a 600-Volt samples conductive. attract secondary do not need to to desiccated and bias on it to Materials sampleselectrons compared be the ET SED on a coated with gold–palladium, for example, and a 300-Volt original normal SEM, which ordinarily has only as much as thus their positive characteristics the be preserved for further testing or manipulation. bias and also may former is relatively far from the sample. Thus the GSED is set up to collect secondary electrons very efficiently. 33
  34. 34. Transmission Electron Microscopy 34
  35. 35. Basic principle The crystalline sample interacts with the electron beam mostly by diffraction rather than by absorption. The intensity of the diffraction depends on the orientation of the planes of atoms in a crystal relative to the electron beam. A high contrast image can be formed by blocking deflected electrons which produces a variation in the electron intensity that reveals information on the crystal structure. This can generate both „bright or light field‟ & „dark field‟ images. 35
  36. 36.  TEM enables Direct 2-D imaging of particle size, shape & surface characteristics.  Changes in nanoparticle structure as a result of interactions with gas, liquid & solid-phase substrates can also be monitored.  Sample must be able to withstand the electron beam & also the high vacuum chamber.  Time consuming.  It needs an analysis by image treatment & must be performed on a statistically significant large no. of samples. 36
  37. 37. HRTEM HRTEM is an imaging mode of TEM that allows the imaging of the crystallographic structure of a sample at an atomic scale. Independent interaction with the sample results the electron wave to pass through the imaging system of the microscope where it undergoes further phase change & interferes as the image wave in the imaging plane. The recorded image is not a direct representation of the samples crystallographic structure. It can be used to study local microstructures like lattice fringe, glide plane or screw axes & the surface atomic arrangement of crystalline nanoparticles. 37
  38. 38. TEM comparison Standard TEM High resolution TEM Courtesy of F. Ernst 38
  39. 39. Scanning Transmission Electron Microscopy This technique works as a mapping device unlike TEM where a stationary, parallel electron beam is used to form images. In STEM, a fine electron probe is scanned over a sample. Since it is a serial recording, the image generation takes longer time as compared to that in TEM. It combines the ideas of looking at the surface of the sample and into the sample with an electron beam. STEM is an invaluable tool for the characterization of nanostructures, providing a range of different imaging modes with the ability to provide information on elemental composition and electronic structure at the ultimate sensitivity. 39
  40. 40. The STEM works on the same principle as the normal SEM, by forming a focused beam of electrons that is scanned over the sample while some desired signal is collected to form an image. The difference with SEM is that thin specimens are used so that transmission modes of imaging are also available. A new possibility is opened up by the new aberration corrected STEMs. Correcting the lens aberrations allows the objective aperture to be opened up, thereby obtaining higher resolution. At the same time, as in an optical instrument aberration corrected STEMs have a depth Present-daylike a camera, the depth of field is reduced. of field of only a few nanometers, and so it becomes possible to effectively depth slice through a sample and to reconstruct the set of images into a 3D representation of the structure. The technique is comparable to confocal optical microscopy, but provides a resolution on nanoscale. 40
  41. 41. Scanning Probe Characterization Techniques Acronym Technique Utility AFM Atomic force microscopy Topology/imaging/surface structure CFM Chemical force microscopy Chemical/surface analysis MFM Magnetic force microscopy Magnetic materials analysis STM Scanning tunneling microscopy Topology/imaging/surface structure APM Atomic probe microscopy Three-dimensional imaging FIM Field ion microscopy Chemical profiles/atomic spacing APT Atomic probe tomography Position sensitive lateral location of atoms 41
  42. 42. Atomic Force Microscopy 42
  43. 43. Basic principle A AFM, a operating parameter is maintained nm) located level & end of Changes in the tip consisting interaction tip(~ 10 atmonitored using the images Inparticularprobe specimen of a sharp are often a constantnear an optical are generated system, in which a loop between the optical detection using lever detectionthrough a feedback laser is reflected off the cantilever &system a cantilever beam is raster scanned across the surface of a specimenonto a & the piezoelectric scanners. position-sensitive photodiode. piezoelectric scanners. 43
  44. 44. AFM modes Contact mode Non-contact mode Tapping mode Tip scans in close contact with surface (repelled) Constant force Highest resolution May damage surface Tip hovers above the surface (attracted) Variable force measured Lowest resolution Non-destructive Intermittent tip contact Variable force measured Improved resolution Non-destructive 44 Courtesy of F. Ernst
  45. 45. Qualitative analysis The AFM offers visualization in three dimensions. Resolution in the vertical, or Z, axis is limited by the vibration environment of the instrument, whereas resolution in the horizontal, or X-Y, axis is limited by the diameter of tip utilized for scanning. Typically, AFM instruments have vertical resolutions of less than 0.1 nm and X-Y resolutions of around 1 nm. 45
  46. 46. Figure: Left: NIST traceable polystyrene microspheres from Duke Scientific scanned with the NANO-RP™. Mean Ø of microspheres is 102nm. Scan size is 1μm x 1μm. Right: 3D view of 1x1μm scan of calibrated spheres Here 73nm NIST traceable microspheres are shown in both perspective view and top view. 3D information is incorporated in both views. In the perspective view, the 3D nature of the image is obvious. In the top view, the intensity of the color reflects the height of the particle. 46
  47. 47. Quantitative analysis For individual particles, size information (length, width, and height) and other physical properties (such as morphology and surface texture) can be measured. Figure: A wood particle scanned with an AFM to measure roughness. Paper products containing such wood fibers can vary in quality based on the physical properties of the particulates. 47
  48. 48. Statistics on groups of particles can also be measured through image analysis and data processing. Commonly desired ensemble statistics include particle counts, particle size distribution, surface area distribution and volume distribution. With knowledge of the material density, mass distribution can be easily calculated. Figure: Left: Latex particles outlined and counted. Right: Particle size distribution of polymer nanospheres. Mean Ø = 102nm 48
  49. 49. Experimental media AFM can be performed in liquid or gas mediums. This capability can be very advantageous for nanoparticle characterization. For example, a major component of the combustion-generated nanoparticles are volatile components that are only present in ambient conditions. Dry particles can be scanned in both ambient air and in controlled environments, such as nitrogen or argon gas. Liquid dispersions of particles can also be scanned, provided the dispersant is not corrosive to the probe tip and can be anchored to the substrate. 49
  50. 50. Particles dispersed in a solid matrix can also be analyzed by topographical or material sensing scans of cross-sections of the composite material. Such a technique is useful for investigating spatial nanocomposites. Fig: Left: Ni3Al precipitates in a nickel aluminum alloy. 27 μm x 27μm topography image. Right: 6.8 x 6.8 μm grain particle on super plastic ceramic. Courtesy of Dr. McCartney group, UCI. 50
  51. 51. In many industries, the ability to scan from the nanometer range into the micron range is important. With AFM, particles anywhere from 1nm to 5μm in height can be measured in a single scan. AFM can characterize nanoparticles in multiple mediums including ambient air, controlled environments & even liquid dispersions. Less costly & less time consuming. The roughness of the substrate must be less than the size of nanoparticles being measured. 51
  52. 52. SEM and AFM images Fig. SEM & AFM images of Cu Nanowires Courtesy of F. Ernst R. Adelung et al. 52
  53. 53. Scanning Tunneling Microscopy
  54. 54. Basic principle It is based on the concept of quantum tunneling. When a conducting tip is brought very near to a metallic or semi-conducting surface, a bias between the two can allow electrons to tunnel through the vacuum between them. Variations in tunneling current as the probe passes over the surface are translated into an image. They normally generate image by holding the current between the tip of the electrode & the specimen at some constant value by using a piezoelectric crystal to adjust the distance between the tip & the specimen surface. 54
  55. 55. Fig. Highly oriented pyrolytic graphite sheet under STM Lateral resolution ~ 0.1 nm Depth resolution ~ 0.01 nm STM can be used not only in ultra high vacuum but also in air & various other liquid or gas, at ambient & wide range of temperature. STM can be a challenging technique, as it requires extremely clean surfaces & sharp tips. 55
  56. 56. Photon(Spectroscopic) Probe Characterization Techniques Acronym Technique Utility UPS Ultraviolet photoemission spectroscopy Surface analysis UVVS UV-visible spectroscopy Chemical analysis AAS Atomic absorption spectroscopy Chemical analysis ICP Inductively coupled plasma spectroscopy Elemental analysis FS Fluorescence spectroscopy Elemental analysis LSPR Localized surface Plasmon resonance Nanosized particle analysis 56
  57. 57. Ion-particle Probe Characterization Techniques Acronym Technique Utility RBS Rutherford back scattering Quantitative-qualitative elemental analysis SANS Small angle neutron scattering Surface characterization NRA Nuclear reaction analysis Depth profiling of solid thin films RS Raman spectroscopy Vibration analysis XRD X-ray diffraction Crystal structure EDX Energy dispersive X-ray spectroscopy Elemental analysis SAXS Small angle X-ray scattering Surface analysis/particle sizing(1-100 nm) CLS Cathodoluminescence Characteristic emission NMR Nuclear magnetic resonance spectroscopy Analysis of odd no. nuclear species 57
  58. 58. X-ray Diffraction XRD can be used to look at various characteristics of the single crystal or polycrystalline materials using Bragg’s Law , nλ = 2d sinθ The use of XRD is often compared to the microscopy techniques. XRD avoids issues of representative samples and determining crystals as opposed to particles as discussed above. XRD is time consuming and requires a large volume of sample. 58
  59. 59. Thermodynamic Characterization Techniques Acronym Technique Utility TGA Thermal gravimetric analysis Mass loss vs. temperature DTA Differential thermal analysis Reaction heats heat capacity DSC Differential scanning calorimetry Reaction heats phase changes NC Nanocalorimetry Latent heats of fusion BET Brunauer-Emmett-Teller method Surface area analysis Sears Sears method Colloid size, specific surface area 59
  60. 60. Other Important Techniques  Nanoparticle tracking analysis  Tilted laser Microscopy  Turbidimetry  Field Flow Fractionation  Hydrophobic interaction Chromatography  Electrophoresis  Isopycnic Centrifugation  Zeta potential measurements 60
  61. 61. 61
  62. 62. Characterization of curcumin nanoparticles (Jain et al., 2011) for anti-microbial study. Instruments used : 30 nm DLS : Malvern Zetasizer S90 series TEM : Morgagni 268 D from FEI SEM : Jeol JSM 840 microscope ~2-40 nm ~50 nm Fig. Size characterization of curcumin nanoparticles (a) DLS (b) TEM (c) SEM image 62
  63. 63. Characterization of potato & cassava starch nanoparticles (Szymońska; 2009) using AFM(Park Scientific Instrument Autoprobe CP II model & the AFM Ultralevers tips of Veeco). Fig. High resolution nc-AFM images & dimensions of potato starch nanoparticles Fig. High resolution nc-AFM images and 63 dimensions of cassava starch nanoparticles
  64. 64. Characterization of a novel photodegradable insecticide nano-imidacloprid (Chi et al., 2008) . Imidacloprid (IMI) microcrystals were directly encapsulated with nature polysaccharides chitosan (CHI) & sodium alginate (ALG) through layer-by-layer (LbL) self-assembly. The coated colloids were characterized using confocal laser scanning microscopy (CLSM) and scanning electron microscopy (SEM). 64
  65. 65. Fig. Transmission CLSM images of the IMI release process from the (CHI/ALG)10 microcapsules. (a) Morphologies of IMI microcrystal before dissolution. (b) Images of IMI microcrystal in dissolution. (c) Images of polysaccharide capsules after removal of the crystal cores Fig. SEM images of IMI microcrystals (a) uncoated, (b) coated with 5 layers of CHI/ALG, (c) coated with 10 layers of CHI-ALG. 65
  66. 66. Summary Nanoparticle - Properties - Application Nanoparticle Characterization - Methods - Comparative analysis Case Study
  67. 67. Nanotechnology is the essence of molecular synthesis, manipulation, and manufacturing. Nanoparticle-based technologies cover different fields, ranging from environmental remediation, energy generation and most recent applications in bioscience. Nanoparticles, are, key components in the development of new advanced technologies. 16/07/2011 Division of Agricultural Chemicals 67
  68. 68. Nanoparticle characterization is necessary to establish understanding and control of nanoparticle synthesis and applications. Nanotechnology has a lot of potential as a futuristic approach but would be largely governed by simultaneous progress in the newer, faster, simpler & more efficient characterization techniques for nanoparticles. 16/07/2011 Division of Agricultural Chemicals 68
  69. 69. Path Ahead Integration of different techniques for better understanding of particle characters AFM with modern probes for attachment with fluoroscent particles to study rate kinetics/degradation kinetics Integration of surface morphology based techniques with 3D imaging techniques 69
  70. 70. Than k 70

×