Review



k562 suspension cells  (ATCC)


Bioz Verified Symbol ATCC is a verified supplier
Bioz Manufacturer Symbol ATCC manufactures this product  
  • Logo
  • About
  • News
  • Press Release
  • Team
  • Advisors
  • Partners
  • Contact
  • Bioz Stars
  • Bioz vStars
  • 99

    Structured Review

    ATCC k562 suspension cells
    ( A ) Working principle of STAT. (i) Two orthogonal standing SAW fields with slightly detuned frequencies, ω x and ω y , pattern PACPs (red) and NACPs (blue) in distinct pressure regions; inset: photo of the STAT chip. (ii) Pressure-field evolution over one detuning cycle (0 to 2π/Δω), showing dynamic shifts of pressure nodes and antinodes induced by the frequency difference Δω. (iii) Schematic of the dynamic, static, and drag forces acting on PACPs and NACPs. ( B ) (i) High-throughput, low-frequency, shear-like oscillation of PACPs under the dynamic force field distribution. (ii) Time-lapse images over one oscillation cycle with 10-μm polystyrene beads in water. ( C ) (i) High-throughput, low-frequency, longitudinal-like oscillation of NACPs within patterned PACPs. Time-lapse images over one oscillation cycle with PDMS clusters within an arrayed pattern of 10 μm polystyrene beads. (ii) Experimental demonstration of selective navigation of a PDMS cluster through a locally stationary polystyrene-bead lattice. ( D ) Schematics and experiments showing that STAT enables (i) gentle oscillation of biological cells and (ii) controllable transport of NACPs while maintaining cells in a patterned lattice. In (B) to (D), the polystyrene beads, PDMS clusters, and <t>K562</t> cells are highlighted in red, blue, and light green, respectively. Oscillation was captured at ω x /2π = 20.094 MHz and ω y /2π = 20.094 MHz − 1 Hz, corresponding to Δω = 1 × 2π Hz, when P x > P y . In (C) and (D), black and green arrows represent transport and oscillation directions, respectively. Scale bars, 45 μm.
    K562 Suspension Cells, supplied by ATCC, used in various techniques. Bioz Stars score: 99/100, based on 10907 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/result/k562 suspension cells/product/ATCC
    Average 99 stars, based on 10907 article reviews
    k562 suspension cells - by Bioz Stars, 2026-05
    99/100 stars

    Images

    1) Product Images from "Space-time acoustofluidic tweezers for dynamic and selective manipulation of microparticles"

    Article Title: Space-time acoustofluidic tweezers for dynamic and selective manipulation of microparticles

    Journal: Science Advances

    doi: 10.1126/sciadv.aee2983

    ( A ) Working principle of STAT. (i) Two orthogonal standing SAW fields with slightly detuned frequencies, ω x and ω y , pattern PACPs (red) and NACPs (blue) in distinct pressure regions; inset: photo of the STAT chip. (ii) Pressure-field evolution over one detuning cycle (0 to 2π/Δω), showing dynamic shifts of pressure nodes and antinodes induced by the frequency difference Δω. (iii) Schematic of the dynamic, static, and drag forces acting on PACPs and NACPs. ( B ) (i) High-throughput, low-frequency, shear-like oscillation of PACPs under the dynamic force field distribution. (ii) Time-lapse images over one oscillation cycle with 10-μm polystyrene beads in water. ( C ) (i) High-throughput, low-frequency, longitudinal-like oscillation of NACPs within patterned PACPs. Time-lapse images over one oscillation cycle with PDMS clusters within an arrayed pattern of 10 μm polystyrene beads. (ii) Experimental demonstration of selective navigation of a PDMS cluster through a locally stationary polystyrene-bead lattice. ( D ) Schematics and experiments showing that STAT enables (i) gentle oscillation of biological cells and (ii) controllable transport of NACPs while maintaining cells in a patterned lattice. In (B) to (D), the polystyrene beads, PDMS clusters, and K562 cells are highlighted in red, blue, and light green, respectively. Oscillation was captured at ω x /2π = 20.094 MHz and ω y /2π = 20.094 MHz − 1 Hz, corresponding to Δω = 1 × 2π Hz, when P x > P y . In (C) and (D), black and green arrows represent transport and oscillation directions, respectively. Scale bars, 45 μm.
    Figure Legend Snippet: ( A ) Working principle of STAT. (i) Two orthogonal standing SAW fields with slightly detuned frequencies, ω x and ω y , pattern PACPs (red) and NACPs (blue) in distinct pressure regions; inset: photo of the STAT chip. (ii) Pressure-field evolution over one detuning cycle (0 to 2π/Δω), showing dynamic shifts of pressure nodes and antinodes induced by the frequency difference Δω. (iii) Schematic of the dynamic, static, and drag forces acting on PACPs and NACPs. ( B ) (i) High-throughput, low-frequency, shear-like oscillation of PACPs under the dynamic force field distribution. (ii) Time-lapse images over one oscillation cycle with 10-μm polystyrene beads in water. ( C ) (i) High-throughput, low-frequency, longitudinal-like oscillation of NACPs within patterned PACPs. Time-lapse images over one oscillation cycle with PDMS clusters within an arrayed pattern of 10 μm polystyrene beads. (ii) Experimental demonstration of selective navigation of a PDMS cluster through a locally stationary polystyrene-bead lattice. ( D ) Schematics and experiments showing that STAT enables (i) gentle oscillation of biological cells and (ii) controllable transport of NACPs while maintaining cells in a patterned lattice. In (B) to (D), the polystyrene beads, PDMS clusters, and K562 cells are highlighted in red, blue, and light green, respectively. Oscillation was captured at ω x /2π = 20.094 MHz and ω y /2π = 20.094 MHz − 1 Hz, corresponding to Δω = 1 × 2π Hz, when P x > P y . In (C) and (D), black and green arrows represent transport and oscillation directions, respectively. Scale bars, 45 μm.

    Techniques Used: High Throughput Screening Assay, Shear, Gentle

    ( A ) Images of K562 cells, showing a half-cycle oscillation with ζ x and ζ y denoting oscillation displacements in x and y . ( B ) Measured cell oscillation displacements as functions of frequency detuning Δω. Green bars show ζ x , while blue bars indicate ζ y . ( C ) Measured cell oscillation displacements as functions of driving voltage amplitudes V x when V y = 11 V pp and V y when V x = 11 V pp . ( D ) Schematics illustrating how tuning Δ P and Δω controls the transport of a PDMS cluster between a lattice pattern of K562 cells, showing gentle oscillations around stable pressure nodes. ( E ) Time-elapse images of tuning Δω and Δ P to selectively manipulate a PDMS cluster through an effectively stationary K562 cell pattern.
    Figure Legend Snippet: ( A ) Images of K562 cells, showing a half-cycle oscillation with ζ x and ζ y denoting oscillation displacements in x and y . ( B ) Measured cell oscillation displacements as functions of frequency detuning Δω. Green bars show ζ x , while blue bars indicate ζ y . ( C ) Measured cell oscillation displacements as functions of driving voltage amplitudes V x when V y = 11 V pp and V y when V x = 11 V pp . ( D ) Schematics illustrating how tuning Δ P and Δω controls the transport of a PDMS cluster between a lattice pattern of K562 cells, showing gentle oscillations around stable pressure nodes. ( E ) Time-elapse images of tuning Δω and Δ P to selectively manipulate a PDMS cluster through an effectively stationary K562 cell pattern.

    Techniques Used: Gentle



    Similar Products

    99
    ATCC k562 suspension cells
    ( A ) Working principle of STAT. (i) Two orthogonal standing SAW fields with slightly detuned frequencies, ω x and ω y , pattern PACPs (red) and NACPs (blue) in distinct pressure regions; inset: photo of the STAT chip. (ii) Pressure-field evolution over one detuning cycle (0 to 2π/Δω), showing dynamic shifts of pressure nodes and antinodes induced by the frequency difference Δω. (iii) Schematic of the dynamic, static, and drag forces acting on PACPs and NACPs. ( B ) (i) High-throughput, low-frequency, shear-like oscillation of PACPs under the dynamic force field distribution. (ii) Time-lapse images over one oscillation cycle with 10-μm polystyrene beads in water. ( C ) (i) High-throughput, low-frequency, longitudinal-like oscillation of NACPs within patterned PACPs. Time-lapse images over one oscillation cycle with PDMS clusters within an arrayed pattern of 10 μm polystyrene beads. (ii) Experimental demonstration of selective navigation of a PDMS cluster through a locally stationary polystyrene-bead lattice. ( D ) Schematics and experiments showing that STAT enables (i) gentle oscillation of biological cells and (ii) controllable transport of NACPs while maintaining cells in a patterned lattice. In (B) to (D), the polystyrene beads, PDMS clusters, and <t>K562</t> cells are highlighted in red, blue, and light green, respectively. Oscillation was captured at ω x /2π = 20.094 MHz and ω y /2π = 20.094 MHz − 1 Hz, corresponding to Δω = 1 × 2π Hz, when P x > P y . In (C) and (D), black and green arrows represent transport and oscillation directions, respectively. Scale bars, 45 μm.
    K562 Suspension Cells, supplied by ATCC, used in various techniques. Bioz Stars score: 99/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/result/k562 suspension cells/product/ATCC
    Average 99 stars, based on 1 article reviews
    k562 suspension cells - by Bioz Stars, 2026-05
    99/100 stars
      Buy from Supplier

    86
    Merck & Co suspension cell line k562
    ( A ) Working principle of STAT. (i) Two orthogonal standing SAW fields with slightly detuned frequencies, ω x and ω y , pattern PACPs (red) and NACPs (blue) in distinct pressure regions; inset: photo of the STAT chip. (ii) Pressure-field evolution over one detuning cycle (0 to 2π/Δω), showing dynamic shifts of pressure nodes and antinodes induced by the frequency difference Δω. (iii) Schematic of the dynamic, static, and drag forces acting on PACPs and NACPs. ( B ) (i) High-throughput, low-frequency, shear-like oscillation of PACPs under the dynamic force field distribution. (ii) Time-lapse images over one oscillation cycle with 10-μm polystyrene beads in water. ( C ) (i) High-throughput, low-frequency, longitudinal-like oscillation of NACPs within patterned PACPs. Time-lapse images over one oscillation cycle with PDMS clusters within an arrayed pattern of 10 μm polystyrene beads. (ii) Experimental demonstration of selective navigation of a PDMS cluster through a locally stationary polystyrene-bead lattice. ( D ) Schematics and experiments showing that STAT enables (i) gentle oscillation of biological cells and (ii) controllable transport of NACPs while maintaining cells in a patterned lattice. In (B) to (D), the polystyrene beads, PDMS clusters, and <t>K562</t> cells are highlighted in red, blue, and light green, respectively. Oscillation was captured at ω x /2π = 20.094 MHz and ω y /2π = 20.094 MHz − 1 Hz, corresponding to Δω = 1 × 2π Hz, when P x > P y . In (C) and (D), black and green arrows represent transport and oscillation directions, respectively. Scale bars, 45 μm.
    Suspension Cell Line K562, supplied by Merck & Co, used in various techniques. Bioz Stars score: 86/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/result/suspension cell line k562/product/Merck & Co
    Average 86 stars, based on 1 article reviews
    suspension cell line k562 - by Bioz Stars, 2026-05
    86/100 stars
      Buy from Supplier

    99
    ATCC suspension k562 cells
    a Experiment setup of the scanning-based SLEC. The cells were sandwiched within a mirror-formed FP cavity. The upper mirror was spin-coated with a dye-doped PS layer, functioning as the gain medium. By adjusting the pump energy, lasing emissions can be achieved only within the nucleolus regions. b Laser threshold and emitting spectrum in regions with and without nucleolus. c Co-localization of the laser emission image with phase contrast image and fluorescence image from nucleolus dye. A549 cells were cultured on the lower mirror as an illustrative example. Scale bar: 5 μm. d Enlarged comparison among phase contrast image, laser emission image and fluorescence image. Scale bar: 5 μm. The lasing emission image indicated distinct subareas attributed to the nucleolus’ inhomogeneity of the refractive index (red arrows indicated). e Configuration of the scanning-based SLEC for tissue sections. f Configuration of the flow-based SLEC for suspended cells. Phase contrast image of a live <t>K562</t> cell (20X objective), the nucleolus laser emission hyperspectral image and its spectrum. Scale bar: 5 μm. Each nucleolus corresponds to its unique laser peak.
    Suspension K562 Cells, supplied by ATCC, used in various techniques. Bioz Stars score: 99/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/result/suspension k562 cells/product/ATCC
    Average 99 stars, based on 1 article reviews
    suspension k562 cells - by Bioz Stars, 2026-05
    99/100 stars
      Buy from Supplier

    99
    ATCC k562 suspension lymphoblast cells
    Cell flow dynamics and encapsulation in phosphate-buffered saline. The <t>lymphoblast</t> <t>(K562)</t> cells suspended in 1× PBS buffer are being continuously injected into a microfluidics device, and cells passing through the observation chamber on a microfluidics device are counted every 20 s. (A) Time trace of cells traversing the observation chamber in 1× PBS buffer (ρ sol = 1.00 g/mL). The inset displays the same data but with the Y -axis (cell count) in a log scale. The cell flow dynamics exhibited three characteristic stages (I, II, III) that markedly differed in droplet occupancies by single cells, 0.01 > λ > 1. (B) Digital photographs of droplets collected at different time points during the experiment. The cells are highlighted in red.
    K562 Suspension Lymphoblast Cells, supplied by ATCC, used in various techniques. Bioz Stars score: 99/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/result/k562 suspension lymphoblast cells/product/ATCC
    Average 99 stars, based on 1 article reviews
    k562 suspension lymphoblast cells - by Bioz Stars, 2026-05
    99/100 stars
      Buy from Supplier

    Image Search Results


    ( A ) Working principle of STAT. (i) Two orthogonal standing SAW fields with slightly detuned frequencies, ω x and ω y , pattern PACPs (red) and NACPs (blue) in distinct pressure regions; inset: photo of the STAT chip. (ii) Pressure-field evolution over one detuning cycle (0 to 2π/Δω), showing dynamic shifts of pressure nodes and antinodes induced by the frequency difference Δω. (iii) Schematic of the dynamic, static, and drag forces acting on PACPs and NACPs. ( B ) (i) High-throughput, low-frequency, shear-like oscillation of PACPs under the dynamic force field distribution. (ii) Time-lapse images over one oscillation cycle with 10-μm polystyrene beads in water. ( C ) (i) High-throughput, low-frequency, longitudinal-like oscillation of NACPs within patterned PACPs. Time-lapse images over one oscillation cycle with PDMS clusters within an arrayed pattern of 10 μm polystyrene beads. (ii) Experimental demonstration of selective navigation of a PDMS cluster through a locally stationary polystyrene-bead lattice. ( D ) Schematics and experiments showing that STAT enables (i) gentle oscillation of biological cells and (ii) controllable transport of NACPs while maintaining cells in a patterned lattice. In (B) to (D), the polystyrene beads, PDMS clusters, and K562 cells are highlighted in red, blue, and light green, respectively. Oscillation was captured at ω x /2π = 20.094 MHz and ω y /2π = 20.094 MHz − 1 Hz, corresponding to Δω = 1 × 2π Hz, when P x > P y . In (C) and (D), black and green arrows represent transport and oscillation directions, respectively. Scale bars, 45 μm.

    Journal: Science Advances

    Article Title: Space-time acoustofluidic tweezers for dynamic and selective manipulation of microparticles

    doi: 10.1126/sciadv.aee2983

    Figure Lengend Snippet: ( A ) Working principle of STAT. (i) Two orthogonal standing SAW fields with slightly detuned frequencies, ω x and ω y , pattern PACPs (red) and NACPs (blue) in distinct pressure regions; inset: photo of the STAT chip. (ii) Pressure-field evolution over one detuning cycle (0 to 2π/Δω), showing dynamic shifts of pressure nodes and antinodes induced by the frequency difference Δω. (iii) Schematic of the dynamic, static, and drag forces acting on PACPs and NACPs. ( B ) (i) High-throughput, low-frequency, shear-like oscillation of PACPs under the dynamic force field distribution. (ii) Time-lapse images over one oscillation cycle with 10-μm polystyrene beads in water. ( C ) (i) High-throughput, low-frequency, longitudinal-like oscillation of NACPs within patterned PACPs. Time-lapse images over one oscillation cycle with PDMS clusters within an arrayed pattern of 10 μm polystyrene beads. (ii) Experimental demonstration of selective navigation of a PDMS cluster through a locally stationary polystyrene-bead lattice. ( D ) Schematics and experiments showing that STAT enables (i) gentle oscillation of biological cells and (ii) controllable transport of NACPs while maintaining cells in a patterned lattice. In (B) to (D), the polystyrene beads, PDMS clusters, and K562 cells are highlighted in red, blue, and light green, respectively. Oscillation was captured at ω x /2π = 20.094 MHz and ω y /2π = 20.094 MHz − 1 Hz, corresponding to Δω = 1 × 2π Hz, when P x > P y . In (C) and (D), black and green arrows represent transport and oscillation directions, respectively. Scale bars, 45 μm.

    Article Snippet: K562 suspension cells and B16-F10 adherent melanoma cells were cultured in RPMI 1640 [American Type Culture Collection (ATCC), 30-2001] and Dulbecco’s modified Eagle’s medium (ATCC, 30-2002), respectively.

    Techniques: High Throughput Screening Assay, Shear, Gentle

    ( A ) Images of K562 cells, showing a half-cycle oscillation with ζ x and ζ y denoting oscillation displacements in x and y . ( B ) Measured cell oscillation displacements as functions of frequency detuning Δω. Green bars show ζ x , while blue bars indicate ζ y . ( C ) Measured cell oscillation displacements as functions of driving voltage amplitudes V x when V y = 11 V pp and V y when V x = 11 V pp . ( D ) Schematics illustrating how tuning Δ P and Δω controls the transport of a PDMS cluster between a lattice pattern of K562 cells, showing gentle oscillations around stable pressure nodes. ( E ) Time-elapse images of tuning Δω and Δ P to selectively manipulate a PDMS cluster through an effectively stationary K562 cell pattern.

    Journal: Science Advances

    Article Title: Space-time acoustofluidic tweezers for dynamic and selective manipulation of microparticles

    doi: 10.1126/sciadv.aee2983

    Figure Lengend Snippet: ( A ) Images of K562 cells, showing a half-cycle oscillation with ζ x and ζ y denoting oscillation displacements in x and y . ( B ) Measured cell oscillation displacements as functions of frequency detuning Δω. Green bars show ζ x , while blue bars indicate ζ y . ( C ) Measured cell oscillation displacements as functions of driving voltage amplitudes V x when V y = 11 V pp and V y when V x = 11 V pp . ( D ) Schematics illustrating how tuning Δ P and Δω controls the transport of a PDMS cluster between a lattice pattern of K562 cells, showing gentle oscillations around stable pressure nodes. ( E ) Time-elapse images of tuning Δω and Δ P to selectively manipulate a PDMS cluster through an effectively stationary K562 cell pattern.

    Article Snippet: K562 suspension cells and B16-F10 adherent melanoma cells were cultured in RPMI 1640 [American Type Culture Collection (ATCC), 30-2001] and Dulbecco’s modified Eagle’s medium (ATCC, 30-2002), respectively.

    Techniques: Gentle

    a Experiment setup of the scanning-based SLEC. The cells were sandwiched within a mirror-formed FP cavity. The upper mirror was spin-coated with a dye-doped PS layer, functioning as the gain medium. By adjusting the pump energy, lasing emissions can be achieved only within the nucleolus regions. b Laser threshold and emitting spectrum in regions with and without nucleolus. c Co-localization of the laser emission image with phase contrast image and fluorescence image from nucleolus dye. A549 cells were cultured on the lower mirror as an illustrative example. Scale bar: 5 μm. d Enlarged comparison among phase contrast image, laser emission image and fluorescence image. Scale bar: 5 μm. The lasing emission image indicated distinct subareas attributed to the nucleolus’ inhomogeneity of the refractive index (red arrows indicated). e Configuration of the scanning-based SLEC for tissue sections. f Configuration of the flow-based SLEC for suspended cells. Phase contrast image of a live K562 cell (20X objective), the nucleolus laser emission hyperspectral image and its spectrum. Scale bar: 5 μm. Each nucleolus corresponds to its unique laser peak.

    Journal: Nature Communications

    Article Title: Single-cell laser emitting cytometry for label-free nucleolus fingerprinting

    doi: 10.1038/s41467-024-51574-5

    Figure Lengend Snippet: a Experiment setup of the scanning-based SLEC. The cells were sandwiched within a mirror-formed FP cavity. The upper mirror was spin-coated with a dye-doped PS layer, functioning as the gain medium. By adjusting the pump energy, lasing emissions can be achieved only within the nucleolus regions. b Laser threshold and emitting spectrum in regions with and without nucleolus. c Co-localization of the laser emission image with phase contrast image and fluorescence image from nucleolus dye. A549 cells were cultured on the lower mirror as an illustrative example. Scale bar: 5 μm. d Enlarged comparison among phase contrast image, laser emission image and fluorescence image. Scale bar: 5 μm. The lasing emission image indicated distinct subareas attributed to the nucleolus’ inhomogeneity of the refractive index (red arrows indicated). e Configuration of the scanning-based SLEC for tissue sections. f Configuration of the flow-based SLEC for suspended cells. Phase contrast image of a live K562 cell (20X objective), the nucleolus laser emission hyperspectral image and its spectrum. Scale bar: 5 μm. Each nucleolus corresponds to its unique laser peak.

    Article Snippet: The Caco-2 cells and suspension K562 cells from ATCC were cultured in RPMI 1640 with 10% FBS and 100 U mL −1 penicillin/streptomycin.

    Techniques: Fluorescence, Cell Culture, Comparison, Refractive Index

    a Configuration of the SLEC chip mounted on the microscope system and the schematic of the flow cytometry. Scale bar: 20 μm. b Four main parameters extracted from the nucleolus laser spectrum. c Phase contrast images of the suspension cells K562 and the Caco−2 cells in the suspension state. Scale bar: 20 μm. d Nucleolus laser spectral fingerprints in laser peak number, average laser peak intensity, laser peak intensity variance, and low intensity (<3e3) percentage. (A549: n = 1121, K562: n = 1182, Caco−2: n = 1276, C2C12: n = 1227). e t-SNE visualization of the laser spectral data of nucleolus. Source data are provided as a Source Data file.

    Journal: Nature Communications

    Article Title: Single-cell laser emitting cytometry for label-free nucleolus fingerprinting

    doi: 10.1038/s41467-024-51574-5

    Figure Lengend Snippet: a Configuration of the SLEC chip mounted on the microscope system and the schematic of the flow cytometry. Scale bar: 20 μm. b Four main parameters extracted from the nucleolus laser spectrum. c Phase contrast images of the suspension cells K562 and the Caco−2 cells in the suspension state. Scale bar: 20 μm. d Nucleolus laser spectral fingerprints in laser peak number, average laser peak intensity, laser peak intensity variance, and low intensity (<3e3) percentage. (A549: n = 1121, K562: n = 1182, Caco−2: n = 1276, C2C12: n = 1227). e t-SNE visualization of the laser spectral data of nucleolus. Source data are provided as a Source Data file.

    Article Snippet: The Caco-2 cells and suspension K562 cells from ATCC were cultured in RPMI 1640 with 10% FBS and 100 U mL −1 penicillin/streptomycin.

    Techniques: Microscopy, Flow Cytometry, Suspension

    Cell flow dynamics and encapsulation in phosphate-buffered saline. The lymphoblast (K562) cells suspended in 1× PBS buffer are being continuously injected into a microfluidics device, and cells passing through the observation chamber on a microfluidics device are counted every 20 s. (A) Time trace of cells traversing the observation chamber in 1× PBS buffer (ρ sol = 1.00 g/mL). The inset displays the same data but with the Y -axis (cell count) in a log scale. The cell flow dynamics exhibited three characteristic stages (I, II, III) that markedly differed in droplet occupancies by single cells, 0.01 > λ > 1. (B) Digital photographs of droplets collected at different time points during the experiment. The cells are highlighted in red.

    Journal: Analytical Chemistry

    Article Title: Increasing Fluid Viscosity Ensures Consistent Single-Cell Encapsulation

    doi: 10.1021/acs.analchem.3c05243

    Figure Lengend Snippet: Cell flow dynamics and encapsulation in phosphate-buffered saline. The lymphoblast (K562) cells suspended in 1× PBS buffer are being continuously injected into a microfluidics device, and cells passing through the observation chamber on a microfluidics device are counted every 20 s. (A) Time trace of cells traversing the observation chamber in 1× PBS buffer (ρ sol = 1.00 g/mL). The inset displays the same data but with the Y -axis (cell count) in a log scale. The cell flow dynamics exhibited three characteristic stages (I, II, III) that markedly differed in droplet occupancies by single cells, 0.01 > λ > 1. (B) Digital photographs of droplets collected at different time points during the experiment. The cells are highlighted in red.

    Article Snippet: K562 suspension lymphoblast cells (ATCC) and 9e10 semiadherent mouse hybridoma cells (ATCC) were cultured in RPMI 1640 and IMDM mediums, respectively, both supplemented with 10% (v/v) FBS and 1× PS.

    Techniques: Encapsulation, Saline, Injection, Cell Counting

    Cell flow dynamics in density-adjusted and viscosity-adjusted buffers. The time traces of lymphoblast (K562) cells are being continuously injected into the microfluidics device in density-adjusted and viscosity-adjusted buffers. (A) Cell flow dynamics in a density-adjusted buffer (ρ sol = 1.053 g/mL) composed of 1× PBS and 20% Optiprep. The inset displays the same data but with the Y -axis (cell count) in a log scale. (B) Cell flow dynamics in PBS buffer having different density values. (C) Cell flow dynamics in a viscosity-adjusted buffer (μ sol = 75 cPs) composed of 1× PBS and 15% dextran. The inset displays the same data but with the Y -axis (cell count) in a log scale. (D) Infusion of different types of cells in a viscosity-adjusted buffer. Solid symbols represent cell loading in 1× PBS supplemented with 15% dextran, and open symbols represent cell loading in 1× PBS supplemented with 0.05% xanthan gum. (E) Droplet occupancy over time in the presence of 15% dextran (MW 500k). (F) Droplet occupancy over time in the presence of 0.05% xanthan (MW 2000k). Scale bars: 100 μm.

    Journal: Analytical Chemistry

    Article Title: Increasing Fluid Viscosity Ensures Consistent Single-Cell Encapsulation

    doi: 10.1021/acs.analchem.3c05243

    Figure Lengend Snippet: Cell flow dynamics in density-adjusted and viscosity-adjusted buffers. The time traces of lymphoblast (K562) cells are being continuously injected into the microfluidics device in density-adjusted and viscosity-adjusted buffers. (A) Cell flow dynamics in a density-adjusted buffer (ρ sol = 1.053 g/mL) composed of 1× PBS and 20% Optiprep. The inset displays the same data but with the Y -axis (cell count) in a log scale. (B) Cell flow dynamics in PBS buffer having different density values. (C) Cell flow dynamics in a viscosity-adjusted buffer (μ sol = 75 cPs) composed of 1× PBS and 15% dextran. The inset displays the same data but with the Y -axis (cell count) in a log scale. (D) Infusion of different types of cells in a viscosity-adjusted buffer. Solid symbols represent cell loading in 1× PBS supplemented with 15% dextran, and open symbols represent cell loading in 1× PBS supplemented with 0.05% xanthan gum. (E) Droplet occupancy over time in the presence of 15% dextran (MW 500k). (F) Droplet occupancy over time in the presence of 0.05% xanthan (MW 2000k). Scale bars: 100 μm.

    Article Snippet: K562 suspension lymphoblast cells (ATCC) and 9e10 semiadherent mouse hybridoma cells (ATCC) were cultured in RPMI 1640 and IMDM mediums, respectively, both supplemented with 10% (v/v) FBS and 1× PS.

    Techniques: Viscosity, Injection, Cell Counting