| Literature DB >> 30538002 |
Xiangying Deng1,2,3, Fang Xiong2, Xiayu Li2,3, Bo Xiang1,2,3, Zheng Li1,2,3, Xu Wu2,4, Can Guo2, Xiaoling Li1,2,3, Yong Li2,5, Guiyuan Li1,2,3, Wei Xiong6,7,8, Zhaoyang Zeng9,10,11.
Abstract
Atomic force microscopy (AFM) allows for nanometer-scale investigation of cells and molecules. Recent advances have enabled its application in cancer research and diagnosis. The physicochemical properties of live cells undergo changes when their physiological conditions are altered. These physicochemical properties can therefore reflect complex physiological processes occurring in cells. When cells are in the process of carcinogenesis and stimulated by external stimuli, their morphology, elasticity, and adhesion properties may change. AFM can perform surface imaging and ultrastructural observation of live cells with atomic resolution under near-physiological conditions, collecting force spectroscopy information which allows for the study of the mechanical properties of cells. For this reason, AFM has potential to be used as a tool for high resolution research into the ultrastructure and mechanical properties of tumor cells. This review describes the working principle, working mode, and technical points of atomic force microscopy, and reviews the applications and prospects of atomic force microscopy in cancer research.Entities:
Keywords: Atomic force microscopy; Cancer cells; Mechanical properties; Morphology
Mesh:
Year: 2018 PMID: 30538002 PMCID: PMC6288943 DOI: 10.1186/s12951-018-0428-0
Source DB: PubMed Journal: J Nanobiotechnology ISSN: 1477-3155 Impact factor: 10.435
Comparison of representative methods in measuring cell mechanics [8, 14–16]
| Methods | Advantages | Disadvantages |
|---|---|---|
| Microfluidics | High throughput (~ 1 cell/s); ability to control cell environment and approximate physiological conditions | Be prone to cell adhesion and clogging; limited materials for fabricating devices; cell size is often neglected |
| Micropipette aspiration | Simple and cost-effective; large range of force (up to ~ 100 nN) | Low throughput; limited special resolution (< 1 cell/10 min); possible damage to cells; mainly for suspended cells |
| Micropost arrays | Ability to measure the traction forces of single cells or cell populations | Mainly for adherent cells; high cost and complexity; the topology of micropost arrays may influence cell activities |
| Magnetic twisting cytometry | Probing the local mechanics of cells; magnetic beads can be bound with diverse types of cellular molecules or structures | Low throughput (< 1 cell/min); difficult to standardize; only for unidirectional forces |
| Optical tweezers | High precision measurements of small forces (0.01–103 pN); can be integrated with microfluidic delivery | Limited force (< 500 pN) applied on cells; detrimental effects on cells due to heating |
| Parallel plate | Simple and cost-effective; ability to study single cells of cell populations | Low throughout; low spatial resolution |
| Atomic force microscopy | Applicable for both suspended cells and adherent cells; simultaneously obtain structural and mechanical information with nanometer resolution | Low throughput (< 1 cell/10 min); the mechanical poking of the AFM tip may influence cell activities |
Fig. 1Schematic diagram of AFM working principles. The AFM instrument is composed of a piezoelectric ceramic tube, a laser generator, a position-sensitive photodiode detector, a controller, and an AFM probe. The AFM probe is a micro-cantilever with a sharp tip attached at its end. The tip, which has a monomolecular point, allows for nanometer resolution imaging and the micro-cantilever is a force sensor that can detect even minute deformation of a sample, enabling very high sensitivity AFM in force measurements
Fig. 2Force-distance curve-based AFM. a Principle of force-distance (FD) curves by approaching (red) and withdrawing (blue) the AFM tip from the sample. The tip of the cantilever is initially distant from the sample [1] to which it is brought into contact [2]. During retraction [3] of the AFM tip, adhesive events may occur at different distances due to nonspecific [4] or specific [5] interactions between tip and sample. b The force-curve plot from an AFM measurement. The slope value is fitted with a linear fit (red line) (a), the adhesion is measured as a single value and the mechanical value of the point (b) indicates the adhesion force
Fig. 3Three basic working modes of AFM. a The curve of both interatomic force and intervals relation. b In contact mode the probe is always slightly contact with the sample and scanned in a constant force mode. c In the non-contact mode the tip of the needle always vibrates on the surface of the sample, but it is never contact with the sample. The scanning detector detects long-range forces such as van der Waals force or electrostatic forces that do not damage the imaged sample. d In the tapping mode the micro cantilever is subjected to stress vibration near its resonant frequency, and the oscillating needle tip gently strikes the surface of the sample, intermittently making contact with it
Fig. 4Imaging of cancer cell morphology and measuring the mechanical properties of cancer cells by AFM. a Representative AFM height image. b Representative AFM deflection image. c 3D distribution of cell height. The force curve is used to calculate mechanical properties. d Image representing Young’s modulus distribution. e Image representing adhesion force distribution. f Image representing stiffness distribution. Parameters are displayed as colors. The results of morphology observation and mechanical properties measurement of the cell were from our study group
Fig. 5Schematic diagram of AFM-based single-molecule force spectroscopy. a Individual antibodies or other molecules immobilized on a functionalized tip are positioned above a cell adhering to a substrate. b Sample and tip molecules are then brought into contact for a defined contact time and with a preset contact force. c The molecules are subsequently separated, and the maximal separation force and the detachment work can be determined using a simultaneously recorded force–distance curve. d The cantilever is retracted until the tip and sample molecules separate
Comparison of high-resolution imaging techniques in molecular and cell biology [171]
| Technique/feature | Atomic force microscopy | Super-resolution microscopy (STED, PALM, STORM) | Transmission electron microscopy | Scanning election microscopy |
|---|---|---|---|---|
| Resolution | ≤ 1 nm–50 nm | 20–50 nm | 0.2–10 nm | 2–10 nm |
| Sample preparation and environment | Sample on support; physiological (buffer solution, temperature, CO2) | Fluorescence labelling; physiological (buffer solution, temperature, CO2) | Sample on grid; dehydrated (negative stain); vitrified (cryo-electron microscopy) | Freeze/critical point drying and metal shadowing |
| Artefacts | Tip, force, scanning | Bleaching, toxicity | Dehydration, ice crystal formation, beam damage | Dehydration, metal shadowing, beam damage |
| Advantages | Imaging under native conditions; no staining, labelling, or fixation necessary; high signal-to-noise ratio; assessment of multiple physical, chemical, and biological parameters | Access to three-dimensional cellular structures; high spatiotemporal resolution; monitoring biomolecular processes in life cells | Solves atomic structures of proteins; conformational snapshot of proteins and complexes; molecular resolution of structures within the cell | Imaging surfaces of tissues, cells, and interfaces as nanometer-scale resolution |
| Limitation | Restricted to surfaces | Imaging restricted to fluorescence labels | No life processes | No life processes |
STED stimulated emission depletion, PALM photo activated localization microscopy, STORM stochastic optical reconstruction microscopy