Cell stiffness measurement by atomic force microscopy

XC Xi Chen
ZX Zichen Xu
KT Kai Tang
GH Guanshuo Hu
PD Pengyu Du
JW Junfang Wang
CZ Cunyu Zhang
YX Ying Xin
KL Keming Li
QZ Qiantang Zhang
JH Jianjun Hu
ZZ Zhuxue Zhang
MY Mo Yang
GW Guixue Wang
YT Youhua Tan
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An atomic force microscope (AFM; Bruker Catalyst) combined with an inverted optical microscope (Nikon) was used to measure cell stiffness. The silicon nitride cantilevers with a spring constant k of 0.02 to 0.08 N/m and tip radius of 20 nm were chosen to probe the cells in a 60-mm dish for the experiment at room temperature. The scan size for all measurements was set to 0 to maintain a constant position over a cell, and the tip was brought into contact with the cell at the indicated regions. The force–indentation curves were recorded at 1 Hz to estimate the cell stiffness. For each cell, the force–indentation curves were obtained from at least 5 different cellular locations and the averaged value was used to represent the stiffness for this cell. The force F between the tip and the cell was the product of the cantilever deflection δ and k, i.e., F = k × δ. The Young’s modulus E could be calculated by fitting the force–indentation curves with Hertzian model for a pyramidal tip, i.e., F = 2/π × tan(α) × E/(1 − v2) × d2, where α is the half tip angle, the Poisson's ratio v is set to 0.5, and d is the indentation depth. d was kept within 500 nm at 1 Hz to avoid potential substrate effects and cell damage.

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