Volume 98, Issue 1, Pages (January 2010)

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Volume 98, Issue 1, Pages 57-66 (January 2010) Force Generation and Dynamics of Individual Cilia under External Loading  David B. Hill, Vinay Swaminathan, Ashley Estes, Jeremy Cribb, E. Timothy O'Brien, C. William Davis, R. Superfine  Biophysical Journal  Volume 98, Issue 1, Pages 57-66 (January 2010) DOI: 10.1016/j.bpj.2009.09.048 Copyright © 2010 Biophysical Society Terms and Conditions

Figure 1 (A) Schematic of the 3DFM in pole-flat configuration: (a) a pair of coverglasses separated by ∼200 μm; (b) one pole tip bent toward the substrate, the “flat” fixed on upper glass labeled a; and (c) cells grown on Millicell membrane. (B) Top-view image of the pole-flat, thin-film magnetics. (C) Bright-field image (40×, 0.6 NA objective, and 1.5 image magnifier) of a 2.8 μm magnetic bead (tracking cursor in place) attached to beating cilia in the 3DFM. The pole tip is clearly visible 12 μm away. The inserted images on the right-hand side are time-series images (0.083 ms apart) of a 1 μm bead bound to beating cilia. A 5 μm scale bar is shown. Biophysical Journal 2010 98, 57-66DOI: (10.1016/j.bpj.2009.09.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 2 Cilia beat pattern in the pulse experiments: (i) effective stroke in the direction of the bead (magnetic) force, and (ii) recovery stroke in the direction of the bead force. (A) Position versus time trace of 2.8 μm beads attached to a human bronchial epithelial cilium. The line at the base of the graph indicates force on/off. (B) CBA and CBF with and without the applied bead force. (C) Closer inspection of the cilia beat pattern with the force on (solid line) and off (dashed line) from panel A. The line is the bead's motion, the squares are the local maximums, and the triangles are the local minimums. The gray arrows indicate the effective stroke of the cilia, and the black arrows the recovery stroke. (D) Instantaneous maximum velocity of beating cilia for the tip position data in panel A. In all charts, the position/velocity scale is oriented to be in the direction of the external force. Biophysical Journal 2010 98, 57-66DOI: (10.1016/j.bpj.2009.09.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 3 Reduction of the CBA in force-ramp experiments. The gray line indicates the path of the bead, with squares indicating the local maximum and triangles the local minimum. The line at the bottom of the figure shows the magnetic driving current; the bead force is shown on a separate horizontal axis. Using our model, the point at which the bead force is sufficient to limit the minimum excursion of the bead to be the midpoint of the baseline motion is defined as the motor force. The position scale is oriented to be in the direction of the external force. Biophysical Journal 2010 98, 57-66DOI: (10.1016/j.bpj.2009.09.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 4 Effect of external force (FB) on the CBA. Cilia beating with their effective stroke in the direction of the bead force are represented by squares (n = 9), and cilia beating with their recovery stroke in the direction of the bead force are shown with diamonds (n = 6). Solid data points are from pulse-type experiments, and open points are from force-ramp experiments. Data from the same ramp are connected with a dotted line. Biophysical Journal 2010 98, 57-66DOI: (10.1016/j.bpj.2009.09.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 5 Axoneme spring constant fit to data. Data points (diamonds) are the local minimums from Fig. 3, and the black squares are the pulse data (n = 9). The data have been replotted such that the applied force (i.e., the sum of the external force FB, and the effective motor force, FM) fall at 0,0. The line is from the nonlinear model with parameters determined by fit to the complete cilia data set of Fig. 4, which is in good agreement with the data. Inset: Schematic of a one-dimensional model for the axoneme with force FB applied to the bead attached to the tip. The axoneme is represented as a nonlinear spring KA that applies a restoring force FA, and an internal force Fm generated by an internal spring Km extended by a system of stepping motors. Biophysical Journal 2010 98, 57-66DOI: (10.1016/j.bpj.2009.09.048) Copyright © 2010 Biophysical Society Terms and Conditions