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Schematic layout of a magnetic tweezers device with horn-shaped yokes. Letters represent different parameterized variables in the geometry. Table 
I
 lists each geometric parameter and indicates the effect of varying that parameter on the 




∇


x






B


⇀





. The line labeled Δx represents the contour along which the 






B


⇀





 values are tabulated. A sample would be placed normal to the distal end of this contour.

Schematic layout of a magnetic tweezers device with horn-shaped yokes. Letters represent different parameterized variables in the geometry. Table I lists each geometric parameter and indicates the effect of varying that parameter on the ∇ x B ⇀ . The line labeled Δx represents the contour along which the B ⇀ values are tabulated. A sample would be placed normal to the distal end of this contour.

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Article
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We present the design methodology for arrays of neodymium iron boron (NdFeB)-based magnets for use in magnetic tweezers devices. Using finite element analysis (FEA), we optimized the geometry of the NdFeB magnet as well as the geometry of iron yokes designed to focus the magnetic fields toward the sample plane. Together, the magnets and yokes form...

Contexts in source publication

Context 1
... understand the effects of magnet and yoke geometry on device performance, we parameterized every aspect of the magnet and yoke geometry, then systematically tested the effects of changing each parameter independently (Fig. 1). To qualitatively compare the various simulations, the magnitude of the ⇀ B field was plotted as a 2-D density plot, providing insight into how the magnet and yoke geometry influence the distribution of field lines around the device (for example, in Figs. 2(a)-2(c)). Additionally, quantitative values of the magnitude of the ⇀ B field ...
Context 2
... of field lines around the device (for example, in Figs. 2(a)-2(c)). Additionally, quantitative values of the magnitude of the ⇀ B field were plotted for a 1-cm long path extending from the midpoint between the tips of the magnetic tweezers device and extending away from the magnets into the area where a sample would be located (given by ∆x, as in Fig. 1). From these data, a figure of merit was developed to quantitatively compare the performance of each magnet and yoke configuration based on a linear fit to ⇀ B versus the magnet-sample separation distance ∆x (Fig. 1). The slope of the fitted line provides a locally averaged estimate of ∇ x ⇀ B , which in the limit of large magnetic ...
Context 3
... of the magnetic tweezers device and extending away from the magnets into the area where a sample would be located (given by ∆x, as in Fig. 1). From these data, a figure of merit was developed to quantitatively compare the performance of each magnet and yoke configuration based on a linear fit to ⇀ B versus the magnet-sample separation distance ∆x (Fig. 1). The slope of the fitted line provides a locally averaged estimate of ∇ x ⇀ B , which in the limit of large magnetic fields (when the bead magnetic moment saturates to a constant value) is directly proportional to the applied force. The calculation of ∇ x ⇀ B also provides an estimate of the distance over which the applied force ...

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... In this case, the magnetic field amplitude and gradient are determined by the specific magnetic material selection and array design, and the field values are fixed with respect to the magnet rest frame. 18,19 The field gradients, and thus forces, can be easily and robustly varied with respect to the specimen plane using motorized stages that change the separation distance between the magnet array and the sample. 20 Although the use of precision linear stages, rather than current control, significantly simplifies the design, eliminates the possibility of hysteretic responses, and removes the need for cooling and complex electronics, 17,21 it also introduces several implementation challenges, including the disruption of the light path, an inability to apply true step forces due to the finite translation time of the heavy magnets, and noise associated with the motion and settling of the magnet into position. ...
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