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Lin et al. Soft Sci 2023;3:14  https://dx.doi.org/10.20517/ss.2023.05            Page 9 of 25

               material, weight ratio, and magnetization direction of the magnetic micro/nanoparticles serves as an
               effective approach to adjusting the tunable elastic and magnetic properties of the composites [114,115] .

               Figure 3A illustrates a soft electronic system based on magnetic composites. The system consists of
               magnetic microparticles (neodymium iron boron (NdFeB), average particle radius: ~5.00 μm; remanence:
               92.3 emu g ; coercive magnetic field: 6375 Oe) and a porous silicone rubber matrix. The embedded
                         –1
               ferromagnetic particles enable the system to convert mechanical deformations into electricity using coils.
               Compared with systems that mix the iron micro/nanoparticles with silicone rubber, the example shown in
               Figure 3A can generate electric signals in the absence of external magnetic fields, which simplifies the device
               configuration [116,117] .


               In the process of heating the mixture of uncured silicone rubber and micro/nanomagnets, an option is to
               introduce air bubbles to form porous composites. Such porous structures not only reduce the modulus, but
               also provide tiny spaces for the micro/nanomagnets to reorientate and move during impulse magnetization,
               eventually forming a chain-like arrangement of the micromagnets associated with the giant magnetoelastic
               effect. Compared with the traditional magnetoelastic effect arising from magnetic domain rearrangement
               and stress-induced magnetic anisotropy under external magnetic field, this giant magnetoelastic effect is
               attributed to the change of micro-magnetic chain structure under mechanical deformation. As shown in the
               right frame of Figure 3A, compression changes the chain structure of the magnet, causing a decrease in
               surface magnetic flux density. The soft system can withstand a tensile strain of up to 190%, and
               demonstrates much lower modulus (at the level of 100 kPa,) compared with conventional magnetic alloy
                                              [118]
               (modulus at the level of 10 GPa) . Such features enhance the biomechanical-to-magnetic energy
               conversion and open many potential applications in soft electronics, including wearable/implantable energy
               harvesters, and stretchable biomedical sensors for continuous monitoring of human pulse waves and heart
               rhythms .
                      [119]
               Another advantage of magnetic composites is that the direction of magnetization can be programmed in a
               heterogeneous manner, as the composite materials are soft enough to be folded, wrapped, or otherwise
               deformed into 3D geometries during magnetization [120,121] . In particular, magnetizing a flexible magnetic film
               with a sinusoidal pattern enables high spatial resolution and the capability to decouple different mechanical
                                [122]
               stimuli [Figure 3B] . The soft tactile sensor involves a soft magnetic composite (modulus: ~2 MPa;
               thickness: 0.5 mm) formed by mixing polydimethylsiloxane (PDMS) and NdFeB magnetic powders with a
               weight ratio of 1:3, a silicone elastomer layer (Ecoflex 00-50, modulus: ~83 kPa), and a commercial Hall
               sensor [left frame of Figure 3B]. The soft magnetic composite deforms under external force and causes a
               change in magnetic flux density, which can be detected by the Hall sensor embedded in the silicone
               elastomer [right frame of Figure 3B]. Here, the sinusoidal pattern (obtained by wrapping the soft magnetic
               composite on a cylinder during magnetization) is crucial for decoupling and super-resolution. On the one
               hand, the magnetic field distribution caused by the sinusoidal pattern is decoupled into two mutually
               orthogonal planes: the magnetic strength B and the magnetic ratio R . The B plane determines the normal
                                                                          B
               force related to the magnetic field rotation angle (or displacement along the z-axis), while the R  plane
                                                                                                    B
               measures the shear force related to the translational movement of the magnetic field (displacement d along
               the x-axis). The capability to decouple various mechanical stimuli overcomes the inherent problem of the
               strong cross-coupling effects in conventional magnetic tactile sensors [123-125] . On the other hand, extending
               the sinusoidal patterns to the form of sensor arrays allows for tactile sensing with super-resolution and
               across large areas. Combined with deep learning algorithm, the sensors can achieve a 60-fold improvement
               in localization (from 6 to 0.1 mm).
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