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Four misalignment coil conditions. (A) Perfectly aligned coil; (B) lateral coil misalignment; (C) angular coil misalignments; (D) general coil misalignments. 

Four misalignment coil conditions. (A) Perfectly aligned coil; (B) lateral coil misalignment; (C) angular coil misalignments; (D) general coil misalignments. 

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Article
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Abstract Use of transcutaneous inductive links is a widely known method for the wireless powering of bio-implanted devices such as implanted microsystems. The design of the coil for inductive links is generally not optimal. In this study, inductive links were used on the basis of the small loop antenna theory to reduce the effects of lateral coil m...

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... analytical and empirical methods are mathematically investigated to address coil misalignment on the basis of the assumption that the coils are separated by air. Four coil misalignment condi- tions, namely, aligned case, lateral misalignment case, angular coil misalignments, and general case, have been well studied theoretically and mathematically as shown in Figure 1 [1,12,14]. ...
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... the lateral misalignment case, the mutual inductance between the two coils is derived from (a, b, d, Δ) and other partial derivatives. Our proposed inductive coil radius dimensions are a = 28 mm, b = 5.8 mm, d = 5 mm, and variable Δ. Figure 1B shows that both coils are in paral- lel planes, but their centers moved a side by Δ distance. The value of Δ was changed parametrically to the X-axis or Y-axis from > 0 to 4 mm, and this value was smaller than the radius of the implanted coil. ...
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... slight drop in the gain at some specific angles can be observed. Figure 10 shows the E-Total gain in the near field when the azimuthal plane θ = 90° was very stable and had a value that ranged from 24.35 to 25.35 dB depending on lateral misalignments. The radiation around the coil was omnidirectional, and there was a very slight drop at angle 150°. ...
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... loss is negligible. Figure 11 shows an accurate presentation of results. In the two-dimensional (2D) simulated radiation pat- terns of the total near field in the elevation plane when Φ = 90°, the gain ranged from 37.65 to 38.30 dB, and for the azimuthal plane when θ = 90°, the gain ranged from 24.35 to 25.35 dB. ...
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... same scenario presented in Figure 8 was achieved with the use of dry skin as shown in Figure 12. The lateral misalignment distance between the reader and the implanted coil was smaller than the radius of the implanted coil (Δ < b). ...
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... these results with those obtained when coil alignment Δ = 0 given in Figure 7, coil performance was not affected by lateral misalignments although dry tissue separated the coils. Figure 13 shows the E-Total gain simulated with para- metric lateral misalignment moving from 0 to 8 mm by 25 2-mm steps. The E-Total gain in near field when the eleva- tion plane Φ = 90° was 37-38 dB, with slight drops in gain in some specific angles. ...
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... E-Total gain in near field when the eleva- tion plane Φ = 90° was 37-38 dB, with slight drops in gain in some specific angles. Figure 14 shows that the E-Total gain in the near-field when the azimuthal plane θ = 90° was simulated was from 24.35 to 24.70 dB. A slight drop in angle 150° and a very slight drop in angles 290°-320° were observed. ...
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... the loss in gain when the lateral misalignment was from Δ = 0 mm to Δ = 8 mm was < -1 dB, which is negligible. Accurate results are shown in Figure 15. In the 2D simulated radiation pattern, the gain in the elevation plane when Φ = 90° was up to 38 dB, and the gain in the azimuthal plane when θ = 90° was 24.35-24.70 ...

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Citations

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