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	<title>Near Field Electromagnetics - Revision history</title>
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		<title>JonoThora: Psionics expansion (01a + 01b): content authored / LaTeX-restored per local submodule; lint-clean.</title>
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		<updated>2026-05-11T20:51:02Z</updated>

		<summary type="html">&lt;p&gt;Psionics expansion (01a + 01b): content authored / LaTeX-restored per local submodule; lint-clean.&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Near-Field Electromagnetics =&lt;br /&gt;
&lt;br /&gt;
{{Audience_Sidebar&lt;br /&gt;
| difficulty   = Intermediate&lt;br /&gt;
| reading_time = 7 minutes&lt;br /&gt;
| prerequisites = Maxwell&amp;#039;s equations; basic antenna concepts; wavelength and frequency.&lt;br /&gt;
| if_too_advanced_see = [[Psionic_Device_Overview]]&lt;br /&gt;
| if_you_want_the_math_see = This page; [[Reactive_Near_Field]]; [[Antenna_Theory_for_Psionic_Devices]]&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
{{Notation&lt;br /&gt;
| signature = Non-relativistic; SI units throughout.&lt;br /&gt;
| units     = E (V/m); H (A/m); B (T); λ (m); D = largest antenna dimension (m); k = 2π/λ.&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Near-field electromagnetics&amp;#039;&amp;#039;&amp;#039; is the branch of electromagnetic theory concerned with the fields near an antenna or radiating element — distances comparable to or smaller than a wavelength. In contrast to &amp;#039;&amp;#039;&amp;#039;far-field&amp;#039;&amp;#039;&amp;#039; (radiation-zone) behaviour, near-field fields exhibit:&lt;br /&gt;
&lt;br /&gt;
* Strong stored (non-radiated) energy.&lt;br /&gt;
* E and H mutually out of phase.&lt;br /&gt;
* Faster than r&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt; spatial decay (r&amp;lt;sup&amp;gt;−2&amp;lt;/sup&amp;gt;, r&amp;lt;sup&amp;gt;−3&amp;lt;/sup&amp;gt; terms).&lt;br /&gt;
* Direct inductive/capacitive coupling to nearby matter.&lt;br /&gt;
&lt;br /&gt;
These properties make the near field the operational regime for [[Psionic_Device_Overview|psionic devices]] such as [[HelmKit]] — devices that must couple strongly to nearby biological tissue (a few cm distant) while minimising far-field radiative exposure.&lt;br /&gt;
&lt;br /&gt;
== Field-zone boundaries ==&lt;br /&gt;
&lt;br /&gt;
For an antenna of largest dimension D operating at wavelength λ = c / f, the EM field is conventionally divided into three zones:&lt;br /&gt;
&lt;br /&gt;
| Zone | Range | Field character | Energy state |&lt;br /&gt;
|---|---|---|---|&lt;br /&gt;
| Reactive near-field | 0 &amp;lt; r &amp;lt; 0.62·√(D&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;/λ) | E and H ~90° out of phase; r&amp;lt;sup&amp;gt;−3&amp;lt;/sup&amp;gt; behavior | Stored |&lt;br /&gt;
| Radiating near-field (Fresnel) | 0.62·√(D&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;/λ) ≤ r &amp;lt; 2D&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/λ | E and H phase-aligning; r&amp;lt;sup&amp;gt;−2&amp;lt;/sup&amp;gt; | Mix |&lt;br /&gt;
| Far-field (Fraunhofer) | r ≥ 2D&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/λ | E ⊥ H ⊥ propagation; plane wave; r&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt; | Radiated |&lt;br /&gt;
&lt;br /&gt;
The transition wavelength-distance r = 2D&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/λ defines the boundary at which the antenna&amp;#039;s emitted wave can be treated as a plane wave — the standard far-field idealisation.&lt;br /&gt;
&lt;br /&gt;
== Worked examples at 2.45 GHz ==&lt;br /&gt;
&lt;br /&gt;
The 2.45 GHz ISM band is the standard operating frequency for many [[HelmKit]]-class devices (chosen because of regulatory allowance and the availability of standard hardware).&lt;br /&gt;
&lt;br /&gt;
At f = 2.45 GHz: λ = c/f = 0.1224 m = 12.24 cm.&lt;br /&gt;
&lt;br /&gt;
=== D = 5 cm coil (HelmKit-typical) ===&lt;br /&gt;
&lt;br /&gt;
* Reactive boundary: 0.62 · √(0.05&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;/0.1224) ≈ 6.3 cm.&lt;br /&gt;
* Fresnel boundary: 2 · 0.05&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/0.1224 ≈ 4.1 cm.&lt;br /&gt;
&lt;br /&gt;
The Fresnel boundary is &amp;#039;&amp;#039;&amp;#039;smaller&amp;#039;&amp;#039;&amp;#039; than the reactive boundary — a sign that the antenna is &amp;#039;&amp;#039;&amp;#039;electrically small&amp;#039;&amp;#039;&amp;#039; (D ≪ λ) and the standard boundary formulas no longer cleanly separate the zones. Essentially the entire local field is reactive.&lt;br /&gt;
&lt;br /&gt;
=== D = 10 cm coil ===&lt;br /&gt;
&lt;br /&gt;
* Reactive: ~ 5.6 cm.&lt;br /&gt;
* Fresnel: ~ 16.3 cm.&lt;br /&gt;
* Far-field begins at r ≈ 16 cm.&lt;br /&gt;
&lt;br /&gt;
=== D = 50 cm dish ===&lt;br /&gt;
&lt;br /&gt;
* Reactive: ~ 63 cm.&lt;br /&gt;
* Fresnel: ~ 4.1 m.&lt;br /&gt;
* Far-field begins at r ≈ 4 m — a real beam emerges at this scale.&lt;br /&gt;
&lt;br /&gt;
== Why the reactive zone matters ==&lt;br /&gt;
&lt;br /&gt;
The reactive near-field is where:&lt;br /&gt;
&lt;br /&gt;
# &amp;#039;&amp;#039;&amp;#039;Inductive/capacitive coupling&amp;#039;&amp;#039;&amp;#039; to nearby matter is strongest. For a coil near a brain, the coil&amp;#039;s stored magnetic energy couples directly into the brain tissue via mutual inductance.&lt;br /&gt;
# &amp;#039;&amp;#039;&amp;#039;EM energy is stored, not radiated&amp;#039;&amp;#039;&amp;#039;. High field amplitudes can be achieved per unit input power. A 100 mW source can produce locally large E-fields without significant radiated power.&lt;br /&gt;
# &amp;#039;&amp;#039;&amp;#039;Field can be spatially shaped&amp;#039;&amp;#039;&amp;#039; with higher precision than the diffraction-limited far-field. Sub-wavelength field structures are easily made in the reactive zone.&lt;br /&gt;
&lt;br /&gt;
For psionic-device design, &amp;#039;&amp;#039;&amp;#039;operate in the reactive zone&amp;#039;&amp;#039;&amp;#039; to maximise coupling to biological tissue while minimising radiative loss and far-field exposure (which would otherwise expand the regulatory compliance burden).&lt;br /&gt;
&lt;br /&gt;
== Electrically small antennas ==&lt;br /&gt;
&lt;br /&gt;
When D ≪ λ — the regime of compact wearable devices — the antenna is &amp;#039;&amp;#039;&amp;#039;electrically small&amp;#039;&amp;#039;&amp;#039; and obeys different scaling laws. See [[Antenna_Theory_for_Psionic_Devices]] for the Chu-Harrington bound, Wheeler radiation resistance, and related limits.&lt;br /&gt;
&lt;br /&gt;
For a 5 cm coil at 2.45 GHz (ka ≈ 1.28), the antenna sits at the boundary between electrically small and resonant. For deeper near-field operation, lower the operating frequency to ~ 300-500 MHz (or larger coils at 2.45 GHz).&lt;br /&gt;
&lt;br /&gt;
== Coupling to ψ in the near field ==&lt;br /&gt;
&lt;br /&gt;
In the [[Psionics|framework]]:&lt;br /&gt;
&lt;br /&gt;
* The ψ-source J&amp;lt;sub&amp;gt;ψ&amp;lt;/sub&amp;gt; = α F&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt;F&amp;lt;sup&amp;gt;μν&amp;lt;/sup&amp;gt; is proportional to E&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; − c&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;B&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; locally.&lt;br /&gt;
* In the reactive near-field, both E and B are large; their product F&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt;F&amp;lt;sup&amp;gt;μν&amp;lt;/sup&amp;gt; ≠ 0.&lt;br /&gt;
* Per-volume ψ-source density can exceed far-field by &amp;#039;&amp;#039;&amp;#039;factors of 10&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;-10&amp;lt;sup&amp;gt;4&amp;lt;/sup&amp;gt;&amp;#039;&amp;#039;&amp;#039; at typical near-field amplitudes.&lt;br /&gt;
* This is the rationale for near-field operation of psionic devices: high-efficiency ψ-source per watt of input power.&lt;br /&gt;
&lt;br /&gt;
== Safety ==&lt;br /&gt;
&lt;br /&gt;
The reactive near-field is also the regime of highest [[Psionic_Device_Safety|biological exposure risk]]. See [[SAR_Calculation_for_Psionic_Devices]] for the ICNIRP/IEEE compliance framework: the localised SAR limit (2.0 W/kg over 10 g of head tissue) demands strict control of near-field E-amplitudes.&lt;br /&gt;
&lt;br /&gt;
== Sanity checks ==&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;r ≫ 2D&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/λ&amp;#039;&amp;#039;&amp;#039; → recovers standard far-field plane-wave radiation. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Static limit (f → 0)&amp;#039;&amp;#039;&amp;#039; → reactive near-field becomes pure inductive/electrostatic. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;ψ → 0&amp;#039;&amp;#039;&amp;#039; (in framework) → standard near-field EM intact; no ψ-coupling. ✓ ([[Sanity_Check_Limits]] §6.)&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[Reactive_Near_Field]]&lt;br /&gt;
* [[Antenna_Theory_for_Psionic_Devices]]&lt;br /&gt;
* [[Caduceus_Coil]]&lt;br /&gt;
* [[Bifilar_Coil]]&lt;br /&gt;
* [[Double-Helix_Antenna]]&lt;br /&gt;
* [[Psionic_Device_Overview]]&lt;br /&gt;
* [[HelmKit]]&lt;br /&gt;
* [[Psionic_Device_Safety]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Balanis, C. A. (2016). &amp;#039;&amp;#039;Antenna Theory: Analysis and Design.&amp;#039;&amp;#039; 4th ed., Wiley.&lt;br /&gt;
* Pozar, D. M. (2011). &amp;#039;&amp;#039;Microwave Engineering.&amp;#039;&amp;#039; 4th ed., Wiley.&lt;br /&gt;
* Kraus, J. D. (1988). &amp;#039;&amp;#039;Antennas.&amp;#039;&amp;#039; 2nd ed., McGraw-Hill.&lt;br /&gt;
&lt;br /&gt;
[[Category:Psionics]]&lt;br /&gt;
[[Category:Electromagnetism]]&lt;br /&gt;
[[Category:Antenna Theory]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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