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	<id>https://wiki.fusiongirl.app:443/index.php?action=history&amp;feed=atom&amp;title=Woodward_Effect</id>
	<title>Woodward Effect - Revision history</title>
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		<id>https://wiki.fusiongirl.app:443/index.php?title=Woodward_Effect&amp;diff=6196&amp;oldid=prev</id>
		<title>JonoThora: Create Woodward Effect — Mach principle mass fluctuation, MEGA drive, PZT implementation, experimental status, NASA NIAC</title>
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		<updated>2026-03-14T06:16:42Z</updated>

		<summary type="html">&lt;p&gt;Create Woodward Effect — Mach principle mass fluctuation, MEGA drive, PZT implementation, experimental status, NASA NIAC&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Infobox&lt;br /&gt;
| title      = Woodward Effect&lt;br /&gt;
| image      =&lt;br /&gt;
| caption    = Mach-principle transient mass fluctuation for propellantless propulsion&lt;br /&gt;
| header1    = Overview&lt;br /&gt;
| label2     = Discoverer&lt;br /&gt;
| data2      = James F. Woodward (Cal State Fullerton)&lt;br /&gt;
| label3     = Theoretical Basis&lt;br /&gt;
| data3      = Mach&amp;#039;s Principle + relativistic scalar gravitational field equation&lt;br /&gt;
| label4     = Key Equation&lt;br /&gt;
| data4      = δm ∝ −(1/Gρc²)·dP/dt&lt;br /&gt;
| label5     = Implementation&lt;br /&gt;
| data5      = MEGA drive — piezoelectric (PZT) stack capacitor, 20–100 kHz&lt;br /&gt;
| label6     = Measured Thrust&lt;br /&gt;
| data6      = ~1–10 µN (at edge of measurement capability)&lt;br /&gt;
| label7     = Funding&lt;br /&gt;
| data7      = NASA NIAC, Space Studies Institute (SSI)&lt;br /&gt;
| label8     = Status&lt;br /&gt;
| data8      = Peer-reviewed theory · Marginal experimental evidence · No independent replication&lt;br /&gt;
| below      = &amp;#039;&amp;#039;The only propellantless thrust concept with both a published GR derivation and NASA funding&amp;#039;&amp;#039;&lt;br /&gt;
}}&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
| ⚡️ || [[Electrogravitics]] - [[Electrogravitic Tech]] || [[Electrokinetics]] - [[Electrokinetic Tech]]&lt;br /&gt;
|-&lt;br /&gt;
| 🧲 || [[Magnetogravitics]] - [[Magnetogravitic Tech]] || [[Magnetokinetics]] - [[Magnetokinetic Tech]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;Woodward effect&amp;#039;&amp;#039;&amp;#039; (also called the &amp;#039;&amp;#039;&amp;#039;Mach effect&amp;#039;&amp;#039;&amp;#039; or &amp;#039;&amp;#039;&amp;#039;Mach effect thrust&amp;#039;&amp;#039;&amp;#039;) is a predicted transient fluctuation in the inertial mass of an accelerating body whose internal energy is changing. Derived from &amp;#039;&amp;#039;&amp;#039;Mach&amp;#039;s principle&amp;#039;&amp;#039;&amp;#039; and general relativity by physicist &amp;#039;&amp;#039;&amp;#039;James F. Woodward&amp;#039;&amp;#039;&amp;#039; (California State University, Fullerton), it predicts that a properly configured piezoelectric device can generate net &amp;#039;&amp;#039;&amp;#039;propellantless thrust&amp;#039;&amp;#039;&amp;#039; by exploiting these mass fluctuations.&lt;br /&gt;
&lt;br /&gt;
If confirmed, the Woodward effect would enable deep-space propulsion without exhaust — a &amp;quot;propellantless drive&amp;quot; with effectively infinite specific impulse. Current experimental signals are ~1–10 µN (micronewtons), at the edge of measurement capability, and have not been independently replicated at high confidence.&lt;br /&gt;
&lt;br /&gt;
== Theoretical Derivation ==&lt;br /&gt;
&lt;br /&gt;
=== Mach&amp;#039;s Principle ===&lt;br /&gt;
&lt;br /&gt;
The theoretical foundation rests on &amp;#039;&amp;#039;&amp;#039;Mach&amp;#039;s principle&amp;#039;&amp;#039;&amp;#039;: the inertial mass of any body is determined by its gravitational interaction with &amp;#039;&amp;#039;&amp;#039;all other mass in the observable universe&amp;#039;&amp;#039;&amp;#039;. In the Sciama-Woodward formulation: &amp;lt;ref&amp;gt;Sciama, D.W. (1953). &amp;quot;On the Origin of Inertia.&amp;quot; &amp;#039;&amp;#039;Monthly Notices of the Royal Astronomical Society&amp;#039;&amp;#039; 113(1), 34–42. doi:10.1093/mnras/113.1.34&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\Phi = \frac{GM_U}{R_U c^2} \approx 1&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;M_U&amp;lt;/math&amp;gt; is the total mass of the observable universe and &amp;lt;math&amp;gt;R_U&amp;lt;/math&amp;gt; is the Hubble radius. The approximate equality to 1 (in appropriate units) is Mach&amp;#039;s principle — inertia &amp;#039;&amp;#039;&amp;#039;is&amp;#039;&amp;#039;&amp;#039; gravitational interaction with distant matter.&lt;br /&gt;
&lt;br /&gt;
=== The Mass Fluctuation Equation ===&lt;br /&gt;
&lt;br /&gt;
Starting from the relativistic scalar gravitational field equation and applying energy-momentum conservation, Woodward derives: &amp;lt;ref&amp;gt;Woodward, J.F. (1990). &amp;quot;A new experimental approach to Mach&amp;#039;s principle and relativistic gravitation.&amp;quot; &amp;#039;&amp;#039;Foundations of Physics Letters&amp;#039;&amp;#039; 3(5), 497–506. doi:10.1007/BF00665932&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;Woodward, J.F. (1991). &amp;quot;Measurements of a Machian transient mass fluctuation.&amp;quot; &amp;#039;&amp;#039;Foundations of Physics Letters&amp;#039;&amp;#039; 4(5), 407–423. doi:10.1007/BF00689887&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\delta m(t) = -\frac{1}{4\pi G \rho c^2} \frac{\partial^2 E_0}{\partial t^2} + \frac{1}{16\pi G \rho c^4}\left(\frac{\partial E_0}{\partial t}\right)^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where:&lt;br /&gt;
* &amp;lt;math&amp;gt;E_0&amp;lt;/math&amp;gt; = rest energy of the body&lt;br /&gt;
* &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; = local mass density&lt;br /&gt;
* &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; = Newton&amp;#039;s gravitational constant&lt;br /&gt;
* &amp;lt;math&amp;gt;c&amp;lt;/math&amp;gt; = speed of light&lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;E_0 = m_0 c^2&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;P = dE_0/dt&amp;lt;/math&amp;gt; (power), this becomes:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\delta m(t) = -\frac{1}{4\pi G \rho c^2} \frac{dP}{dt} + \frac{1}{16\pi G \rho c^4} P^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Physical Interpretation ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ The Two Mass Fluctuation Terms&lt;br /&gt;
|-&lt;br /&gt;
! Term !! Expression !! Character !! Magnitude&lt;br /&gt;
|-&lt;br /&gt;
| &amp;#039;&amp;#039;&amp;#039;First (dominant)&amp;#039;&amp;#039;&amp;#039; || &amp;lt;math&amp;gt;-\frac{1}{4\pi G \rho c^2} \frac{dP}{dt}&amp;lt;/math&amp;gt; || Oscillatory — mass fluctuates with dP/dt || Primary effect&lt;br /&gt;
|-&lt;br /&gt;
| &amp;#039;&amp;#039;&amp;#039;Second (DC)&amp;#039;&amp;#039;&amp;#039; || &amp;lt;math&amp;gt;+\frac{1}{16\pi G \rho c^4} P^2&amp;lt;/math&amp;gt; || Always positive — permanent mass increase || Suppressed by &amp;lt;math&amp;gt;c^4&amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The first term says: &amp;#039;&amp;#039;&amp;#039;the inertial mass of an object fluctuates in proportion to the time derivative of the power being delivered to it&amp;#039;&amp;#039;&amp;#039;. If you rapidly pulse energy into an object while simultaneously accelerating it, the acceleration acts on a time-varying mass — and the time-averaged force is non-zero.&lt;br /&gt;
&lt;br /&gt;
== The MEGA Drive ==&lt;br /&gt;
&lt;br /&gt;
=== Operating Principle ===&lt;br /&gt;
&lt;br /&gt;
MEGA = &amp;#039;&amp;#039;&amp;#039;Mach Effect Gravitational Assist&amp;#039;&amp;#039;&amp;#039; (Woodward&amp;#039;s preferred term).&lt;br /&gt;
&lt;br /&gt;
The practical implementation uses a &amp;#039;&amp;#039;&amp;#039;piezoelectric (PZT) stack&amp;#039;&amp;#039;&amp;#039;:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ MEGA Drive Design&lt;br /&gt;
|-&lt;br /&gt;
! Component !! Function&lt;br /&gt;
|-&lt;br /&gt;
| PZT stack || Lead zirconate titanate capacitor — converts electrical energy to mechanical strain&lt;br /&gt;
|-&lt;br /&gt;
| AC drive || High-frequency voltage oscillation (20–100 kHz) → energy fluctuation → mass fluctuation&lt;br /&gt;
|-&lt;br /&gt;
| DC bias / reaction mass || Provides steady acceleration of the stack against a reaction mass&lt;br /&gt;
|-&lt;br /&gt;
| Phase controller || Synchronizes AC mass fluctuation with DC acceleration for net thrust&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Thrust Generation ===&lt;br /&gt;
&lt;br /&gt;
For a PZT capacitor driven at angular frequency &amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt; with peak voltage &amp;lt;math&amp;gt;V_0&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
# AC power input: &amp;lt;math&amp;gt;P(t) = C V_0^2 \omega \cos(\omega t) \sin(\omega t)&amp;lt;/math&amp;gt;&lt;br /&gt;
# Mass fluctuation: &amp;lt;math&amp;gt;\delta m \propto dP/dt \propto \omega^2 C V_0^2 \cos(2\omega t)&amp;lt;/math&amp;gt;&lt;br /&gt;
# DC acceleration &amp;lt;math&amp;gt;a_0&amp;lt;/math&amp;gt; acts on the fluctuating mass&lt;br /&gt;
# Net time-averaged thrust:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\langle F \rangle \propto \frac{\omega^2 C V_0^2 a_0}{G \rho c^2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Key scaling:&lt;br /&gt;
* Thrust scales as &amp;#039;&amp;#039;&amp;#039;ω²&amp;#039;&amp;#039;&amp;#039; — higher frequency = more thrust&lt;br /&gt;
* Thrust scales as &amp;#039;&amp;#039;&amp;#039;V₀²&amp;#039;&amp;#039;&amp;#039; — higher voltage = more thrust&lt;br /&gt;
* Thrust scales as &amp;#039;&amp;#039;&amp;#039;a₀&amp;#039;&amp;#039;&amp;#039; — stronger DC acceleration = more thrust&lt;br /&gt;
* Denominator contains &amp;lt;math&amp;gt;Gc^2&amp;lt;/math&amp;gt; — extremely small, which is why the effect is tiny&lt;br /&gt;
&lt;br /&gt;
== Experimental Results ==&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Woodward&amp;#039;s Experimental Campaign&lt;br /&gt;
|-&lt;br /&gt;
! Period !! Setup !! Result !! Notes&lt;br /&gt;
|-&lt;br /&gt;
| 1990–2000 || PZT stacks on torsion balance || ~µN signals detected || Multiple configurations tested&lt;br /&gt;
|-&lt;br /&gt;
| 2000–2010 || Improved PZT stacks, vacuum chamber || ~1–10 µN at 20–40 kHz || Consistent with ω² scaling&lt;br /&gt;
|-&lt;br /&gt;
| 2010–2015 || Heavier PZT stacks, better isolation || Similar magnitude || Thermal/vibrational artifacts investigated&lt;br /&gt;
|-&lt;br /&gt;
| 2015–present || MEGA prototypes; SSI-funded || Ongoing || Scaling behavior partially confirmed&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Experimental Challenges ===&lt;br /&gt;
&lt;br /&gt;
The signals are extraordinarily small and plagued by systematics:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Systematic Error Sources&lt;br /&gt;
|-&lt;br /&gt;
! Source !! Mechanism !! Mitigation&lt;br /&gt;
|-&lt;br /&gt;
| Thermal expansion || PZT heating → mechanical displacement || Thermal compensation; duty-cycle control&lt;br /&gt;
|-&lt;br /&gt;
| Vibration coupling || PZT stack vibrates → mechanical coupling to balance || Vibration isolation; frequency modulation&lt;br /&gt;
|-&lt;br /&gt;
| EM interference || AC drive creates stray EM fields || Faraday cage; twisted-pair leads&lt;br /&gt;
|-&lt;br /&gt;
| Acoustic coupling || Audible/ultrasonic radiation from PZT || Vacuum operation; acoustic baffles&lt;br /&gt;
|-&lt;br /&gt;
| Center-of-mass shift || Internal mass redistribution mimics thrust || Measure with accelerometers; reverse orientation&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Independent Replication ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Replication Attempts&lt;br /&gt;
|-&lt;br /&gt;
! Group !! Year !! Result&lt;br /&gt;
|-&lt;br /&gt;
| Cramer et al. (U. Washington) || 2004 || Null result — but used different configuration&lt;br /&gt;
|-&lt;br /&gt;
| March &amp;amp; Palfreyman (PlasmaLinx) || 2006 || Possible signal — inconclusive&lt;br /&gt;
|-&lt;br /&gt;
| Tajmar &amp;amp; Fiedler (TU Dresden) || 2015 || Measured signals, but attributed to thermal artifact &amp;lt;ref&amp;gt;Tajmar, M. &amp;amp; Fiedler, G. (2015). &amp;quot;Direct Thrust Measurements of an EMDrive and Evaluation of Possible Side-Effects.&amp;quot; &amp;#039;&amp;#039;AIAA 2015-4083&amp;#039;&amp;#039;.&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| Fearn et al. (CSU Fullerton) || 2015 || Supportive theoretical analysis &amp;lt;ref&amp;gt;Fearn, H., Woodward, J.F. &amp;amp; van Rossum, N. (2015). &amp;quot;Theory of a Mach Effect Thruster.&amp;quot; &amp;#039;&amp;#039;J. Modern Physics&amp;#039;&amp;#039; 6, 1868–1880. doi:10.4236/jmp.2015.613192&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
No independent group has confirmed the effect at high statistical significance.&lt;br /&gt;
&lt;br /&gt;
== Relationship to General Relativity ==&lt;br /&gt;
&lt;br /&gt;
The Woodward effect&amp;#039;s theoretical status is debated:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Theoretical Assessment&lt;br /&gt;
|-&lt;br /&gt;
! Aspect !! Status&lt;br /&gt;
|-&lt;br /&gt;
| Derivation from GR || &amp;#039;&amp;#039;&amp;#039;Plausible&amp;#039;&amp;#039;&amp;#039; — follows from scalar gravitational field equation + Mach&amp;#039;s principle&lt;br /&gt;
|-&lt;br /&gt;
| Mach&amp;#039;s principle in GR || &amp;#039;&amp;#039;&amp;#039;Debated&amp;#039;&amp;#039;&amp;#039; — GR is compatible with Mach&amp;#039;s principle but does not require it&lt;br /&gt;
|-&lt;br /&gt;
| Mathematical consistency || &amp;#039;&amp;#039;&amp;#039;Questioned&amp;#039;&amp;#039;&amp;#039; — some physicists argue the derivation improperly manipulates field equations&lt;br /&gt;
|-&lt;br /&gt;
| Thermodynamic consistency || &amp;#039;&amp;#039;&amp;#039;Questioned&amp;#039;&amp;#039;&amp;#039; — net thrust from internal energy changes potentially violates conservation laws&lt;br /&gt;
|-&lt;br /&gt;
| Lorentz invariance || &amp;#039;&amp;#039;&amp;#039;Compatible&amp;#039;&amp;#039;&amp;#039; — the derivation is explicitly relativistic&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Connection to Other Frameworks ==&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Cross-Theory Comparison&lt;br /&gt;
|-&lt;br /&gt;
! Framework !! Woodward Effect Relationship&lt;br /&gt;
|-&lt;br /&gt;
| [[Gravitoelectromagnetism]] || GEM provides the weak-field framework; Woodward operates in GEM territory&lt;br /&gt;
|-&lt;br /&gt;
| [[Kaluza-Klein Unification]] || Both are GR-based; KK unifies EM and gravity geometrically while Woodward modifies mass inertially&lt;br /&gt;
|-&lt;br /&gt;
| [[Ning Li|Li-Torr]] || Different mechanism entirely — Li-Torr generates B_g field; Woodward modifies m&lt;br /&gt;
|-&lt;br /&gt;
| [[Pais Effect]] || Both target mass modification; Pais via vacuum polarization, Woodward via Mach principle&lt;br /&gt;
|-&lt;br /&gt;
| [[Heim Theory]] || Heim predicts new forces from extra dimensions; Woodward stays within 4D GR&lt;br /&gt;
|-&lt;br /&gt;
| [[Biefeld-Brown Effect]] || Woodward uses PZT at low voltage; Brown uses high voltage; different physics&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Significance for Magneto Speeder ==&lt;br /&gt;
&lt;br /&gt;
The Woodward effect provides an &amp;#039;&amp;#039;&amp;#039;alternative mechanism&amp;#039;&amp;#039;&amp;#039; for the [[Magneto Speeder]]:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Primary design:&amp;#039;&amp;#039;&amp;#039; Magnetogravitic — [[Gravitomagnetic London Moment]] via rotor array&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Secondary/hybrid:&amp;#039;&amp;#039;&amp;#039; Woodward-type mass fluctuation in PZT-embedded structural elements&lt;br /&gt;
&lt;br /&gt;
Key advantages of a hybrid approach:&lt;br /&gt;
* Woodward effect does not require superconductors — could serve as backup/auxiliary propulsion&lt;br /&gt;
* PZT actuators are compact, lightweight, and commercially available&lt;br /&gt;
* If both mechanisms contribute, thrust requirements for each are relaxed&lt;br /&gt;
&lt;br /&gt;
Key limitation: current Woodward thrust (~µN) is ~10⁹× too weak for vehicle-scale propulsion. Scaling requires:&lt;br /&gt;
* Much higher frequencies (GHz regime)&lt;br /&gt;
* Much larger PZT arrays&lt;br /&gt;
* Significant theoretical breakthrough in coupling efficiency&lt;br /&gt;
&lt;br /&gt;
== Publications ==&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Key Woodward Publications&lt;br /&gt;
|-&lt;br /&gt;
! Year !! Title !! Venue&lt;br /&gt;
|-&lt;br /&gt;
| 1990 || &amp;quot;A new experimental approach to Mach&amp;#039;s principle and relativistic gravitation&amp;quot; || Found. Phys. Lett.&lt;br /&gt;
|-&lt;br /&gt;
| 1991 || &amp;quot;Measurements of a Machian transient mass fluctuation&amp;quot; || Found. Phys. Lett.&lt;br /&gt;
|-&lt;br /&gt;
| 2004 || &amp;quot;Flux Capacitors and the Origin of Inertia&amp;quot; || Found. Phys.&lt;br /&gt;
|-&lt;br /&gt;
| 2013 || &amp;#039;&amp;#039;Making Starships and Stargates&amp;#039;&amp;#039; || Springer (book)&lt;br /&gt;
|-&lt;br /&gt;
| 2015 || &amp;quot;Theory of a Mach Effect Thruster&amp;quot; (with Fearn et al.) || J. Modern Phys.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
* [[Gravitoelectromagnetism]]&lt;br /&gt;
* [[Pais Effect]]&lt;br /&gt;
* [[Heim Theory]]&lt;br /&gt;
* [[Ning Li]]&lt;br /&gt;
* [[Martin Tajmar]]&lt;br /&gt;
* [[Electrogravitics]]&lt;br /&gt;
* [[Magnetogravitics]]&lt;br /&gt;
* [[Magneto Speeder]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Category:Physics]]&lt;br /&gt;
[[Category:Technology]]&lt;br /&gt;
[[Category:Electrogravitic Tech]]&lt;br /&gt;
[[Category:Magnetogravitic Tech]]&lt;br /&gt;
[[Category:Clan Tho&amp;#039;ra]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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