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	<id>https://wiki.fusiongirl.app:443/index.php?action=history&amp;feed=atom&amp;title=Magnetohydrodynamics</id>
	<title>Magnetohydrodynamics - Revision history</title>
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	<updated>2026-04-30T18:26:59Z</updated>
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		<id>https://wiki.fusiongirl.app:443/index.php?title=Magnetohydrodynamics&amp;diff=6164&amp;oldid=prev</id>
		<title>JonoThora: Deep rewrite — full MHD equations, dimensionless numbers, atmospheric propulsion engineering</title>
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		<updated>2026-03-14T02:05:18Z</updated>

		<summary type="html">&lt;p&gt;Deep rewrite — full MHD equations, dimensionless numbers, atmospheric propulsion engineering&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      = Magnetohydrodynamics&lt;br /&gt;
| image      =&lt;br /&gt;
| caption    = MHD — fluid dynamics of conducting fluids in magnetic fields&lt;br /&gt;
| header1    = Overview&lt;br /&gt;
| label2     = Abbreviation&lt;br /&gt;
| data2      = MHD&lt;br /&gt;
| label3     = Domain&lt;br /&gt;
| data3      = Plasma physics · fluid mechanics · electromagnetism&lt;br /&gt;
| label4     = Key Equation&lt;br /&gt;
| data4      = ρ(Dv/Dt) = −∇P + J×B + η∇²v&lt;br /&gt;
| label5     = Applications&lt;br /&gt;
| data5      = Propulsion · power generation · astrophysics&lt;br /&gt;
| label6     = Tho&amp;#039;ra Use&lt;br /&gt;
| data6      = [[Magneto Speeder]] + [[Star Speeder]] primary thrust&lt;br /&gt;
| header7    = Key Parameters&lt;br /&gt;
| label8     = Reynolds_m&lt;br /&gt;
| data8      = Rm = μ₀σvL (magnetic Reynolds number)&lt;br /&gt;
| label9     = Hartmann&lt;br /&gt;
| data9      = Ha = BL√(σ/η) (flow-field coupling)&lt;br /&gt;
| label10    = Alfvén Speed&lt;br /&gt;
| data10     = v_A = B/√(μ₀ρ)&lt;br /&gt;
| below      = &amp;#039;&amp;#039;Foundation of [[MHD Tech]]&amp;#039;&amp;#039;&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Magnetohydrodynamics&amp;#039;&amp;#039;&amp;#039; (&amp;#039;&amp;#039;&amp;#039;MHD&amp;#039;&amp;#039;&amp;#039;) is the study of electrically conducting fluids — plasmas, liquid metals, ionized gases — under the influence of magnetic fields. It unifies fluid mechanics with electromagnetism via the Lorentz force &amp;lt;math&amp;gt;\mathbf{J} \times \mathbf{B}&amp;lt;/math&amp;gt;, creating a rich physics that governs phenomena from stellar dynamos to submarine propulsion.&lt;br /&gt;
&lt;br /&gt;
In Tho&amp;#039;ra technology, MHD provides the &amp;#039;&amp;#039;&amp;#039;primary atmospheric thrust mechanism&amp;#039;&amp;#039;&amp;#039; for the [[Magneto Speeder]] and a key subsystem of the [[Star Speeder]]&amp;#039;s integrated propulsion.&lt;br /&gt;
&lt;br /&gt;
== Governing Equations ==&lt;br /&gt;
&lt;br /&gt;
The MHD system is described by coupled partial differential equations combining the Navier-Stokes equations with Maxwell&amp;#039;s equations:&lt;br /&gt;
&lt;br /&gt;
=== Momentum Equation ===&lt;br /&gt;
&amp;lt;math&amp;gt;\rho\left(\frac{\partial \mathbf{v}}{\partial t} + (\mathbf{v} \cdot \nabla)\mathbf{v}\right) = -\nabla P + \mathbf{J} \times \mathbf{B} + \eta\nabla^2\mathbf{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The &amp;lt;math&amp;gt;\mathbf{J} \times \mathbf{B}&amp;lt;/math&amp;gt; term is the Lorentz body force — this is what generates thrust. When current flows perpendicular to a magnetic field, the resulting force accelerates the conducting fluid, and by Newton&amp;#039;s third law, the vehicle.&lt;br /&gt;
&lt;br /&gt;
=== Induction Equation ===&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\partial \mathbf{B}}{\partial t} = \nabla \times (\mathbf{v} \times \mathbf{B}) + \frac{\eta_m}{\mu_0}\nabla^2\mathbf{B}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\eta_m = 1/(\mu_0\sigma)&amp;lt;/math&amp;gt; is the magnetic diffusivity. The first term represents advection (flux frozen into the fluid), and the second represents diffusion (field decay due to resistivity).&lt;br /&gt;
&lt;br /&gt;
=== Ohm&amp;#039;s Law (MHD form) ===&lt;br /&gt;
&amp;lt;math&amp;gt;\mathbf{E} + \mathbf{v} \times \mathbf{B} = \frac{\mathbf{J}}{\sigma}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In ideal MHD (&amp;lt;math&amp;gt;\sigma \rightarrow \infty&amp;lt;/math&amp;gt;): &amp;lt;math&amp;gt;\mathbf{E} = -\mathbf{v} \times \mathbf{B}&amp;lt;/math&amp;gt;, and magnetic field lines are &amp;quot;frozen&amp;quot; into the fluid.&lt;br /&gt;
&lt;br /&gt;
=== Energy Equation ===&lt;br /&gt;
&amp;lt;math&amp;gt;\rho\left(\frac{\partial \varepsilon}{\partial t} + \mathbf{v} \cdot \nabla\varepsilon\right) = -P\nabla \cdot \mathbf{v} + \nabla \cdot (k\nabla T) + \frac{J^2}{\sigma}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The &amp;lt;math&amp;gt;J^2/\sigma&amp;lt;/math&amp;gt; term represents Ohmic (Joule) heating — significant for MHD thruster thermal management.&lt;br /&gt;
&lt;br /&gt;
=== Continuity Equation ===&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\partial \rho}{\partial t} + \nabla \cdot (\rho\mathbf{v}) = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Dimensionless Numbers ==&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Key MHD Dimensionless Parameters&lt;br /&gt;
|-&lt;br /&gt;
! Number !! Definition !! Physical Meaning !! Magneto Speeder Value&lt;br /&gt;
|-&lt;br /&gt;
| Magnetic Reynolds (&amp;lt;math&amp;gt;R_m&amp;lt;/math&amp;gt;) || &amp;lt;math&amp;gt;\mu_0 \sigma v L&amp;lt;/math&amp;gt; || Advection vs. diffusion of B-field || ~10–100 (ionized air)&lt;br /&gt;
|-&lt;br /&gt;
| Hartmann (&amp;lt;math&amp;gt;Ha&amp;lt;/math&amp;gt;) || &amp;lt;math&amp;gt;BL\sqrt{\sigma/\eta}&amp;lt;/math&amp;gt; || EM force vs. viscous force || ~50–500&lt;br /&gt;
|-&lt;br /&gt;
| Stuart (&amp;lt;math&amp;gt;N&amp;lt;/math&amp;gt;) || &amp;lt;math&amp;gt;\sigma B^2 L / (\rho v)&amp;lt;/math&amp;gt; || EM force vs. inertial force || ~0.1–10&lt;br /&gt;
|-&lt;br /&gt;
| Alfvén Mach (&amp;lt;math&amp;gt;M_A&amp;lt;/math&amp;gt;) || &amp;lt;math&amp;gt;v/v_A = v\sqrt{\mu_0\rho}/B&amp;lt;/math&amp;gt; || Flow vs. Alfvén wave speed || ~0.01–1&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Alfvén Waves ===&lt;br /&gt;
MHD supports transverse waves propagating along magnetic field lines:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;v_A = \frac{B}{\sqrt{\mu_0 \rho}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For the Magneto Speeder&amp;#039;s ionized air channel (&amp;lt;math&amp;gt;B = 2\,\text{T}&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\rho = 0.1\,\text{kg/m}^3&amp;lt;/math&amp;gt;):&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;v_A = \frac{2}{\sqrt{4\pi \times 10^{-7} \times 0.1}} \approx 5{,}640\,\text{m/s}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Alfvén waves carry energy and information through the MHD propulsion channel, enabling distributed thrust control.&lt;br /&gt;
&lt;br /&gt;
== MHD Propulsion Engineering ==&lt;br /&gt;
&lt;br /&gt;
=== Principle of Operation ===&lt;br /&gt;
An MHD thruster accelerates a conducting fluid using the Lorentz force:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\mathbf{F}_{\text{thrust}} = \int_V (\mathbf{J} \times \mathbf{B})\,dV&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a channel of length &amp;lt;math&amp;gt;L&amp;lt;/math&amp;gt;, width &amp;lt;math&amp;gt;w&amp;lt;/math&amp;gt;, height &amp;lt;math&amp;gt;h&amp;lt;/math&amp;gt;, with uniform &amp;lt;math&amp;gt;J&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;B&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;F = J \cdot B \cdot L \cdot w \cdot h = \sigma(E + vB) \cdot B \cdot V_{\text{channel}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Atmospheric MHD (Magneto Speeder) ===&lt;br /&gt;
The [[Magneto Speeder]] ionizes air ahead of the vehicle using:&lt;br /&gt;
* UV photoionization array (excimer laser, 172 nm)&lt;br /&gt;
* Microwave breakdown (2.45 GHz magnetron, ~1 kW)&lt;br /&gt;
* Seed injection (cesium or potassium vapor for lowered ionization potential)&lt;br /&gt;
&lt;br /&gt;
Achievable ionization fraction: &amp;lt;math&amp;gt;\alpha \approx 10^{-4}&amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;10^{-2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Effective air conductivity with cesium seeding: &amp;lt;ref&amp;gt;Rosa, R.J. (1987). &amp;#039;&amp;#039;Magnetohydrodynamic Energy Conversion&amp;#039;&amp;#039;. Hemisphere Publishing. ISBN 0-89116-690-9.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\sigma_{\text{air}} = \frac{n_e e^2}{m_e \nu_{en}} \approx 10 - 100\,\text{S/m}\quad\text{(with seeding at 2000–3000 K)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Compare: seawater &amp;lt;math&amp;gt;\sigma \approx 5\,\text{S/m}&amp;lt;/math&amp;gt;, copper &amp;lt;math&amp;gt;\sigma \approx 5.8 \times 10^7\,\text{S/m}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
=== Seawater MHD (Historical Precedent) ===&lt;br /&gt;
The Yamato 1 (1992) demonstrated seawater MHD propulsion: &amp;lt;ref&amp;gt;Motora, S. et al. (1992). &amp;quot;An Experimental Study on Superconducting MHD Ship Propulsion.&amp;quot; &amp;#039;&amp;#039;J. Ship Research&amp;#039;&amp;#039; 36(4), 361–367.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* 4 Tesla superconducting magnets&lt;br /&gt;
* Seawater as working fluid (&amp;lt;math&amp;gt;\sigma \approx 5\,\text{S/m}&amp;lt;/math&amp;gt;)&lt;br /&gt;
* Achieved ~8 knots (limited by low conductivity and electrode drag)&lt;br /&gt;
* Demonstrated the principle; atmospheric MHD with ionized air achieves higher &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== MHD Thruster Performance ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ Estimated MHD Thruster Parameters (Magneto Speeder)&lt;br /&gt;
|-&lt;br /&gt;
! Parameter !! Value !! Notes&lt;br /&gt;
|-&lt;br /&gt;
| Magnetic field (B) || 2–5 T || HTS magnets (REBCO tape)&lt;br /&gt;
|-&lt;br /&gt;
| Channel volume || 0.1 m³ (total, 4 nozzles) || Distributed around vehicle&lt;br /&gt;
|-&lt;br /&gt;
| Air conductivity (σ) || 50 S/m (seeded, ionized) || Cs-seeded at ~2500 K&lt;br /&gt;
|-&lt;br /&gt;
| Current density (J) || 10⁴ A/m² || External drive + self-excitation&lt;br /&gt;
|-&lt;br /&gt;
| Thrust per nozzle || ~2.5 kN || &amp;lt;math&amp;gt;F = JBV = 10^4 \times 3 \times 0.025 \times 3&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| Total thrust || ~10 kN || 4 nozzles, full power&lt;br /&gt;
|-&lt;br /&gt;
| Specific impulse || ~3,000–8,000 s || Working fluid is ambient air&lt;br /&gt;
|-&lt;br /&gt;
| Power input || ~50 kW || From [[Micro Fusion Fuel Cells]]&lt;br /&gt;
|-&lt;br /&gt;
| Thrust-to-power || ~200 N/kW || Competitive with ion thrusters&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Efficiency ===&lt;br /&gt;
MHD thruster electrical efficiency:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\eta_{\text{MHD}} = \frac{F \cdot v}{P_{\text{input}}} = \frac{\text{thrust power}}{\text{electrical input}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the Magneto Speeder&amp;#039;s cruise speed of Mach 1 (~340 m/s):&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\eta = \frac{10{,}000 \times 340}{50{,}000} = 68\%&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This increases with vehicle speed (unlike propeller propulsion which decreases), making MHD &amp;#039;&amp;#039;especially efficient&amp;#039;&amp;#039; at high Mach numbers.&lt;br /&gt;
&lt;br /&gt;
== Symbol Definitions ==&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+ MHD Equation Symbols&lt;br /&gt;
|-&lt;br /&gt;
! Symbol !! Name !! Units&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; || Fluid density || kg/m³&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\mathbf{v}&amp;lt;/math&amp;gt; || Fluid velocity || m/s&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;P&amp;lt;/math&amp;gt; || Pressure || Pa&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\mathbf{J}&amp;lt;/math&amp;gt; || Current density || A/m²&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\mathbf{B}&amp;lt;/math&amp;gt; || Magnetic field || T&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\mathbf{E}&amp;lt;/math&amp;gt; || Electric field || V/m&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\eta&amp;lt;/math&amp;gt; || Dynamic viscosity || Pa·s&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt; || Electrical conductivity || S/m&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\mu_0&amp;lt;/math&amp;gt; || Vacuum permeability || H/m&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt; || Thermal conductivity || W/(m·K)&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\varepsilon&amp;lt;/math&amp;gt; || Specific internal energy || J/kg&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Related Topics ==&lt;br /&gt;
* [[MHD Fluids, Quantum Mechanics and Spin Waves]]&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
* [[MHD Core]]&lt;br /&gt;
* [[Magnetogravitics]]&lt;br /&gt;
* [[Electrogravitics]]&lt;br /&gt;
* [[Magneto Speeder]]&lt;br /&gt;
* [[Star Speeder]]&lt;br /&gt;
* [[MHD Tech]]&lt;br /&gt;
* [[Clan Tho&amp;#039;ra]]&lt;br /&gt;
&lt;br /&gt;
{{PhysicsPortal}}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Category:Technology]]&lt;br /&gt;
[[Category:MHD Tech]]&lt;br /&gt;
[[Category:Physics]]&lt;br /&gt;
[[Category:Propulsion]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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