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		<title>imported&gt;WikiHarold at 18:08, 28 April 2026</title>
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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Magnetic field component encircling the plasma cross-section in toroidal systems}}&lt;br /&gt;
&lt;br /&gt;
[[Book:Quantum_Collection/Matter_(by_scale)#Fields|← Back to Matter (by scale) Fields]]&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;poloidal field&amp;#039;&amp;#039;&amp;#039; is the component of the magnetic field that runs around the short (poloidal) direction of a toroidal plasma, such as in a [[Physics:Quantum Tokamak|tokamak]]. Together with the toroidal field, it forms helical magnetic field lines that confine charged particles within the plasma.&lt;br /&gt;
&lt;br /&gt;
In magnetic confinement systems, the combination of toroidal and poloidal fields is essential for achieving stable confinement. Without a poloidal component, particles would drift across field lines and escape the plasma.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;float:right; border:1px solid #e0d890; background:#fff8cc; padding:6px; margin:0 0 1em 1em; width:400px;&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Tokamak poloidal toroidal fields.svg|400px]]&lt;br /&gt;
&amp;lt;div style=&amp;quot;font-size:90%;&amp;quot;&amp;gt;Magnetic field geometry in a tokamak: the toroidal field wraps around the torus, while the poloidal field encircles the plasma cross-section, producing helical field lines.&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Physical meaning ==&lt;br /&gt;
&lt;br /&gt;
In a toroidal geometry, two directions are defined:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Toroidal direction&amp;#039;&amp;#039;&amp;#039; — around the major axis of the torus  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Poloidal direction&amp;#039;&amp;#039;&amp;#039; — around the minor cross-section  &lt;br /&gt;
&lt;br /&gt;
The poloidal field follows the second direction and is typically weaker than the toroidal field. However, it plays a crucial role in shaping the magnetic topology.&lt;br /&gt;
&lt;br /&gt;
The resulting helical field lines guide charged particles, preventing them from drifting freely across the plasma.&lt;br /&gt;
&lt;br /&gt;
== Generation of the poloidal field ==&lt;br /&gt;
&lt;br /&gt;
In a tokamak, the poloidal field is primarily generated by an electric current flowing through the plasma itself. This current is induced by transformer action and produces a magnetic field that encircles the plasma column.&lt;br /&gt;
&lt;br /&gt;
Additional external coils can also contribute to the poloidal field, allowing control of plasma position and shape.&lt;br /&gt;
&lt;br /&gt;
== Role in confinement ==&lt;br /&gt;
&lt;br /&gt;
The poloidal field is essential for magnetic confinement:&lt;br /&gt;
&lt;br /&gt;
* It twists magnetic field lines into helices  &lt;br /&gt;
* It reduces particle drift losses  &lt;br /&gt;
* It contributes to closed magnetic surfaces  &lt;br /&gt;
&lt;br /&gt;
Without the poloidal component, the magnetic field would be purely toroidal, and charged particles would gradually escape due to curvature and gradient drifts.&lt;br /&gt;
&lt;br /&gt;
== Relation to safety factor ==&lt;br /&gt;
&lt;br /&gt;
The ratio between toroidal and poloidal field components determines the &amp;#039;&amp;#039;&amp;#039;safety factor&amp;#039;&amp;#039;&amp;#039;:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
q = \frac{\text{toroidal turns}}{\text{poloidal turns}}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This parameter describes how magnetic field lines wind around the torus and is a key quantity in plasma stability analysis.&lt;br /&gt;
&lt;br /&gt;
== Connection to plasma stability ==&lt;br /&gt;
&lt;br /&gt;
The strength and structure of the poloidal field influence many plasma instabilities:&lt;br /&gt;
&lt;br /&gt;
* [[Physics:Kink instability|Kink instability]] depends on field line twist  &lt;br /&gt;
* [[Physics:Tearing mode|Tearing mode]] occurs at rational surfaces  &lt;br /&gt;
* [[Physics:Ballooning instability|Ballooning instability]] is affected by field curvature  &lt;br /&gt;
&lt;br /&gt;
Careful control of the poloidal field is therefore required to maintain stable confinement.&lt;br /&gt;
&lt;br /&gt;
== Applications ==&lt;br /&gt;
&lt;br /&gt;
Poloidal fields are central to:&lt;br /&gt;
&lt;br /&gt;
* [[Physics:Quantum Tokamak|Tokamak]] operation  &lt;br /&gt;
* [[Physics:Quantum Magnetically confined plasmas|Magnetic confinement systems]]  &lt;br /&gt;
* Plasma shaping and equilibrium control  &lt;br /&gt;
* Fusion reactor design  &lt;br /&gt;
&lt;br /&gt;
They are also relevant in astrophysical plasmas where toroidal and poloidal field components coexist.&lt;br /&gt;
&lt;br /&gt;
== Physical interpretation ==&lt;br /&gt;
&lt;br /&gt;
The poloidal field represents the coupling between plasma current and magnetic confinement. It transforms a simple toroidal field into a structured, self-consistent system capable of confining high-temperature plasma.&lt;br /&gt;
&lt;br /&gt;
Together with the toroidal field, it defines the geometry of magnetically confined plasmas.&lt;br /&gt;
&lt;br /&gt;
=See also=&lt;br /&gt;
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also}}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
{{reflist|3}}&lt;br /&gt;
&lt;br /&gt;
{{Author|Harold Foppele}}&lt;br /&gt;
&lt;br /&gt;
{{Sourceattribution|Poloidal field|1}}&lt;/div&gt;</summary>
		<author><name>imported&gt;WikiHarold</name></author>
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