<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-19T09:22:23Z</responseDate><request verb="GetRecord" identifier="oai:wakespace.lib.wfu.edu:10339/90751" metadataPrefix="dim">https://wakespace.lib.wfu.edu/server/oai/request</request><GetRecord><record><header><identifier>oai:null:10339/90751</identifier><datestamp>2026-09-02T08:58:02Z</datestamp><setSpec>com_10339_14934</setSpec><setSpec>col_10339_38132</setSpec></header><metadata><dim:dim xmlns:dim="http://www.dspace.org/xmlns/dspace/dim" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.dspace.org/xmlns/dspace/dim http://www.dspace.org/schema/dim.xsd">
   <dim:field mdschema="dc" element="contributor" qualifier="author" lang="en_US">McConkey, Robert</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="accessioned">2018-05-24T08:36:17Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="available">2018-05-24T08:36:17Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="issued" lang="en_US">2018</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="uri">https://wakespace.lib.wfu.edu/handle/10339/90751</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="abstract" lang="en_US">In  this  thesis  we  will  focus  on  the  topic  of  helicity.   Helicity  gives  us  a  way  to&#xd;
measure the coiling of flow lines in a vector field, computed by the formula&#xd;
[see formula in PDF file]&#xd;
.&#xd;
To start our exploration of helicity we begin with the topic of differential forms and&#xd;
their  correspondence  with  vector  fields  in&#xd;
R&#xd;
3&#xd;
.   Then  we  use  the  correspondence  of&#xd;
forms  and  vector  fields  to  show  that  Maxwell’s  Equations  can  be  reduced  to  two&#xd;
equations of differential forms. We continue our exploration of mathematics in physics&#xd;
with the Biot-Savart operator; this operator calculates the associated magnetic field&#xd;
on a domain Ω given an electric current on Ω.  The Biot-Savart operator gives us a&#xd;
way to compute vector field helicity.&#xd;
We will begin our exploration of helicity with its standard definition above, and&#xd;
where it comes of use in both mathematics and physics.  Next we return to differential&#xd;
forms to show how the correspondence to vector fields allows us to define the helicity&#xd;
of forms.  Then using helicity of forms we can expand on the three-dimensional idea&#xd;
of helicity to both submanifolds and higher dimension ambient spaces.</dim:field>
   <dim:field mdschema="dc" element="language" qualifier="iso" lang="en_US">en</dim:field>
   <dim:field mdschema="dc" element="publisher" lang="en_US">Wake Forest University</dim:field>
   <dim:field mdschema="dc" element="subject" lang="en_US" />
   <dim:field mdschema="dc" element="title" lang="en_US">Submanifold Helicity</dim:field>
   <dim:field mdschema="dc" element="type" lang="en_US">Thesis</dim:field>
   <dim:field mdschema="thesis" element="contributor" qualifier="committeeChair" lang="en_US">Parsley, Robert J</dim:field>
   <dim:field mdschema="thesis" element="contributor" qualifier="committeeMember" lang="en_US">Moore, William F</dim:field>
   <dim:field mdschema="thesis" element="degree" qualifier="discipline" lang="en_US">Mathematics and Statistics</dim:field>
   <dim:field mdschema="others" element="access-status">open.access</dim:field>
</dim:dim>
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