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	<title>TDK Propulsion &#187; Oxamide</title>
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	<description>Research 2.0</description>
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		<title>Mass Flux and Erosive Burning</title>
		<link>http://www.tdkpropulsion.com/2008/07/mass-flux-and-erosive-burning/</link>
		<comments>http://www.tdkpropulsion.com/2008/07/mass-flux-and-erosive-burning/#comments</comments>
		<pubDate>Tue, 01 Jul 2008 23:49:16 +0000</pubDate>
		<dc:creator>David Reese</dc:creator>
				<category><![CDATA[Propulsion Theory]]></category>
		<category><![CDATA[Double-Taper]]></category>
		<category><![CDATA[erosive burning]]></category>
		<category><![CDATA[Mass Flux]]></category>
		<category><![CDATA[Oxamide]]></category>
		<category><![CDATA[theory]]></category>

		<guid isPermaLink="false">http://www.tdkpropulsion.com/?p=31</guid>
		<description><![CDATA[There has been a lot of discussion as of late regarding erosive burning and its relation to mass flux. Many have suggested that propellants with certain additives (notably, Oxamide) have a better response to high mass flux conditions, and have proven with ample results that it in fact does. While the effect these additives have [...]]]></description>
			<content:encoded><![CDATA[<p><img src="http://www.tdkpropulsion.com/wp-content/uploads/2008/07/zfs.jpg" alt="Business end of my first P motor in flight." title="What's the flow velocity HERE?  I bet you know!" width="450" height="162" class="aligncenter size-full wp-image-33" /><br />
There has been a lot of discussion as of late regarding erosive burning and its relation to mass flux.  Many have suggested that propellants with certain additives (notably, Oxamide) have a better response to high mass flux conditions, and have proven with <a href="http://tqc.yuku.com/topic/1024">ample</a> <a href="http://tqc.yuku.com/topic/2409">results</a> that it in fact does.  While the effect these additives have is noticeable, it does not seem to scale linearly with pressure, as I might have expected thanks to the basic interpretation of Vielle&#8217;s law.  After doing some thinking and some research, I happened upon some useful information on how to characterize the effect mass flux has on erosivity.  <span id="more-31"></span></p>
<p>Let&#8217;s start with mass flux.  <strong>Mass flux</strong> (
<p class="ql-center-displayed-equation" style="line-height: 12px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-670a7d70a0db0334aa060c3626c8fcc3_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#92;&#100;&#111;&#116;&#32;&#109;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p>) is simply a measurement of flow over an area at a certain velocity, and has units of mass per time-area.  In SI form, this turns out to be
<p class="ql-center-displayed-equation" style="line-height: 37px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-2907ee01cec58e47f1af372e7731f42b_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#92;&#100;&#111;&#116;&#32;&#109;&#32;&#61;&#32;&#92;&#102;&#114;&#97;&#99;&#123;&#107;&#103;&#125;&#123;&#109;&#94;&#50;&#45;&#115;&#101;&#99;&#125;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p>Conveniently, this has the same units as, and is in fact equal to<br /> 
<p class="ql-center-displayed-equation" style="line-height: 16px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-c2580bbbb4967474e13513f46096b80d_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#92;&#100;&#111;&#116;&#32;&#109;&#32;&#61;&#32;&#92;&#114;&#104;&#111;&#32;&#118;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p>where
<p class="ql-center-displayed-equation" style="line-height: 12px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-2b73a5909f983745cceecd4114496ffd_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#92;&#114;&#104;&#111;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> is the density of the stuff, and
<p class="ql-center-displayed-equation" style="line-height: 8px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-5fc4a527c3bd34ca6087e93430ea7298_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#118;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> is the stuff&#8217;s velocity.</p>
<p>In a rocket motor, there is equal pressure throughout the motor, and as the combustion products can be considered relatively homogeneous, it is a reasonable approximation to consider
<p class="ql-center-displayed-equation" style="line-height: 12px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-2b73a5909f983745cceecd4114496ffd_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#92;&#114;&#104;&#111;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> to be constant.  Thus it seems that
<p class="ql-center-displayed-equation" style="line-height: 12px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-670a7d70a0db0334aa060c3626c8fcc3_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#92;&#100;&#111;&#116;&#32;&#109;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> is essentially directly proportional to flow velocity
<p class="ql-center-displayed-equation" style="line-height: 8px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-5fc4a527c3bd34ca6087e93430ea7298_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#118;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p>, assuming non-choked conditions.</p>
<p>Perusing <a href="http://www.amazon.com/Gas-Dynamics-Maurice-J-Zucrow/dp/047198440X">a gas dynamics book</a> one day (like all good children of science?), I happened upon our good old friend, Vielle&#8217;s Law.  Except it was weird.  There was something else involved.  Zucrow and Hoffman had written it this way:
<p class="ql-center-displayed-equation" style="line-height: 18px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-5dfbdadffbc7b6de8e1a8e38e5666df9_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#92;&#100;&#111;&#116;&#32;&#114;&#32;&#61;&#32;&#40;&#49;&#43;&#107;&#86;&#41;&#97;&#80;&#94;&#110;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p>  At first glance, it&#8217;s much different from the one I learned from McCreary and Wickman, but really it&#8217;s the same thing with an extra constant on the front &#8212;
<p class="ql-center-displayed-equation" style="line-height: 14px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-5712af9eb397836dced9372f29d327b6_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#49;&#43;&#107;&#86;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> &#8212; a constant relating to velocity.</p>
<p>Light bulb goes on.  That&#8217;s an erosive burning modifier.</p>
<p>Using simple 1-D fluid models, it makes terrific sense.  Thus it seems that the addition of Oxamide (or any other burn rate modifier) isn&#8217;t just tampering with just the values for
<p class="ql-center-displayed-equation" style="line-height: 8px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-691a919eed4c5df8249fbb0508b14590_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#97;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> and
<p class="ql-center-displayed-equation" style="line-height: 8px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-0aeb904cf570356166bc0c876656655a_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#110;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> &#8212; it&#8217;s messing with the erosive constant
<p class="ql-center-displayed-equation" style="line-height: 13px;"><span class="ql-right-eqno"> &nbsp; </span><span class="ql-left-eqno"> &nbsp; </span><img src="http://www.tdkpropulsion.com/wp-content/ql-cache/quicklatex.com-b032361e970a9b2688b36af433646309_l3.png"class="ql-img-displayed-equation" alt="&#92;&#91;&#107;&#92;&#93;" title="Rendered by QuickLaTeX.com"/></p>
<p> as well.  Man, this is worse than Robert Goulet in that Corn Nuts commercial.  Looks like you&#8217;ll need a few more test burns, Scott!</p>
<p>After this delightful epiphany, I then continued to ponder.  Why is <em>mass flux</em> such a big deal, rather than <em>flow velocity</em>?  I mean, it&#8217;s not like we can directly measure either one in an operating motor &#8212; why pick mass flux to be the <a href="http://www.thrustgear.com/topics/erosiveburn.htm">anointed child</a>?</p>
<p>Well, for now, I&#8217;ve settled on the conclusion that it&#8217;s easier to simulate mass flux than it is to simulate flow velocity.  Total mass flux can easily be calculated using a simple surface area model, while local flow velocity (note the word local &#8212; the equation requires the flow velocity at the propellant element under consideration to solve the new erosive rate) requires many assumptions about path, temperature, and upstream behavior of the gas.  Numerical flow code like FLUENT can probably do it.  I can&#8217;t (easily).</p>
<p>So mass flux is a decent method by which to figure out what the overall picture of the operating motor is, erosive-ly speaking.  It also allows the configuration of unique grain designs (double-taper, anyone?) by solving the mass flux at the internal choke point(s), allowing the designer to figure out how fast the odd points will wear away, and perhaps give some insight as to what&#8217;s going to happen when the motor comes on.  And mass flux seems to have a nice, solid basis in the world of fluid dynamics.  But in the end, it&#8217;s still just a model.  Testing of each unique design is still required.</p>
<p>Darn.  Another excuse to fire more rocket motors.</p>
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