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		<updated>2026-05-23T11:54:42Z</updated>
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	<entry>
		<id>http://wiki.newmars.com/index.php?title=Rocket_equation&amp;diff=892</id>
		<title>Rocket equation</title>
		<link rel="alternate" type="text/html" href="http://wiki.newmars.com/index.php?title=Rocket_equation&amp;diff=892"/>
				<updated>2010-04-09T21:04:28Z</updated>
		
		<summary type="html">&lt;p&gt;Techer: /* Relativistic Rocket Equation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The rocket equation is one solution to the momentum method of calculating a rocket&amp;#039;s [[delta v]].  The equation is:&lt;br /&gt;
&lt;br /&gt;
 v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; - v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; &amp;#039;&amp;#039;ln&amp;#039;&amp;#039;R&lt;br /&gt;
&lt;br /&gt;
where: &lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;\Delta&amp;lt;/math&amp;gt;v = v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; - v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&lt;br /&gt;
 v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; = Final Velocity of Rocket&lt;br /&gt;
 v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = Initial Velocity of Rocket&lt;br /&gt;
 v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; = [[Exhaust Velocity]] of the rocket&lt;br /&gt;
 R = [[Mass Ratio]] of Rocket&lt;br /&gt;
 &lt;br /&gt;
&amp;#039;&amp;#039;ln&amp;#039;&amp;#039;R is the natural logarithm of R.&lt;br /&gt;
&lt;br /&gt;
==Mathematics==&lt;br /&gt;
&lt;br /&gt;
The rocket equation is derived from the conservation of momentum.&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Sigma p_{i} = \Sigma p_{f} = Constant &amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If mass is exhausted from a rocket engine at some mass flow rate m&amp;#039;&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; and some exhaust velocity v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt;, then that exhaust steam carries momentum, manifested as [[thrust]]:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;{dp \over dt} = m&amp;#039;_{e} v_{e} = v_{e} {dm \over dt} = m {dv \over dt}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using the algebraic representation of derivatives, this differential equation can be reduced to:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;dv = v_{e} {dm \over m}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the exhaust velocity is constant, then the integral of this is the rocket equation.&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta v = \int dv = v_{e} \int {dm \over m} = v_{e} ln (R)&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Conservation of momentum can be applied to more propulsion situations than the simple case presented above.  For example, under the influence of constant gravity:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;{dp \over dt} = m&amp;#039;_{e} v_{e} + g cos( \theta )&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using the substitutions listed above, the integral of this relationship becomes:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta v = v_{e} ln (R) + g t cos( /theta )&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the exhaust consists of two separate gas streams whose mass flow rates keep some constant ratio, r, to each other:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;r = {m&amp;#039;_{1} \over m&amp;#039;_{2}}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;v_{avg} = { v_{1} m&amp;#039;_{1} + v_{2} m&amp;#039;_{2} \over m&amp;#039;_{1} + m&amp;#039;_{2}}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;v_{avg} = { r v_{1} + v_{2} \over r + 1 }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and v&amp;lt;sub&amp;gt;avg&amp;lt;/sub&amp;gt; can be substituted into the rocket equation rather than v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Example==&lt;br /&gt;
&lt;br /&gt;
==Relativistic Rocket Equation==&lt;br /&gt;
The rocket equation for speeds that become relativistic (~0.1c) is: &lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\frac{\Delta v}{c} = \tanh(\frac{v_e \ln(m_i/m_f)}{c\sqrt{1-\frac{v_e^2}{c^2}}})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;tanh&amp;#039;&amp;#039; is the hyperbolic tangent function.&lt;br /&gt;
&lt;br /&gt;
==External Links==&lt;br /&gt;
&lt;br /&gt;
*[http://en.wikipedia.org/wiki/Rocket_equation Wikipedia Article: Tsiolkovsky Rocket Equation]&lt;/div&gt;</summary>
		<author><name>Techer</name></author>	</entry>

	<entry>
		<id>http://wiki.newmars.com/index.php?title=Rocket_equation&amp;diff=803</id>
		<title>Rocket equation</title>
		<link rel="alternate" type="text/html" href="http://wiki.newmars.com/index.php?title=Rocket_equation&amp;diff=803"/>
				<updated>2009-10-22T23:23:38Z</updated>
		
		<summary type="html">&lt;p&gt;Techer: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The rocket equation is one solution to the momentum method of calculating a rocket&amp;#039;s [[delta v]].  The equation is:&lt;br /&gt;
&lt;br /&gt;
 v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; - v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; &amp;#039;&amp;#039;ln&amp;#039;&amp;#039;R&lt;br /&gt;
&lt;br /&gt;
where: &lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;\Delta&amp;lt;/math&amp;gt;v = v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; - v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&lt;br /&gt;
 v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; = Final Velocity of Rocket&lt;br /&gt;
 v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = Initial Velocity of Rocket&lt;br /&gt;
 v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; = [[Exhaust Velocity]] of the rocket&lt;br /&gt;
 R = [[Mass Ratio]] of Rocket&lt;br /&gt;
 &lt;br /&gt;
&amp;#039;&amp;#039;ln&amp;#039;&amp;#039;R is the natural logarithm of R.&lt;br /&gt;
&lt;br /&gt;
==Mathematics==&lt;br /&gt;
&lt;br /&gt;
The rocket equation is derived from the conservation of momentum.&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Sigma p_{i} = \Sigma p_{f} = Constant &amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If mass is exhausted from a rocket engine at some mass flow rate m&amp;#039;&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; and some exhaust velocity v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt;, then that exhaust steam carries momentum, manifested as [[thrust]]:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;{dp \over dt} = m&amp;#039;_{e} v_{e} = v_{e} {dm \over dt} = m {dv \over dt}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using the algebraic representation of derivatives, this differential equation can be reduced to:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;dv = v_{e} {dm \over m}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the exhaust velocity is constant, then the integral of this is the rocket equation.&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta v = \int dv = v_{e} \int {dm \over m} = v_{e} ln (R)&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Conservation of momentum can be applied to more propulsion situations than the simple case presented above.  For example, under the influence of constant gravity:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;{dp \over dt} = m&amp;#039;_{e} v_{e} + g cos( \theta )&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using the substitutions listed above, the integral of this relationship becomes:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta v = v_{e} ln (R) + g t cos( /theta )&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the exhaust consists of two separate gas streams whose mass flow rates keep some constant ratio, r, to each other:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;r = {m&amp;#039;_{1} \over m&amp;#039;_{2}}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;v_{avg} = { v_{1} m&amp;#039;_{1} + v_{2} m&amp;#039;_{2} \over m&amp;#039;_{1} + m&amp;#039;_{2}}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;v_{avg} = { r v_{1} + v_{2} \over r + 1 }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and v&amp;lt;sub&amp;gt;avg&amp;lt;/sub&amp;gt; can be substituted into the rocket equation rather than v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Example==&lt;br /&gt;
&lt;br /&gt;
==Relativistic Rocket Equation==&lt;br /&gt;
The rocket equation for speeds that become relativistic (~0.1c) is: &lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta&amp;lt;/math&amp;gt;v \over c = &amp;#039;&amp;#039;tanh&amp;#039;&amp;#039; ( {v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; \over c} &amp;#039;&amp;#039;ln&amp;#039;&amp;#039; R)&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;tanh&amp;#039;&amp;#039; is the hyperbolic tangent function.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==External Links==&lt;br /&gt;
&lt;br /&gt;
*[http://en.wikipedia.org/wiki/Rocket_equation Wikipedia Article: Tsiolkovsky Rocket Equation]&lt;/div&gt;</summary>
		<author><name>Techer</name></author>	</entry>

	<entry>
		<id>http://wiki.newmars.com/index.php?title=Rocket_equation&amp;diff=802</id>
		<title>Rocket equation</title>
		<link rel="alternate" type="text/html" href="http://wiki.newmars.com/index.php?title=Rocket_equation&amp;diff=802"/>
				<updated>2009-10-18T21:44:40Z</updated>
		
		<summary type="html">&lt;p&gt;Techer: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The rocket equation is one solution to the momentum method of calculating a rocket&amp;#039;s [[delta v]].  The equation is:&lt;br /&gt;
&lt;br /&gt;
 v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; - v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; &amp;#039;&amp;#039;ln&amp;#039;&amp;#039;R&lt;br /&gt;
&lt;br /&gt;
where: &lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;\Delta&amp;lt;/math&amp;gt;v = v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; - v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&lt;br /&gt;
 v&amp;lt;sub&amp;gt;f&amp;lt;/sub&amp;gt; = Final Velocity of Rocket&lt;br /&gt;
 v&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = Initial Velocity of Rocket&lt;br /&gt;
 v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; = [[Exhaust Velocity]] of the rocket&lt;br /&gt;
 R = [[Mass Ratio]] of Rocket&lt;br /&gt;
 &lt;br /&gt;
&amp;#039;&amp;#039;ln&amp;#039;&amp;#039;R is the natural logarithm of R.&lt;br /&gt;
&lt;br /&gt;
==Mathematics==&lt;br /&gt;
&lt;br /&gt;
The rocket equation is derived from the conservation of momentum.&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Sigma p_{i} = \Sigma p_{f} = Constant &amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If mass is exhausted from a rocket engine at some mass flow rate m&amp;#039;&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; and some exhaust velocity v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt;, then that exhaust steam carries momentum, manifested as [[thrust]]:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;{dp \over dt} = m&amp;#039;_{e} v_{e} = v_{e} {dm \over dt} = m {dv \over dt}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using the algebraic representation of derivatives, this differential equation can be reduced to:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;dv = v_{e} {dm \over m}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the exhaust velocity is constant, then the integral of this is the rocket equation.&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta v = \int dv = v_{e} \int {dm \over m} = v_{e} ln (R)&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Conservation of momentum can be applied to more propulsion situations than the simple case presented above.  For example, under the influence of constant gravity:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;{dp \over dt} = m&amp;#039;_{e} v_{e} + g cos( \theta )&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using the substitutions listed above, the integral of this relationship becomes:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta v = v_{e} ln (R) + g t cos( /theta )&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the exhaust consists of two separate gas streams whose mass flow rates keep some constant ratio, r, to each other:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;r = {m&amp;#039;_{1} \over m&amp;#039;_{2}}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;v_{avg} = { v_{1} m&amp;#039;_{1} + v_{2} m&amp;#039;_{2} \over m&amp;#039;_{1} + m&amp;#039;_{2}}&amp;lt;/math&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus:&lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;v_{avg} = { r v_{1} + v_{2} \over r + 1 }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and v&amp;lt;sub&amp;gt;avg&amp;lt;/sub&amp;gt; can be substituted into the rocket equation rather than v&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Example==&lt;br /&gt;
&lt;br /&gt;
==Relativistic Rocket Equation==&lt;br /&gt;
The rocket equation for speeds that become relativistic (~0.1c) is: &lt;br /&gt;
&lt;br /&gt;
     &amp;lt;math&amp;gt;\Delta&amp;lt;/math&amp;gt;v \over c = &amp;#039;&amp;#039;tanh&amp;#039;&amp;#039; ( &amp;#039;&amp;#039;ln&amp;#039;&amp;#039; R)&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;tanh&amp;#039;&amp;#039; is the hyperbolic tangent function.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==External Links==&lt;br /&gt;
&lt;br /&gt;
*[http://en.wikipedia.org/wiki/Rocket_equation Wikipedia Article: Tsiolkovsky Rocket Equation]&lt;/div&gt;</summary>
		<author><name>Techer</name></author>	</entry>

	</feed>