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	<title>Solutions of Linear Systems - Revision history</title>
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	<updated>2026-05-21T02:17:33Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<id>https://mathresearch.utsa.edu/wiki/index.php?title=Solutions_of_Linear_Systems&amp;diff=4041&amp;oldid=prev</id>
		<title>Khanh at 06:29, 19 November 2021</title>
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		<updated>2021-11-19T06:29:54Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 06:29, 19 November 2021&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l16&quot; &gt;Line 16:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 16:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \phi(t) = Cy_1(t) + Dy_2(t) \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \phi(t) = Cy_1(t) + Dy_2(t) \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* So all solutions for this differential equation are a linear combination of the solutions &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* So all solutions for this differential equation are a linear combination of the solutions &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* &amp;lt;math&amp;gt;\Rightarrow&amp;lt;/math&amp;gt; Suppose that every point &amp;lt;math&amp;gt;t_0 \in I&amp;lt;/math&amp;gt; is such that &amp;lt;math&amp;gt;W(y_1, y_2) \bigg|_{t_0} = 0&amp;lt;/math&amp;gt;, that is, there exists no point &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; on &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; where the Wronskian of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; evaluated at &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; is nonzero. Let &amp;lt;math&amp;gt;y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y'_0&amp;lt;/math&amp;gt; be values for which the system &amp;lt;math&amp;gt;\left\{\begin{matrix} Cy_1(t_0) + Dy_2(t_0) = y_0 \\ Cy_1'(t_0) + Dy_2'(t_0) = y'_0 \end{matrix}\right.&amp;lt;/math&amp;gt; has no solutions for a set of constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* &amp;lt;math&amp;gt;\Rightarrow&amp;lt;/math&amp;gt; Suppose that every point &amp;lt;math&amp;gt;t_0 \in I&amp;lt;/math&amp;gt; is such that &amp;lt;math&amp;gt;W(y_1, y_2) \bigg|_{t_0} = 0&amp;lt;/math&amp;gt;, that is, there exists no point &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; on &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; where the Wronskian of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; evaluated at &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; is nonzero. Let &amp;lt;math&amp;gt;y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y'_0&amp;lt;/math&amp;gt; be values for which the system &amp;lt;math&amp;gt;\left\{\begin{matrix} Cy_1(t_0) + Dy_2(t_0) = y_0 \\ Cy_1'(t_0) + Dy_2'(t_0) = y'_0 \end{matrix}\right.&amp;lt;/math&amp;gt; has no solutions for a set of constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;	&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;	&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;*Now since &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; are continuous on an open interval &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; containing &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt;, such a solution &amp;lt;math&amp;gt;\phi(t)&amp;lt;/math&amp;gt; satisfies the initial conditions &amp;lt;math&amp;gt;y(t_0) = y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y'(t_0) = y'_0&amp;lt;/math&amp;gt;. Note though this solution is not a linear combination of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; though which completes our proof. &amp;lt;math&amp;gt;\blacksquare&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;*Now since &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; are continuous on an open interval &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; containing &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt;, such a solution &amp;lt;math&amp;gt;\phi(t)&amp;lt;/math&amp;gt; satisfies the initial conditions &amp;lt;math&amp;gt;y(t_0) = y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y'(t_0) = y'_0&amp;lt;/math&amp;gt;. Note though this solution is not a linear combination of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; though which completes our proof. &amp;lt;math&amp;gt;\blacksquare&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;	&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;	&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Theorem 1 above implies that if we can find two solutions &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; for which the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2) \neq 0&amp;lt;/math&amp;gt;, then for constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;, all solutions of the second order linear homogenous differential equation &amp;lt;math&amp;gt;\frac{d^2 y}{dt^2} + p(t) \frac{dy}{dt} + q(t) y = 0&amp;lt;/math&amp;gt; are given by:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Theorem 1 above implies that if we can find two solutions &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; for which the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2) \neq 0&amp;lt;/math&amp;gt;, then for constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;, all solutions of the second order linear homogenous differential equation &amp;lt;math&amp;gt;\frac{d^2 y}{dt^2} + p(t) \frac{dy}{dt} + q(t) y = 0&amp;lt;/math&amp;gt; are given by:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \quad y = Cy_1(t) + Dy_2(t) \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \quad y = Cy_1(t) + Dy_2(t) \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Also note that thus far we have not said that &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; need to be distinct. However, with the Theorem above, we see that if &amp;lt;math&amp;gt;y_1(t) = y_2(t)&amp;lt;/math&amp;gt; then the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2) = W(y_1, y_1) = W(y_2, y_2)&amp;lt;/math&amp;gt; is zero (as you should verify) and so not all solutions to a second order linear homogenous differential are given by the linear combination of just &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Also note that thus far we have not said that &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; need to be distinct. However, with the Theorem above, we see that if &amp;lt;math&amp;gt;y_1(t) = y_2(t)&amp;lt;/math&amp;gt; then the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2) = W(y_1, y_1) = W(y_2, y_2)&amp;lt;/math&amp;gt; is zero (as you should verify) and so not all solutions to a second order linear homogenous differential are given by the linear combination of just &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l41&quot; &gt;Line 41:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 45:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \quad W(y_1, y_2) \bigg|_{t_0} = \begin{vmatrix} y_1(t_0) &amp;amp; y_2(t_0) \\ y_1'(t_0) &amp;amp; y_2'(t_0)\end{vmatrix} = \begin{vmatrix} 1 &amp;amp;a 0\\ 0 &amp;amp; 1 \end{vmatrix} = 1 \neq 0 \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \quad W(y_1, y_2) \bigg|_{t_0} = \begin{vmatrix} y_1(t_0) &amp;amp; y_2(t_0) \\ y_1'(t_0) &amp;amp; y_2'(t_0)\end{vmatrix} = \begin{vmatrix} 1 &amp;amp;a 0\\ 0 &amp;amp; 1 \end{vmatrix} = 1 \neq 0 \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Thus Theorem 1 implies that ALL solutions to this differential equation are given by &amp;lt;math&amp;gt;y = Cy_1(t) + Dy_2(t)&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt; are constants. Thus &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; form a fundamental set of solutions for this differential equation. &amp;lt;math&amp;gt;\blacksquare&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Thus Theorem 1 implies that ALL solutions to this differential equation are given by &amp;lt;math&amp;gt;y = Cy_1(t) + Dy_2(t)&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt; are constants. Thus &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; form a fundamental set of solutions for this differential equation. &amp;lt;math&amp;gt;\blacksquare&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l47&quot; &gt;Line 47:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 52:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Licensing ==  &lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Licensing ==  &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Content obtained and/or adapted from:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Content obtained and/or adapted from:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [] under a CC BY-SA license&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;http://mathonline.wikidot.com/fundamental-solutions-to-linear-homogenous-differential-equa Fundamental Solutions to Linear Homogenous Differential Equations, mathonline.wikidot.com&lt;/ins&gt;] under a CC BY-SA license&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Khanh</name></author>
		
	</entry>
	<entry>
		<id>https://mathresearch.utsa.edu/wiki/index.php?title=Solutions_of_Linear_Systems&amp;diff=4040&amp;oldid=prev</id>
		<title>Khanh: Created page with &quot;==Fundamental Solutions to Linear Homogenous Differential Equations==  &lt;blockquote style=&quot;background: white; border: 1px solid black; padding: 1em;&quot;&gt;  :'''Theorem 1:''' Let &lt;m...&quot;</title>
		<link rel="alternate" type="text/html" href="https://mathresearch.utsa.edu/wiki/index.php?title=Solutions_of_Linear_Systems&amp;diff=4040&amp;oldid=prev"/>
		<updated>2021-11-19T06:27:44Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;==Fundamental Solutions to Linear Homogenous Differential Equations==  &amp;lt;blockquote style=&amp;quot;background: white; border: 1px solid black; padding: 1em;&amp;quot;&amp;gt;  :&amp;#039;&amp;#039;&amp;#039;Theorem 1:&amp;#039;&amp;#039;&amp;#039; Let &amp;lt;m...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;==Fundamental Solutions to Linear Homogenous Differential Equations==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;blockquote style=&amp;quot;background: white; border: 1px solid black; padding: 1em;&amp;quot;&amp;gt; &lt;br /&gt;
:'''Theorem 1:''' Let &amp;lt;math&amp;gt;\frac{d^2 y}{dt^2} + p(t) \frac{dy}{dt} + q(t)y = 0&amp;lt;/math&amp;gt; be a second order linear homogenous differential equation where &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; are continuous on an open interval &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; such that &amp;lt;math&amp;gt;t_0 \in I&amp;lt;/math&amp;gt;, and let &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; be two solutions to this differential equation. The set of all linear combinations of these two solutions, &amp;lt;math&amp;gt;y = Cy_1(t) + Dy_2(t)&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt; are constants contains all solutions to this differential equation if and only if there exists a point &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; for which the Wronksian of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; at &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; is nonzero, that is &amp;lt;math&amp;gt;W(y_1, y_2) \bigg|_{t_0} \neq 0&amp;lt;/math&amp;gt;.&lt;br /&gt;
&amp;lt;/blockquote&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* '''Proof:''' Let &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; both be solutions to the differential equation &amp;lt;math&amp;gt;\frac{d^2 y}{dt^2} + p(t) \frac{dy}{dt} + q(t)y = 0&amp;lt;/math&amp;gt; and suppose that &amp;lt;math&amp;gt;y = \phi (t)&amp;lt;/math&amp;gt; is any arbitrary solution as well. We want to show that &amp;lt;math&amp;gt;\phi (t)&amp;lt;/math&amp;gt; is a linear combination of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; for some constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
*&amp;lt;math&amp;gt;\Leftarrow&amp;lt;/math&amp;gt; Let &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; be such that the Wronskian of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; evaluated at &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; is nonzero, that is:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \quad W(y_1, y_2) \bigg|_{t_0} \neq 0 \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
* Take this value &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; and evaluate both &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\phi'&amp;lt;/math&amp;gt; at this point. Then &amp;lt;math&amp;gt;\phi (t_0) = y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\phi'(t_0) = y'_0&amp;lt;/math&amp;gt; (since &amp;lt;math&amp;gt;y = \phi(t)&amp;lt;/math&amp;gt; is a solution to our differential equation). Now consider the initial value problem &amp;lt;math&amp;gt;\frac{d^2 y}{dt^2} + p(t) \frac{dy}{dt} + q(t) y = 0&amp;lt;/math&amp;gt; with the initial conditions &amp;lt;math&amp;gt;y(t_0) = y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y'(t_0) = y'_0&amp;lt;/math&amp;gt;. The function &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; satisfies this differential equation. Since &amp;lt;math&amp;gt;W(y_1, y_2) \bigg|_{t_0} \neq 0&amp;lt;/math&amp;gt; then we have that there exists constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt; such that &amp;lt;math&amp;gt;y = Cy_1(t) + Dy_2(t)&amp;lt;/math&amp;gt; satisfies this initial value problem. But since &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; are continuous on the open interval &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; containing &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; then this implies that a unique solution exists, and so:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \phi(t) = Cy_1(t) + Dy_2(t) \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* So all solutions for this differential equation are a linear combination of the solutions &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
* &amp;lt;math&amp;gt;\Rightarrow&amp;lt;/math&amp;gt; Suppose that every point &amp;lt;math&amp;gt;t_0 \in I&amp;lt;/math&amp;gt; is such that &amp;lt;math&amp;gt;W(y_1, y_2) \bigg|_{t_0} = 0&amp;lt;/math&amp;gt;, that is, there exists no point &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; on &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; where the Wronskian of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; evaluated at &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt; is nonzero. Let &amp;lt;math&amp;gt;y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y'_0&amp;lt;/math&amp;gt; be values for which the system &amp;lt;math&amp;gt;\left\{\begin{matrix} Cy_1(t_0) + Dy_2(t_0) = y_0 \\ Cy_1'(t_0) + Dy_2'(t_0) = y'_0 \end{matrix}\right.&amp;lt;/math&amp;gt; has no solutions for a set of constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;.&lt;br /&gt;
	&lt;br /&gt;
*Now since &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; are continuous on an open interval &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; containing &amp;lt;math&amp;gt;t_0&amp;lt;/math&amp;gt;, such a solution &amp;lt;math&amp;gt;\phi(t)&amp;lt;/math&amp;gt; satisfies the initial conditions &amp;lt;math&amp;gt;y(t_0) = y_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y'(t_0) = y'_0&amp;lt;/math&amp;gt;. Note though this solution is not a linear combination of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; though which completes our proof. &amp;lt;math&amp;gt;\blacksquare&amp;lt;/math&amp;gt;&lt;br /&gt;
	&lt;br /&gt;
Theorem 1 above implies that if we can find two solutions &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; for which the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2) \neq 0&amp;lt;/math&amp;gt;, then for constants &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;, all solutions of the second order linear homogenous differential equation &amp;lt;math&amp;gt;\frac{d^2 y}{dt^2} + p(t) \frac{dy}{dt} + q(t) y = 0&amp;lt;/math&amp;gt; are given by:&lt;br /&gt;
&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \quad y = Cy_1(t) + Dy_2(t) \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Also note that thus far we have not said that &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; need to be distinct. However, with the Theorem above, we see that if &amp;lt;math&amp;gt;y_1(t) = y_2(t)&amp;lt;/math&amp;gt; then the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2) = W(y_1, y_1) = W(y_2, y_2)&amp;lt;/math&amp;gt; is zero (as you should verify) and so not all solutions to a second order linear homogenous differential are given by the linear combination of just &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;blockquote style=&amp;quot;background: white; border: 1px solid black; padding: 1em;&amp;quot;&amp;gt; &lt;br /&gt;
:'''Definition:''' Let &amp;lt;math&amp;gt;\frac{d^2 y}{dt^2} + p(t) \frac{dy}{dt} + q(t)y = 0&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; are continuous on an open interval &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; such that &amp;lt;math&amp;gt;t_0 \in I&amp;lt;/math&amp;gt; and let &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; be solutions to this differential equation. If the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2) \neq 0&amp;lt;/math&amp;gt; then the set of linear combinations of &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; is known as the '''Fundamental Set of Solutions''' to this differential equation.&lt;br /&gt;
&amp;lt;/blockquote&amp;gt;&lt;br /&gt;
&lt;br /&gt;
From the definition above, we see that if we can find two solutions &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; for which the Wronskian &amp;lt;math&amp;gt;W(y_1, y_2)&amp;lt;/math&amp;gt; is nonzero, then &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; form a fundamental set of solutions. The next question that we might pose is whether or not a second order linear homogenous differential equation always has a fundamental set of solutions.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;blockquote style=&amp;quot;background: white; border: 1px solid black; padding: 1em;&amp;quot;&amp;gt; &lt;br /&gt;
:'''Theorem 2:''' Let &amp;lt;math&amp;gt;\frac{d^2 y}{dt} + p(t) \frac{dy}{dt} + q(t) y = 0&amp;lt;/math&amp;gt; be a second order linear homogenous differential equation where &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; are continuous on an open interval &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; such that &amp;lt;math&amp;gt;t_0 \in I&amp;lt;/math&amp;gt;. If &amp;lt;math&amp;gt;y = y_1(t)&amp;lt;/math&amp;gt; is a solution to this differential equation that satisfies the initial conditions &amp;lt;math&amp;gt;y_1(t_0) = 1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_1'(t_0) = 0&amp;lt;/math&amp;gt;, and if &amp;lt;math&amp;gt;y = y_2(t)&amp;lt;/math&amp;gt; be a solution to this differential equation that satisfies the initial conditions &amp;lt;math&amp;gt;y_2(t_0) = 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2'(t_0) = 1&amp;lt;/math&amp;gt;. Then &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; form a fundamental set of solutions for this differential equation.&lt;br /&gt;
&amp;lt;/blockquote&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*'''Proof:''' We note that:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt;\begin{align} \quad W(y_1, y_2) \bigg|_{t_0} = \begin{vmatrix} y_1(t_0) &amp;amp; y_2(t_0) \\ y_1'(t_0) &amp;amp; y_2'(t_0)\end{vmatrix} = \begin{vmatrix} 1 &amp;amp;a 0\\ 0 &amp;amp; 1 \end{vmatrix} = 1 \neq 0 \end{align}&amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Thus Theorem 1 implies that ALL solutions to this differential equation are given by &amp;lt;math&amp;gt;y = Cy_1(t) + Dy_2(t)&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt; are constants. Thus &amp;lt;math&amp;gt;y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y_2&amp;lt;/math&amp;gt; form a fundamental set of solutions for this differential equation. &amp;lt;math&amp;gt;\blacksquare&amp;lt;/math&amp;gt;&lt;br /&gt;
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== Licensing == &lt;br /&gt;
Content obtained and/or adapted from:&lt;br /&gt;
* [] under a CC BY-SA license&lt;/div&gt;</summary>
		<author><name>Khanh</name></author>
		
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