diff --git a/src/pages/about/docs.astro b/src/pages/about/docs.astro
index b4edb2bd..0d94535e 100644
--- a/src/pages/about/docs.astro
+++ b/src/pages/about/docs.astro
@@ -78,6 +78,8 @@ import Slideshow from "../../components/Slideshow.astro";
             <ul class='list-group list-group-flush py-0'>
                 <li class='list-group-item py-0'><a class='text-decoration-none subsubsection' href='#same-page'> Within </a></li>
                 <li class='list-group-item py-0'><a class='text-decoration-none subsubsection' href='#int-page'> MechRef </a></li>
+                <li class = 'list-group-item py-0'><a class = 'text-decoration-none subsubsection' href = '#links_to_warnings'>Links to warnings</a></li>
+                <li class = 'list-group-item py-0'><a class = 'text-decoration-none subsubsection' href = '#links_to_examples'>Links to examples</a></li>
                 <li class='list-group-item py-0'><a class='text-decoration-none subsubsection' href='#ext-page'> External </a></li>
                 <li class='list-group-item py-0'><a class='text-decoration-none subsubsection' href='#ext-video'> Video </a></li>
             </ul>
@@ -844,6 +846,38 @@ All titles should be done in sentence case.
 
 </SubSubSection> 
 
+    <SubSubSection title = "Links to Warnings" id = "links_to_warnings">
+        <p>
+            Tag type: Warning
+        </p>
+        Options:
+        <ul>
+            <li>href: insert the id of the warning you want to link to after '#warning_'.</li>
+        </ul>
+        Example:
+        <CodeBox language = "html" code = `<a href = "/xxx/CoursePage#warning_id">TEXT</a>`/>
+        <a href = "/dyn/vectors#warning_rvv-wl">TEXT</a>
+        <p>
+            <em>*For demonstration purposes, this links to a warning in the vectors page in dynamics.</em>
+        </p>
+    </SubSubSection>
+
+    <SubSubSection title = "Links to Examples" id = "links_to_examples">
+        <p>
+            Tag type: Example
+        </p>
+        Options:
+        <ul>
+            <li>href: insert the id of the example you want to link to after '#example_btn_'.</li>
+        </ul>
+        Example:
+        <CodeBox language = "html" code = `<a href = "/xxx/CoursePage#example_btn_id">TEXT</a>`/>
+        <a href = "/dyn/vectors#example_btn_rvv-xn">TEXT</a>
+        <p>
+            <em>*For demonstration purposes, this links to an example in the vectors page in dynamics.</em>
+        </p>
+    </SubSubSection>
+
 <SubSubSection title="External page" id="ext-page">
 
     <p>Tag type: Regular</p>
diff --git a/src/pages/dyn/work_and_energy.astro b/src/pages/dyn/work_and_energy.astro
index 030119f0..c57748bb 100644
--- a/src/pages/dyn/work_and_energy.astro
+++ b/src/pages/dyn/work_and_energy.astro
@@ -59,7 +59,7 @@ import Col from "../../components/Col.astro"
 
 <DisplayEquation equation="\\begin{aligned}\\vec{F} &amp;= -\\nabla V \\\\&amp; = -\\frac{\\partial V}{\\partial x}\\hat{\\imath} -\\frac{\\partial V}{\\partial y}\\hat{\\jmath} - \\frac{\\partial V}{\\partial z}\\hat{k}\\end{aligned}" id="ren-efp" title="Force and potential energy." background="True" derivation="True">
 	<p>
-		Beginning with <a href="#ren-ec">#ren-ec</a> and generalizing it to one-dimensional displacement in the y-direction, the equation becomes:
+		Beginning with <a href="#ren-wc">#ren-wc</a> and generalizing it to one-dimensional displacement in the y-direction, the equation becomes:
 		<DisplayEquation equation="\\begin{aligned}		W &amp;= \\vec{F} \\cdot \\Delta{\\vec{y}}		\\end{aligned}" />
 
 	</p>
@@ -105,7 +105,7 @@ import Col from "../../components/Col.astro"
 
 		  </p>
 		  <p>
-			Since gravity only acts in one direction, we can simplify <a href="ren-efp">#ren-efp</a> to:
+			Since gravity only acts in one direction, we can simplify <a href="#ren-efp">#ren-efp</a> to:
 			<DisplayEquation equation="\\begin{aligned}			F &amp;= -\\frac{dV}{dy} \\\\			-mg &amp;= -\\frac{dV}{dy} \\\\			mg \\, dy &amp;= dV \\\\			\\end{aligned}" />
 
 		  </p>
@@ -141,7 +141,7 @@ import Col from "../../components/Col.astro"
 
 		  </p>
 		  <p>
-			Since the restoring force in a spring only acts in one direction, we can simplify <a href="ren-efp">#ren-efp</a> to:
+			Since the restoring force in a spring only acts in one direction, we can simplify <a href="#ren-efp">#ren-efp</a> to:
 			<DisplayEquation equation="\\begin{aligned}			F &amp;= -\\frac{dV}{dx} \\\\			-kx &amp;= -\\frac{dV}{dx} \\\\			kx \\, dx &amp;= dV \\\\			\\end{aligned}" />
 
 		  </p>
@@ -238,12 +238,12 @@ import Col from "../../components/Col.astro"
 
 	</p>
 	<p>
-		Using conservation of energy, and the fact that a vector dotted with itself equals its magnitude squared (see <a href="rvi.html#rvi-eg">#rvi-eg</a>), then:
+		Using conservation of energy, and the fact that a vector dotted with itself equals its magnitude squared (see <a href="/dyn/vector_calculus#rvi-eg">#rvi-eg</a>), then:
 		<DisplayEquation equation="\\begin{aligned}		T &amp; = \\frac{1}{2}mv^2\\\\		\\end{aligned}" />
 
 	</p>
 	<p>
-		Another perhaps less intuitive way is to begin with the work definition <a href="#ren-ef">#ren-ef</a>:
+		Another perhaps less intuitive way is to begin with the work definition <a href="#ren-wf">#ren-wf</a>:
 		<DisplayEquation equation="\\begin{aligned}		W &amp;= \\int_{\\vec{r}_1}^{\\vec{r}_2} \\vec{F} \\cdot d\\vec{r} \\\\		&amp; = \\int_{t_1}^{t_2} \\vec{F} \\cdot \\dot{\\vec{r}}dt \\\\ 		&amp; = \\int_{t_1}^{t_2} \\vec{F} \\cdot \\vec{v} \\, dt		\\end{aligned}" />
 
 	</p>
@@ -290,14 +290,14 @@ import Col from "../../components/Col.astro"
 
 <DisplayEquation id="ren-ea" equation="T = \\frac{1}{2} m v_Q^2 + m \\vec{v}_Q \\cdot \\left( \\vec\\omega \\times \\vec{r}_{QC} \\right) + \\frac{1}{2} I_{Q,\\hat\\omega} \\omega^2" title="Kinetic energy of a rigid body about an arbitrary body point \\(Q\\)." background="True" derivation="true">
 	<p>
-		We start with the general expression <a href="#rem-eb">#rem-eb</a>:
+		We start with the general expression <a href="/dyn/geometric_properties#rem-eb">#rem-eb</a>:
 
 		<DisplayEquation equation="\\begin{aligned}		T &amp;= \\iiint_{\\mathcal{B}} \\frac{1}{2} \\rho v_P^2 \\, dV,		\\end{aligned}" />
 
 
 		where we integrate over the body with a location \(P\). We
 		choose a point \(Q\) fixed to the body and
-		use <a href="rkg.html#rkg-er">#rkg-er</a> to express the
+		use <a href="/dyn/rigid_body_kinematics#rkg-er">#rkg-er</a> to express the
 		velocity of \(P\) in terms of <InlineEquation equation="\\vec{v}_Q" /> and
 		\(\vec\omega\), giving
 
@@ -317,7 +317,7 @@ import Col from "../../components/Col.astro"
 		orthogonal distance to point \(P\) from the line through
 		\(Q\) in direction <InlineEquation equation="\\vec\\omega" />
 		, so
-		from <a href="rem.html#rem-ei">#rem-ei</a> we see that
+		from <a href="/dyn/geometric_properties#rem-ei">#rem-ei</a> we see that
 		the final integral above is the moment of inertia
 		<InlineEquation equation="I_{Q,\\hat\\omega}" />
   about the  axis through
@@ -327,13 +327,13 @@ import Col from "../../components/Col.astro"
 
 <DisplayEquation id="ren-wk" equation="W = \\Delta T" title="Work-kinetic energy theorem." background="True" derivation="true">
 	<p>
-		Skipping the derivation shown in <a href="#ren-ep">#ren-ep</a>, taking the last step with the integral:
+		Skipping the derivation shown in <a href="#ren-ek">#ren-ek</a>, taking the last step with the integral:
 		<DisplayEquation equation="\\begin{aligned}		\\int dW &amp; = \\int_{\\vec{v_1}}^{\\vec{v_2}}m\\vec{v} \\, d\\vec{v} \\\\		W &amp; = \\frac{1}{2}m\\left[\\vec{v} \\cdot \\vec{v}\\right]_{\\vec{v_1}}^{\\vec{v_2}} \\\\		&amp; = \\Delta T		\\end{aligned}" />
 	</p>
 </DisplayEquation>
 
 <DisplayEquationCustom id="ren-eco" title="Work-energy theorem." background="True">
-	<DisplayEquation equation="W = \Delta T + \Delta V"/>
+	<DisplayEquation equation="W = \\Delta T + \\Delta V"/>
 	<p>
 		where \(W\) is the work done by non-conservative forces. If non-conservative forces are not present, then
 		it becomes conservation of energy.
@@ -405,7 +405,7 @@ import Col from "../../components/Col.astro"
 		</div>
 	</DisplayEquationCustom>
 
-	<DisplayEquationCustom id="ren-wm" title="Work done by a moment \\(M\\)." background="True" derivation="true">
+	<DisplayEquationCustom id="ren-wm" title="Work done by a moment \\(M\\)." background="True">
 		<DisplayEquation equation="\\begin{aligned}W &amp;= \\int_{\\theta_1}^{\\theta_2} M \\, d\\theta \\\\&amp; = \\int_{t_1}^{t_2} M \\dot\\theta \\, dt \\\\&amp;= M \\, \\Delta \\theta \\text{ (for constant M)}\\end{aligned}" />
 		<p>
 			The rotation angle \(\theta\) is measured around the same
@@ -463,7 +463,7 @@ import Col from "../../components/Col.astro"
 
 <p> Work done by friction can be positive, zero, or negative. </p>
 
-	<Example id="wdf-rws" title="Friction during rolling wihtout slip." solution=True>
+	<Example id="wdf-rws" title="Friction during rolling without slip." solution=True>
     <div>
 	  <Image src="/dyn/work_and_energy/WorkForce_example2.png" width="10"></Image>
 	  <ol> 
@@ -501,7 +501,7 @@ import Col from "../../components/Col.astro"
     
 <SubSubSection title="Work done by a moment"  id="work_moment">
 
-<DisplayEquation equation=" W = \\int_{\\theta_0}^{\\theta_f} M_z \\,d\\theta = \\int_{t_0}^{t_f} M_z \\ \\dot{\\theta} \\,d\\theta " background="True"  id="wan-wm"> </DisplayEquation>
+<DisplayEquation equation=" W = \\int_{\\theta_0}^{\\theta_f} M_z \\,d\\theta = \\int_{t_0}^{t_f} M_z \\ \\dot{\\theta} \\,dt" background="True"  id="wan-wm"> </DisplayEquation>
 
 	<Example id="wdm-rm" title="Rod with friction moment." solution=True>
     <div>
@@ -608,4 +608,4 @@ import Col from "../../components/Col.astro"
 
 </Layout>
 
-<script src="/dyn/work_and_energy/canvases.js" is:inline></script>
\ No newline at end of file
+<script src="/dyn/work_and_energy/canvases.js" is:inline></script>