diff --git a/public_html/assets/css/main.css b/public_html/assets/css/main.css
index 9b63a56..8bad004 100644
--- a/public_html/assets/css/main.css
+++ b/public_html/assets/css/main.css
@@ -1846,7 +1846,7 @@ header h6+p {
 
 header.major {
     text-align: center;
-    margin-top: 4em;
+    margin-top: 8em;
 }
 
 header.major h1,
diff --git a/public_html/circuitos.html b/public_html/circuitos.html
index 9694094..e0d751a 100644
--- a/public_html/circuitos.html
+++ b/public_html/circuitos.html
@@ -65,6 +65,38 @@
                     <h2>Corriente Alterna</h2>
                 </header>
                 <section>
+                    <p></p>
+                    <p>Corriente alterna (abreviada CA en español y AC en inglés, de alternating current) se denomina a la corriente
+                        eléctrica en la que la magnitud y el sentido varían cíclicamente.</p>
+                    <p>La forma de oscilación de la corriente alterna más comúnmente utilizada es la oscilación senoidal (sinusoidal
+                        en inglés) ​con la que se consigue una transmisión más eficiente de la energía, a tal punto que al
+                        hablar de corriente alterna se sobrentiende que se refiere a la corriente alterna senoidal.</p>
+                    </p>
+                    <img class="symbol" src="images/Corriente_Alterna.png" height="240" />
+                    <p>Sin embargo, en ciertas aplicaciones se utilizan otras formas de oscilación periódicas, tales como la
+                        triangular o la cuadrada.</p>
+                    <p>Utilizada genéricamente, la CA se refiere a la forma en la cual la electricidad llega a los hogares y
+                        a las industrias. Sin embargo, las señales de audio y de radio transmitidas por los cables eléctricos,
+                        son también ejemplos de corriente alterna. En estos usos, el fin más importante suele ser la transmisión
+                        y recuperación de la información codificada (o modulada) sobre la señal de la CA.</p>
+                    <p>Algunos tipos de oscilaciones periódicas tienen el inconveniente de no tener definida su expresión matemática,
+                        por lo que no se puede operar analíticamente con ellas. Por el contrario, la oscilación sinusoidal
+                        no tiene esta indeterminación matemática y presenta las siguientes ventajas:</p>
+                    <ol>
+                        <li>La función seno está perfectamente definida mediante su expresión analítica y gráfica. Mediante la
+                            teoría de los números complejos se analizan con suma facilidad los circuitos de alterna.</li>
+                        <li>Las oscilaciones periódicas no sinusoidales se pueden descomponer en suma de una serie de oscilaciones
+                            sinusoidales de diferentes frecuencias que reciben el nombre de armónicos. Esto es una aplicación
+                            directa de las series de Fourier.</li>
+                        <li>Se pueden generar con facilidad y en magnitudes de valores elevados para facilitar el transporte
+                            de la energía eléctrica.</li>
+                        <li>Su transformación en otras oscilaciones de distinta magnitud se consigue con facilidad mediante la
+                            utilización de transformadores.</li>
+                    </ol>
+                    <h4>Potencia en C.A</h4>
+                    <img class="symbol" src="images/symbols/Corriente_Alterna_01.png" height="30" />
+                    <h4>Impedancia</h4>
+                    <img class="symbol" src="images/symbols/Corriente_Alterna_02.png" height="120" />
                 </section>
             </div>
         </div>
@@ -81,7 +113,21 @@
                     <h2>Corriente Continua</h2>
                 </header>
                 <section>
-
+                    <p>La corriente continua (abreviada CD en español y DC en inglés, de direct current) se refiere al flujo
+                        continuo de carga eléctrica a través de un conductor entre dos puntos de distinto potencial y carga
+                        eléctrica, que no cambia de sentido con el tiempo.​ A diferencia de la corriente alterna, en la corriente
+                        continua las cargas eléctricas circulan siempre en la misma dirección.</p>
+                    <img class="symbol" src="images/Corriente_Continua_01.png" height="240" />
+                    <p>Aunque comúnmente se identifica la corriente continua con una corriente constante, es continua toda corriente
+                        que mantenga siempre la misma polaridad, así disminuya su intensidad conforme se va consumiendo la
+                        carga (por ejemplo cuando se descarga una batería eléctrica).</p>
+                    <img class="symbol" src="images/Corriente_Continua_02.png" height="240" />
+                    <img class="symbol" src="images/Corriente_Continua_03.png" height="240" />
+                    <p>También se dice corriente continua cuando los electrones se mueven siempre en el mismo sentido, el flujo
+                        se denomina corriente continua y va (por convenio) del polo positivo al negativo.</p>
+                    <p>Los cálculos de circuitos de corriente continua se realizan respectivamente aplicando las leyes de Ohm,
+                        leyes de Kirchhoff, circuitos delta y estrella, teoremas de mallas y nodos, teorema de superposición,
+                        y ley de Thevenin y Norton.</p>
                 </section>
             </div>
         </div>
@@ -98,7 +144,36 @@
                     <h2>Bobinas</h2>
                 </header>
                 <section>
+                    <header id="tema3.1">
+                        <h4>Definición</h4>
+                    </header>
+                    <p>Un inductor, bobina o reactor es un componente pasivo de un circuito eléctrico que, debido al fenómeno
+                        de la autoinducción, almacena energía en forma de campo magnético.</p>
+                    <img class="symbol" src="images/bobina01.jpg" height="180" />
 
+                    <header id="tema3.2">
+                        <h4>Construcción</h4>
+                    </header>
+                    <p>Un inductor está constituido normalmente por una bobina de conductor, típicamente alambre o hilo de cobre
+                        esmaltado. Existen inductores con núcleo de aire o con núcleo hecho de material ferroso (por ejemplo,
+                        acero magnético), para incrementar su capacidad de magnetismo.
+                    </p>
+                    <img class="symbol" src="images/bobina03.jpg" height="180" />
+
+                    <header id="tema3.3">
+                        <h4>Funcionamiento</h4>
+                    </header>
+                    <p>La bobina almacena energía en forma de campo magnético cuando aumenta la intensidad de corriente, devolviéndola
+                        cuando ésta disminuye.</p>
+                    <img class="symbol" src="images/bobina02.jpg" height="180" />
+                    <header id="tema3.4">
+                        <h4>Voltaje y Corriente a través de una Bobina</h4>
+                    </header>
+                    <p> Matemáticamente se puede demostrar que la energía U, almacenada por una bobina con inductancia L, que
+                        es recorrida por una corriente de intensidad I, viene dada por:</p>
+                    <img class="symbol" src="images/symbols/Bobinas_01.png" height="120" />
+                    <p>Y la Corriente viene dada por:</p>
+                    <img class="symbol" src="images/symbols/Bobinas_02.png" height="90" />
                 </section>
             </div>
         </div>
@@ -175,6 +250,7 @@
                 <header class="major">
                     <h2>Circuitos Transitorios</h2>
                 </header>
+
                 <section>
                     <header class="major">
                         <h3>Circuitos RC</h3>
@@ -184,7 +260,7 @@
                         al bloquear ciertas frecuencias y permitir otras.</p>
                     <p>El Circuito RC mas simple es un Capacitor cargado y una Resistencia conectadas entre ellas, el Capacitor
                         va a descargar creando un voltaje, este valor depende del tiempo y se reduce hasta llegar a 0</p>
-                    <img class="symbol" src="images/symbols/Discharging_capacitor.svg" height="360" />
+                    <img class="symbol" src="images/symbols/Discharging_capacitor.svg" height="240" />
                     <header id="tema4.1.1">
                         <h4>Voltaje en el Circuito</h4>
                     </header>
@@ -193,22 +269,22 @@
                         <a href="#tema4.4">tema anterior</a>
                         la corriente que atravesara el Capacitor variara con el tiempo, y deducimos que:
                     </p>
-                    <img class="symbol" src="images/symbols/Circuito_RC_01.svg" height="120" />
+                    <img class="symbol" src="images/symbols/Circuito_RC_01.svg" height="90" />
                     <p>Al despejar el Voltaje obtenemos la formula de la Caída Exponencial, Si V0 es el Voltaje inicial del
                         Capacitor
                     </p>
-                    <img class="symbol" src="images/symbols/Circuito_RC_02.svg" height="120" />
+                    <img class="symbol" src="images/symbols/Circuito_RC_02.svg" height="80" />
                     <p>Ademas, el tiempo requerido para que el voltaje disminuya a un 1/e de su valor inicial, se conoce como
                         la Constante de Tiempo RC, y esta definida por:
                     </p>
-                    <img class="symbol" src="images/symbols/Circuito_RC_03.svg" height="90" />
+                    <img class="symbol" src="images/symbols/Circuito_RC_03.svg" height="50" />
                 </section>
 
                 <section>
                     <header class="major">
                         <h3>Circuitos RL</h3>
                     </header>
-                    <p></p>
+                    <img class="symbol" src="images/RL_Series.png" height="180" />
                     <p>Es un Circuito compuesto por Inductores y Resistencias en serie. Se pueden usar para filtrar una señal,
                         específicamente los circuitos de Respuesta Infinita al Impulso esta compuesto de una sola Resistencia
                         con un Inductor</p>
@@ -224,14 +300,65 @@
                         <a href="#tema3.4">tema anterior</a> y en simetría con los
                         <a href="#tema4.1.1">Circuitos RC</a> la corriente que generara el Inductor esta dada por:
                     </p>
-                    <img class="symbol" src="images/symbols/Circuito_RL_01.svg" height="120" />
+                    <img class="symbol" src="images/symbols/Circuito_RL_01.svg" height="80" />
                     <p>Definiendo la Constante de Tiempo RL como:
                     </p>
-                    <img class="symbol" src="images/symbols/Circuito_RL_02.svg" height="120" />
+                    <img class="symbol" src="images/symbols/Circuito_RL_02.svg" height="100" />
                     <p>Por lo que terminamos con:
                     </p>
-                    <img class="symbol" src="images/symbols/Circuito_RL_03.svg" height="120" />
+                    <img class="symbol" src="images/symbols/Circuito_RL_03.svg" height="80" />
                 </section>
+
+                <section>
+                    <header class="major">
+                        <h3>Circuitos RLC</h3>
+                    </header>
+                    <p>Es un circuito eléctrico que consiste de una Resistencia (R), un Inductor (L) y un Condensador (C), conectados
+                        en serie o paralelo. Estos circuitos se caracterizan por su comportamiento de oscilador armónico,
+                        de la misma forma que un circuito LC, pero en la realidad no es posible obtener una resistencia de
+                        0 en un circuito fuera de la super conductividad</p>
+                    <img class="symbol" src="images/RLC_Series.jpg" height="120" />
+
+                    <header>
+                        <h4>Circuito LC</h4>
+                    </header>
+                    <p>Para entender mejor el funcionamiento de un circuito RLC es mejor examinar el caso ideal donde la resistencia
+                        es nula: un circuito LC</p>
+                    <img class="symbol" src="images/symbols/Circuito_LC.svg" height="180" />
+                    <p>Como se puede observer el comportamiento de los Inductores al oponerse a los cambios de de corriente,
+                        incluyendo su disminución, y la de los Capacitores de almacenar cargas eléctricas hasta cargarse
+                        y luego descargarse expulsando las cargas en sentido opuesto, causan un efecto de Oscilación</p>
+                    <img class="symbol" src="images/LC_Circuit.gif" height="180" />
+                    <p>El Capacitor cargado expulsaría electrones hasta que ambas capas estuvieran al mismo potencial, sin embargo
+                        el campo magnético del inductor retrasa la corriente al inicio, cuando esta es fuerte, manteniendo
+                        la diferencia de potencial, y al final cuando quedan pocas cargas en el negativo del capacitor, el
+                        campo magnético acumulado las empuja hasta el otro terminal, de forma que todas las cargas son transferidas
+                        de un terminal del Condensador al otro</p>
+                    <p>El funcionamiento de los Circuitos RLC es como esto pero obviamente con una Resistencia agregada, esta
+                        tendrá el efecto de disipar una parte de la energía en cada Oscilación, conocido como Amortiguamiento</p>
+
+                    <header>
+                        <h4>Circuito RLC en Serie</h4>
+                    </header>
+                    <img class="symbol" src="images/symbols/Circuito_RLC_Serie.svg" height="180" />
+                    <p>Para poder explicar funcionamiento del circuito primero es importante discutir las medidas frecuencia
+                        angular,
+                        <b>α</b> y
+                        <b>ω0</b>.
+                        <b>α</b> es la frecuencia neperiana o Atenuación, y es una medida de que tan rápido la respuesta del
+                        circuito morirá después de ser removido una fuente de estimulo.
+                        <b>ω0</b> es la frecuencia de resonancia angular. En un circuito en series estas están dadas por:</p>
+                    <img class="symbol" src="images/symbols/Resonancia_Atenuacion_Serie.svg" height="120" />
+                    <p>Definiendo a las raíces S como:</p>
+                    <img class="symbol" src="images/symbols/Raices_RLC.svg" height="120" />
+                    <p>Se puede calcular la formula para la Corriente en el circuito:</p>
+                    <img class="symbol" src="images/symbols/Corriente_RLC_Serie.svg" height="45" />
+                    <p>En donde los coeficientes A1 e A2 son dependientes del circuito y se calculan al realizar un sistema
+                        de ecuaciones con la formula resulta para el valor de la Corriente en el tiempo inicial y el que
+                        va atener después de un tiempo infinito</p>
+
+                </section>
+
             </div>
         </div>
     </section>
diff --git a/public_html/images/Corriente_Alterna.png b/public_html/images/Corriente_Alterna.png
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diff --git a/public_html/images/Corriente_Continua_01.png b/public_html/images/Corriente_Continua_01.png
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diff --git a/public_html/images/symbols/Bobinas_02.png b/public_html/images/symbols/Bobinas_02.png
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diff --git a/public_html/images/symbols/Circuito_LC.svg b/public_html/images/symbols/Circuito_LC.svg
new file mode 100644
index 0000000..dc71ac9
--- /dev/null
+++ b/public_html/images/symbols/Circuito_LC.svg
@@ -0,0 +1,45 @@
+
+
+<svg height="220" width="300" 
+    xmlns="http://www.w3.org/2000/svg" version="1.1">
+
+    <!-- wires -->
+
+    <polyline points="70,70 70,30 230,30 230,70" 
+        style="fill:none;stroke:black;stroke-width:2"/>
+
+    <polyline points="70,150 70,190 230,190 230,150" 
+        style="fill:none;stroke:black;stroke-width:2"/>
+
+
+    <!-- Electric current arrow and label -->
+
+    <polygon points="125,30 115,25 115,35" 
+        style="fill:black;stroke:black;stroke-width:1"/>
+
+    <text x="125" y="20" fill="black" font-size="18" style="font-family:Verdana;font-style:italic;">i</text>
+
+
+    <!-- Inductor -->
+    <path id="inductor" d="M 70 70  l 0 15   q -40 5 0 10   q -40 5 0 10   
+        q -40 5 0 10   q -40 5 0 10  q -40 5 0 10   l 0 15 "
+        stroke="black" stroke-width="2" fill="none" />
+
+    <text x="20" y="120" fill="black" font-size="24" style="font-family:Verdana">L</text>
+
+
+
+    <!-- Capacitor -->
+    <path id="capacitor" d="M 230 70 l 0 35   m -20 0   l 40 0    m 0 10  l -40 0  m 20 0 l 0 35 "
+        stroke="black" stroke-width="2" fill="none" />
+
+    <text x="260" y="120" fill="black" font-size="24" style="font-family:Verdana">C</text>
+
+    
+    <text x="140" y="50" fill="black" font-size="12" style="font-family:Verdana">+</text>
+    <text x="140" y="115" fill="black" font-size="18" style="font-family:Verdana;font-style:italic;">v</text>
+    <text x="140" y="180" fill="black" font-size="12" style="font-family:Verdana">-</text>
+	
+
+
+</svg>
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new file mode 100644
index 0000000..dac3145
--- /dev/null
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@@ -0,0 +1,269 @@
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