Maxwell's Equations - Revision history

DemasMa at 02:52, 6 April 2007

2007-04-06T02:52:00Z

2007-04-06T02:51:22Z

In the presence of charges and dielectric media

2007-04-06T02:46:44Z

In the presence of charges and dielectric media

2007-04-06T02:43:10Z

In the presence of charges and dielectric media

2007-04-06T02:41:28Z

In the presence of charges and dielectric media

2007-04-06T02:40:41Z

2007-04-06T02:39:30Z

In the presence of charges and dielectric media

2007-04-06T01:42:59Z

2007-03-21T15:46:03Z

In Free Space

2007-03-21T15:45:51Z

In Free Space

@@ Line 20: / Line 20: @@
 == In the Presence of Charges and Dielectric Media ==
 {|align=center
@@ Line 40: / Line 39: @@
 Where <math>\boldsymbol{D} = \epsilon_0 \boldsymbol{E}</math> and <math>\boldsymbol{B} = \mu_0 \boldsymbol{H}</math>.

@@ Line 19: / Line 19: @@
 |}
-== In the presence of charges and dielectric media ==
+== In the Presence of Charges and Dielectric Media ==
 <font color="red">Need to add possibly derivation of wave equation and definitely Maxwell's equation in presence.  Need also to introduce D and H and relate them to E and B.</font>

← Older revision		Revision as of 02:46, 6 April 2007
Line 38:		Line 38:
	\|}		\|}

−	Where <math>\boldsymbol{D} = \epsilon_0 \boldsymbol{E}</math> and <math>\boldsymbol{B} = \mu_0 \boldsymbol{H}</math>	+
		+	Where <math>\boldsymbol{D} = \epsilon_0 \boldsymbol{E}</math> and <math>\boldsymbol{B} = \mu_0 \boldsymbol{H}</math>.

← Older revision		Revision as of 02:43, 6 April 2007
Line 38:		Line 38:
	\|}		\|}

−	Where	+	Where <math>\boldsymbol{D} = \epsilon_0 \boldsymbol{E}</math> and <math>\boldsymbol{B} = \mu_0 \boldsymbol{H}</math>
−	<math>\boldsymbol{D} = \epsilon_0 \boldsymbol{E}</math>
−
−	<math>\boldsymbol{B} = \mu_0 \boldsymbol{H}</math>

@@ Line 38: / Line 38: @@
 |}
 <math>\boldsymbol{D} = \epsilon_0 \boldsymbol{E}</math>
 <math>\boldsymbol{B} = \mu_0 \boldsymbol{H}</math>

← Older revision		Revision as of 02:39, 6 April 2007
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	\|width="400"\|<math>\boldsymbol{\nabla \times H} - \frac{\partial \boldsymbol{D}}{\partial t}= \boldsymbol{j} </math>		\|width="400"\|<math>\boldsymbol{\nabla \times H} - \frac{\partial \boldsymbol{D}}{\partial t}= \boldsymbol{j} </math>
	\|}		\|}
		+
		+	<math>\boldsymbol{D = \epsilon_0 E}</math>
		+	<math>\boldsymbol{B = \mu_0 H}</math>

@@ Line 10: / Line 10: @@
 |<math>\boldsymbol{\nabla \cdot B} = 0</math>
 |-
-|height="50"|&nbsp;||&nbsp;
+|height="20"|&nbsp;||&nbsp;
 |-
 |Faradays's Law: