(Energy)
(Energy)
Line 4: Line 4:
 
<br><br><br><math> E = \int_{1}^{2} |3x|^2\ dt \!</math>
 
<br><br><br><math> E = \int_{1}^{2} |3x|^2\ dt \!</math>
  
<br><br><math> E = [3x]_{t=1}^{t=2}</math>
+
<br><br><math> E = [x]_{t=1}^{t=2}</math>
  
 
<br><br><br><math> E = 3(2)-3(1)</math>
 
<br><br><br><math> E = 3(2)-3(1)</math>
 
<br><br><br><math> E = 2</math>
 
<br><br><br><math> E = 2</math>
 
<br><br><br><math> E = 2</math>
 
<br><br><br><math> E = 2</math>

Revision as of 20:45, 4 September 2008

Energy

$ E = \int_{T2}^{T1} |x(t)|^2\ dt \! $


$ E = \int_{1}^{2} |3x|^2\ dt \! $



$ E = [x]_{t=1}^{t=2} $




$ E = 3(2)-3(1) $


$ E = 2 $


$ E = 2 $

Alumni Liaison

Abstract algebra continues the conceptual developments of linear algebra, on an even grander scale.

Dr. Paul Garrett