Changes

Jump to navigation Jump to search
no edit summary
Line 122: Line 122:     
The resistor voltage drop equations all take the form
 
The resistor voltage drop equations all take the form
: <math>\Delta V = IR</math>
+
: <math>\Delta V = IR\,\!</math>
 
or alternately
 
or alternately
: <math>V_\alpha - IR = V_\beta</math>.
+
: <math>V_\alpha - IR = V_\beta\,\!</math>.
 
They describe the voltage drop associated with current crossing a resistor, according to [http://en.wikipedia.org/wiki/Ohm's_law Ohm's Law].  As such, there is one equation per resistor in the circuit.
 
They describe the voltage drop associated with current crossing a resistor, according to [http://en.wikipedia.org/wiki/Ohm's_law Ohm's Law].  As such, there is one equation per resistor in the circuit.
   −
* <math>R_1</math>: <math>V_b - I_1 \!\cdot\! R_1 = V_1</math>
+
* R<sub>1</sub>: V<sub>b</sub> - I<sub>1</sub>R<sub>1</sub> = V<sub>1</sub>
* <math>R_2</math>: <math>V_2 - I_2 \!\cdot\! R_2 = 0</math>
+
* R<sub>2</sub>: V<sub>2</sub> - I<sub>2</sub>R<sub>2</sub> = 0
* <math>R_3</math>: <math>V_4 - I_3 \!\cdot\! R_3 = V_3</math>
+
* R<sub>3</sub>: V<sub>4</sub> - I<sub>3</sub>R<sub>3</sub> = V<sub>3</sub>
* <math>R_4</math>: <math>V_3 - I_4 \!\cdot\! R_4 = 0</math>
+
* R<sub>4</sub>: V<sub>3</sub> - I<sub>4</sub>R<sub>4</sub> = 0
* <math>R_5</math>: <math>V_5 - I_5 \!\cdot\! R_5 = V_4</math>
+
* R<sub>5</sub>: V<sub>5</sub> - I<sub>5</sub>R<sub>5</sub> = V<sub>4</sub>
* <math>R_6</math>: <math>V_c - I_6 \!\cdot\! R_6 = V_5</math>
+
* R<sub>6</sub>: V<sub>c</sub> - I<sub>6</sub>R<sub>6</sub> = V<sub>5</sub>
* <math>R_7</math>: <math>V_c - I_7 \!\cdot\! R_7 = V_7</math>
+
* R<sub>7</sub>: V<sub>c</sub> - I<sub>7</sub>R<sub>7</sub> = V<sub>7</sub>
* <math>R_t</math>: <math>V_{out} - I_t \!\cdot\! R_t = 0</math>
+
* R<sub>t</sub>: V<sub>out</sub> - I<sub>t</sub>R<sub>t</sub> = 0
    
=== Node charge flow ===
 
=== Node charge flow ===
461

edits

Navigation menu