Kirchhoff's Laws PHY 112 John Stahl Kalamazoo Valley Community College Example I1 I2 Problem: The circuit I3 A B shown has two loops. The current directions and the final branch current values are unknown. Use Kirchhoff's Voltage Loop rules, current rule, and Ohm’s law. Find: For the circuit shown find all the branch currents (I1, I2, I3). Equations π£=0 • By adding the voltages around each loop we get two equations. • Replace the resistors voltages with their Ohm’s law relationships. • The last equation is the current relationship at the top node. ππππ π£ = ππ 1 − ππ 3 + 12π£ − 6π£ = 0 ππππ π΄ π£ = −ππ 3 + ππ 2 + 12π£ − 9π£ = 0 ππππ π΅ π = πΌπ πΌ1 π 1 − πΌ3 π 3 = −6π£ −πΌ3 π 3 + πΌ2 π 2 = −3π£ 6πΌ1 − 5πΌ3 = −6π£ 10πΌ2 − 5πΌ3 = −3π£ πΌππ = πΌππ’π‘ πΌ1 +πΌ2 +πΌ3 = 0 Direct Substitution With Direct substitution each equitation is used to find a relationship between each variable. 6πΌ1 − 5πΌ3 = −6π£ Eq.1 10πΌ2 − 5πΌ3 = −3π£ Eq.2 πΌ1 +πΌ2 +πΌ3 = 0 Eq.3 πΈππ’ππ‘πππ 1 6πΌ1 − 5πΌ3 = −6π£ πΌ1 = The relationships are all placed into equation 3. Solve for I3. −6π£ + 5πΌ3 6 πΈππ’ππ‘πππ 2 10πΌ2 − 5πΌ3 = −3π£ Eq.2 πΌ2 = −3π£ + 5πΌ3 10 πΈππ’ππ‘πππ 3 πΌ1 + πΌ2 + πΌ3 = 0 −6π£ + 5πΌ3 −3π£ + 5πΌ3 + + πΌ3 = 0 6 10 Direct Substitution • Solve for I3. • Use the solution for I3 and solve for the other branch currents. • Check to make sure the sum of currents equal zero. −6π£ + 5πΌ3 −3π£ + 5πΌ3 + + πΌ3 = 0 6 10 5πΌ3 −3π£ 5πΌ3 1π£ + + + + πΌ3 = 0 6 10 10 2.333πΌ3 = 1.3 πΌ3 = 0.557π΄ πΌ1 = −6π£ + 5πΌ3 6 πΌ1 = −0.536A −3π£ + 5πΌ3 πΌ2 = 10 πΌ2 = −0.0214A −0.536A − 0.0214A + 0.557π΄ = 0 οΌ Matrix Method • Use the three equations and pad them with zeros where needed. • Separate the variables from the weights. • Take the inverse of the matrix on the left. • Taking the inverse of a 3x3 matrix is not a trivial task. 6πΌ1 + 0πΌ2 − 5πΌ3 = −6π£ Eq.1 0πΌ1 + 10πΌ2 − 5πΌ3 = −3π£ Eq.2 πΌ1 +πΌ2 +πΌ3 = 0 Eq.3 6 0 1 πΌ1 −6 0 −5 10 −5 × πΌ2 = −3 πΌ3 0 1 1 πΌ1 6 0 πΌ2 = 0 10 πΌ3 1 1 −5 −5 1 −1 −6 × −3 0 πΌ1 −0.536π΄ πΌ2 = −0.0214π΄ πΌ3 0.557π΄