Presentation on theme: "1 Gustav Kirchhoff 1824-1887 German Physicist. Circuit Definitions Node – any point where 2 or more circuit elements are connected together Wires usually."— Presentation transcript:
1 Gustav Kirchhoff German Physicist
Circuit Definitions Node – any point where 2 or more circuit elements are connected together Wires usually have negligible resistance Each node has one voltage (w.r.t. ground) Branch – a circuit element between two nodes Loop – a collection of branches that form a closed path returning to the same node without going through any other nodes or branches twice
Problem-Solving Strategy Applying Kirchhoff’s Rules to a Circuit: 1. Assign labels and symbols to all the known and unknown quantities. 2. Assign directions to the currents in each part of the circuit. Although the assignment of current directions is arbitrary, you must stick with your original choices throughout the problem as you apply Kirchhoff ’s rules. 3. Apply the junction rule to any junction in the circuit. The rule may be applied as many times as a new current (one not used in a previously found equation) appears in the resulting equation. 4. Apply Kirchhoff’s loop rule to as many loops in the circuit as are needed to solve for the unknowns. In order to apply this rule, you must correctly identify the change in electric potential as you cross each element in traversing the closed loop. Watch out for signs! 5. Solve the equations simultaneously for the unknown quantities, using substitution or any other method familiar to the student. 6. Check your answers by substituting them into the original equations.
Compound Circuits simplifications
Example Circuit(1): Solve for the currents through each resistor And the voltages across each resistor using Series and parallel simplification.
Example Circuit(1): The 6 and 4 ohm resistors are in series, so are combined into 6+4 = 10Ω
Example Circuit(1): The 8 and 10 ohm resistors are in parallel, so are combined into 8∙10/(8+10) =14.4 Ω
Example Circuit The 10 and 4.4 ohm resistors are in series, so are combined into 10+4 = 14.4Ω
Example Circuit(1): Writing KVL, I 1 ∙14.4Ω – 50 v = 0 Or I 1 = 50 v / 14.4Ω = 3.46 A + I 1 ∙14.4Ω -
Example Circuit(1): If I 1 = 3.46 A, then I 1 ∙10 Ω = 34.6 v So the voltage across the 8 Ω = 15.4 v v v -
Example Circuit(1): If I 2 ∙8 Ω = 15.4 v, then I 2 = 15.4/8 = 1.93 A By KCL, I 1 -I 2 -I 3 =0, so I 3 = I 1 –I 2 = 1.53 A v v -
The circuit here has three resistors, R 1, R 2, and R 3 and two sources of emf, V emf,1 and V emf,2 This circuit cannot be resolved into simple series or parallel structures To analyze this circuit, we need to assign currents flowing through the resistors. We can choose the directions of these currents arbitrarily. Example (2)
At junction b the incoming current must equal the outgoing current At junction a we again equate the incoming current and the outgoing current But this equation gives us the same information as the previous equation! We need more information to determine the three currents – 2 more independent equations Example (2):
To get the other equations we must apply Kirchhoff’s Loop Rule. This circuit has three loops. Left R 1, R 2, V emf,1 Right R 2, R 3, V emf,2 Outer R 1, R 3, V emf,1, V emf,2 Example (2)
Going around the left loop counterclockwise starting at point b we get Going around the right loop clockwise starting at point b we get Going around the outer loop clockwise starting at point b we get But this equation gives us no new information! Example - Kirchhoff’s Laws (4)
We now have three equations And we have three unknowns i 1, i 2, and i 3 We can solve these three equations in a variety of ways Example - Kirchhoff’s Laws (5)
Example (3): Find the currents in the circuit shown in Figure by using Kirchhoff’s rules. Solution: Apply the junction rule to point c. I 1 is directed into the junction, I 2 and I 3 are directed out of the junction. Select the bottom loop, and traverse it clockwise starting at point a, generating an equation with the loop rule: Select the top loop, and traverse it clockwise from point c. Notice the gain across the 9.0- resistor, because it is traversed against the direction of the current
Rewrite the three equations, rearranging terms and dropping units for the moment, for convenience: Solve eq. 3 for I 2, substitute into eq. 1: Substitute I 3 back into eq. 3 to get I 2 From eq.1 Substitute the latter expression Substitute I 3 into eq. 2 to get I 1 into eq. 2 and solve for I 3
Homework : Suppose the 6.0V battery is replaced by a battery of unknown emf, and an ammeter measures I 1 =1.5 A. Find the other two currents and the emf of the battery. Answers I 2 =0.96 A, I 3 =0.54 A, =11 V VV I 1 =1.5 A
Example (4): Find I 1, I 2, and I 3 in Figure
2.5. What is the current through the 4- resistor in this circuit? a) 0.67 A b) 0.75 A c) 1.0 A d) 1.3 A e) 1.5 A
2.6. What is the current through the 1- resistor in this circuit? a) 2.8 A b) 3.0 A c) 3.4 A d) 4.0 A e) 4.8 A
2.7. Which one of the following equations is not correct relative to the other four equations determined by applying Kirchoff’s Rules to the circuit shown? a) I 2 = I 1 + I 4 b) I 2 = I 3 + I 5 c) 6 V (8 ) I 1 (5 ) I 2 (4 ) I 3 = 0 d) 6 V (6 ) I 4 (5 ) I 2 (2 ) I 5 = 0 e) 6 V (8 ) I 1 (6 ) I 4 6 V (2 ) I 5 (4 ) I 3 = 0 Not a loop!
2.8.Given is the multi-loop circuit on the right. Which of the following statements cannot be true: A) B) C) D) Junction rule Not a loop! Upper right loop Left loop
2.7. Consider the three resistors and the battery in the circuit shown. Which resistors, if any, are connected in parallel? a) R 1 and R 2 b) R 1 and R 3 c) R 2 and R 3 d) R 1 and R 2 and R 3 e) No resistors are connected in parallel.