1. Lecture 7 Circuits Chp. 28 Cartoon -Kirchoff’s Laws Opening Demo- transmission lines Physlet Topics –Direct Current Circuits –Kirchoff’s Two Rules –Analysis of Circuits Examples –Ammeter and voltmeter –RC circuits Demos –Ohms Law –Power loss in transmission lines –Resistivity of a pencil –Blowing a fuse Warm-up problems

2. Transmission line demo

3. Direct Current Circuits 1.The sum of the potential charges around a closed loop is zero. This follows from energy conservation and the fact that the electric field is a conservative force. 2. The sum of currents into any junction of a closed circuit must equal the sum of currents out of the junction. This follows from charge conservation.

4. Example (Single Loop Circuit) No junction so we don’t need that rule. How do we apply Kirchoff’s rule? Must assume the direction of the current – assume clockwise. Choose a starting point and apply Ohm’s Law as you go around the circuit. a.Potential across resistors is negative b.Sign of E for a battery depends on assumed current flow c.If you guessed wrong on the sign, your answer will be negative Start in the upper left hand corner.

5. Put in numbers. Suppose: amp Suppose: amp We get a minus sign. It means our assumed direction of current must be reversed. Note that we could have simply added all resistors and get the R eq. and added the EMFs to get the E eq. And simply divided. amp Sign of EMF Battery 1 current flows from - to + in battery +E 1 Battery 2 current flows from + to - in battery -E 2 In 1 the electrical potential energy increases In 2 the electrical potential energy decreases

6. Example with numbers Quick solution: Question: What is the current in the circuit? Write down Kirchoff’s loop equation. Loop equation Assume current flow is clockwise. Do the batteries first – Then the current.

7. Example with numbers (continued) Question: What are the terminal voltages of each battery? 12V: 2V: 4V:

8. Multiloop Circuits Kirchoff’s Rules 1. in any loop 2. at any junction Find i, i 1, and i 2 Rule 1 – Apply to 2 loops (2 inner loops) a. b. Rule 2 a. We now have 3 equations with 3 unknowns. multiply by 2 multiply by 3 subtract them Find the Joule heating in each resistor P=i 2 R. Is the 5V battery being charged?

9. Method of determinants for solving simultaneous equations For example solve for i You try it for i 1 and i 2. See Appendix in your book on how to use Cramer’s Rule.

10. Another example Find all the currents including directions. Loop 1Loop 2 multiply by 2 i = i 1 + i 2 Loop 1 Loop 2 ii i i i1i1 i2i2 i2i2

11. Rules for solving multiloop circuits 1.Replace series resistors or batteries with their equivalent values. 2.Choose a direction for i in each loop and label diagram. 3.Write the junction rule equation for each junction. 4.Apply the loop rule n times for n interior loops. 5.Solve the equations for the unknowns. Use Cramer’s Rule if necessary. 6.Check your results by evaluating potential differences.

12. How does a capacitor behave in a circuit with a resistor? Charge capacitor with 9V battery with switch open, then remove battery. Now close the switch. What happens?

13. Discharging a capacitor through a resistor V(t) Potential across capacitor = V = just before you throw switch at time t = 0. Potential across Resistor = iR at t > 0. What is the current I at time t?

14. Time constant = RC

15. What is the current? Ignore - sign RC

16. How the charge on a capacitor varies with time as it is being charged

18. Ohmmeter

19. Ammeter

20. Voltmeter

21. Warm up set 7 Warm up set 7 Due 8:00 am Tuesday 1. HRW6 28.TB.05. [119859] In the context of the loop and junctions rules for electrical circuits a junction is: where a wire is connected to a battery where three or more wires are joined where a wire is bent where a wire is connected to a resistor where only two wires are joined 2. HRW6 28.TB.18. [119872] Two wires made of the same material have the same length but different diameter. They are connected in parallel to a battery. The quantity that is NOT the same for the wires is: the electric field the electron drift velocity the current the current density the end-to-end potential difference 3. HRW6 28.TB.26. [119880] The emf of a battery is equal to its terminal potential difference: only when there is no current in the battery only when a large current is in the battery under all conditions under no conditions only when the battery is being charged