1. Mondady Feb. 10, 2014PHYS 1442-004, Dr. Andrew Brandt 1 PHYS 1442 – Section 004 Lecture #8 Monday February 10, 2014 Dr. Andrew Brandt CH 18 Electric Power CH 19 Resistors Series and parallel “Simple” circuits ***Defer AC to Monday 17 th along with short review

2. Announcements a) HW4 on ch 18 due Tues at 11:30 pm c) HW5 on part of ch 19 due Monday 17 th at 5:25 pm (can get a 24 hour extension if in class) d) Test on Weds. Feb. 19 th ch 16-18 plus part of ch 19 th Mostly multiple guess, bring a scantron, I don’t know how many problems Mondady Feb. 10, 2014 2 PHYS 1442-004, Dr. Andrew Brandt

3. Mondady Feb. 10, 2014 3 PHYS 1442-004, Dr. Andrew Brandt Electric Energy Why is electric energy useful? –It can be transformed easily into different forms of energy: Motors, pumps, etc, transform electric energy to mechanical energy Heaters, dryers, cook-tops, etc., transform electricity to thermal energy Light bulb filaments transform electric energy to light energy –Only about 10% of the energy turns to light with 90% lost via heat –Typical household light bulb and heating elements have resistance of order few ohms to few hundred of ohms How does electric energy transform to thermal energy? –Flowing electrons collide with the vibrating atoms of the wire. –In each collision, part of electron’s kinetic energy is transferred to the atom it collides with. –The kinetic energy of wire’s atoms increases, and thus the temperature of the wire increases. –The increased thermal energy can be transferred as heat through conduction and convection to the air in a heater or to food in a pan; it can also be radiated as light.

4. Mondady Feb. 10, 2014 4 PHYS 1442-004, Dr. Andrew Brandt Electric Power How do we find out the power of an electric device? –What is definition of the power? The rate at which work is done or the energy is transferred What energy is transferred when charge q moves through a potential difference V? –U=qV; So to move a small amount of charge q q in a small amount of time  t through a potential difference V, the power P is – –Thus, we obtain. –What is the unit? –What kind of quantity is the electrical power? Scalar –P=IV can apply to any device, while the formulae involving resistance only applies to Ohmic resistors. What is this? Watts = J/s In terms of resistance

5. Mondady Feb. 10, 2014 5 PHYS 1442-004, Dr. Andrew Brandt Example Headlights: Calculate the resistance of a 40-W automobile headlight designed for a 12V battery. Since the power is 40W and the voltage is 12V, we use the formula with V and R. Solve for R

6. Mondady Feb. 10, 2014 6 PHYS 1442-004, Dr. Andrew Brandt Power in Household Circuits Household devices usually have small resistance –But since they draw current, if it become large enough, wires can heat up (overload) and cause a fire Why is using thicker wires safer? –Thicker wires have less resistance, lower heat How do we prevent this? –Put in a switch that disconnects the circuit when overloaded Fuse or circuit breakers They open up the circuit when the current exceeds a certain value Overload

7. Mondady Feb. 10, 2014 7 PHYS 1442-004, Dr. Andrew Brandt Example Will a 30A fuse blow? Determine the total current drawn by all the devices in the circuit in the figure. The total current is the sum of current drawn by the individual devices. Solve for I BulbHeater StereoDryer Total current What is the total power? Max power?

8. Mondady Feb. 10, 2014 8 PHYS 1442-004, Dr. Andrew Brandt What do we need to have current in an electric circuit? –A device that provides a potential difference, such as battery or generator typically it converts some type of energy into electric energy These devices are called sources of electromotive force ( emf ) –This does NOT refer to a real “force”. The potential difference between terminals of the source, when no current flows to an external circuit, is called the emf (  ) of the source. A battery itself has some internal resistance ( r ) due to the flow of charges in the electrolyte –Why do headlights dim when you start the car? The starter needs a large amount of current but the battery cannot provide charge fast enough to supply current to both the starter and the headlights EMF and Terminal Voltage

9. Mondady Feb. 10, 2014 9 PHYS 1442-004, Dr. Andrew Brandt Since the internal resistance is inside the battery, we cannot separate the two. EMF and Terminal Voltage So the terminal voltage difference is V ab =V a -V b. When no current is drawn from the battery, the terminal voltage equals the emf which is determined by the chemical reaction; V ab = .. However when the current I flows from the battery, there is an internal drop in voltage which is equal to Ir. Thus the actual delivered terminal voltage is

10. Mondady Feb. 10, 2014 10 PHYS 1442-004, Dr. Andrew Brandt Resistors are in series when two or more of them are connected end to end –These resistors represent simple electrical devices in a circuit, such as light bulbs, heaters, dryers, etc. Resistors in Series What is common in a circuit connected in series? –the current is the same through all the elements in series Potential difference across each element in the circuit is: V 1 =IR 1, V 2 =IR 2 and V 3 =IR 3 Since the total potential difference is V, we obtain V=IR eq =V 1 +V 2 +V 3 =I(R 1 +R 2 +R 3 ) Thus, R eq =R 1 +R 2 +R 3 Resistors in series When resistors are connected in series, the total resistance increases and the current through the circuit decreases compared to a single resistor.

11. Mondady Feb. 10, 2014 11 PHYS 1442-004, Dr. Andrew Brandt Why is it true that V=V 1 +V 2 +V 3 ? Energy Losses in Resistors What is the potential energy loss when charge q passes through the resistor R 1, R2 R2 and R3R3  U 1 =qV 1,  U 2 =qV 2,  U 3 =qV 3 Since the total energy loss should be the same as the energy provided to the system by the battery, we obtain  U=qV=  U 1 +  U 2 +  U 3 =q(V 1 +V 2 +V 3 ) Thus, V=V 1 +V 2 +V 3

12. Mondady Feb. 10, 2014 12 PHYS 1442-004, Dr. Andrew Brandt Example Battery with internal resistance. A 65.0-  resistor is connected to the terminals of a battery whose emf is 12.0V and whose internal resistance is 0.5- . Calculate (a) the current in the circuit, (b) the terminal voltage of the battery, V ab, and (c) the power dissipated in the resistor R and in the battery’s internal resistor. (a) Since We obtain Solve for I (b) The terminal voltage V ab is (c) The power dissipated in R and r are What is this? A battery or a source of emf.

13. Mondady Feb. 10, 2014 13 PHYS 1442-004, Dr. Andrew Brandt Resistors are in parallel when two or more resistors are connected in separate branches –Most house and building wirings are arranged this way. Resistors in Parallel What is common in a circuit connected in parallel? –T–The voltage is the same across all the resistors. –T–The total current that leaves the battery, is however, split. The current that passes through every element is I 1 =V/R 1, I 2 =V/R 2, I 3 =V/R 3 Since the total current is I, we obtain I=V/R eq =I 1 +I 2 +I 3 =V(1/R 1 +1/R 2 +1/R 3 ) Thus, 1/R eq =1/R 1 +1/R 2 +1/R 3 Resistors in parallel When resistors are connected in parallel, the total resistance decreases and the current through the circuit increases compared to a single resistor.

14. Mondady Feb. 10, 2014 14 PHYS 1442-004, Dr. Andrew Brandt Parallel Capacitor arrangements Resistor and Capacitor Arrangements Series Resistor arrangements Series Capacitor arrangements Parallel Resistor arrangements

15. Mondady Feb. 10, 2014 15 PHYS 1442-004, Dr. Andrew Brandt Example Series or parallel? (a) The light bulbs in the figure are identical and have identical resistance R. Which configuration produces more light? (b) Which way do you think the headlights of a car are wired? (a) What are the equivalent resistances for the two cases? Series The bulbs get brighter when the total power transformed is larger. series ParallelSo parallel So parallel circuit provides brighter lighting. (b) Car’s headlights are in parallel to provide brighter light and also to prevent both lights going out at the same time when one burns out. So what is bad about parallel circuits?

16. Mondady Feb. 10, 2014 16 Example Current in one branch. What is the current flowing through the 500-  resistor in the figure? What do we need to find first? Thus the total current in the circuit is We need to find the total current. To do that we need to compute the equivalent resistance. R eq of the small parallel branch is: R eq of the circuit is: The voltage drop across the parallel branch is The current flowing across 500-  resistor is therefore What is the current flowing in the 700-  resister? What is the current flowing in the 400-  resister? PHYS 1442-004, Dr. Andrew Brandt

17. Resistors in Series and in Parallel Conceptual Example: An illuminating surprise. A 100-W, 120-V light bulb and a 60-W, 120-V light bulb are connected in two different ways as shown. In each case, which bulb glows more brightly? Ignore change of filament resistance with current (and temperature). Solution: a.) Each bulb sees the full 120V drop, as they are designed to do, so the 100- W bulb is brighter. b.) P = V 2 /R, so at constant voltage the bulb dissipating more power will have lower resistance. In series, then, the 60-W bulb – whose resistance is higher – will be brighter. (More of the voltage will drop across it than across the 100-W bulb). 17 Mondady Feb. 10, 2014

18. Resistors in Series and in Parallel Conceptual Example: Bulb brightness in a circuit. The circuit shown has three identical light bulbs, each of resistance R. (a) When switch S is closed, how will the brightness of bulbs A and B compare with that of bulb C? (b) What happens when switch S is opened? Use a minimum of mathematics in your answers. Solution: a. When S is closed, the bulbs in parallel have half the resistance of the series bulb. Therefore, the voltage drop across them is smaller. Bulbs A and B will be equally bright, but much dimmer than C. b. With switch S open, no current flows through A, so it is dark. B and C are now equally bright, and each has half the voltage across it, so C is somewhat dimmer than it was with the switch closed, and B is brighter. 18 Mondady Feb. 10, 2014