W10D2 DC Circuits Today’s Reading Assignment W10D2 DC Circuits & Kirchhoff’s Loop Rules Course Notes: Sections 7.1-7.5 1 Announcements PS 8 due Week 11 Tuesday at 9 pm in boxes outside 32-082 or 26-152 Next Reading Assignment W10D3 PS07: PhET: Building a Circuit 7.1-7.5, 7.10 Exam 3 Thursday April 24 7:30 pm –9:30 pm Conflict Exam 3 Friday April 25 8-10 am, 10-12 noon If you have a regularly scheduled MIT activity that conflicts with Exam 3, contact padour@mit.edu and explain conflict and request time to take conflict exam. 2 Outline DC Circuits Kirchoff’s Laws Electrical Power Measuring Voltage and Current 3 Class 12 1 DC Circuits 4 Examples of Circuits 5 Symbols for Circuit Elements Battery Resistor Capacitor Switch Equipotential Junction Branch 6 Class 12 2 Electromotive Force (EMF) The work per unit charge around a closed path done is called electromotive force EMF. Thisis a bad name because it is not a force. Let fs denote the force per unit charge, then the EMF is ε = ∫ fs ⋅ d s closd path If a conducting closed path is present then ε = IR 7 Ideal Battery 1) Inside Battery: chemical force fs , non-zero inside battery (zero outside), moves in which charges through a region static electric field Estatic opposes motion Estatic = − fs 2) Ideal battery: net force on charges is zero 3) Potential difference between its terminals + + V (+) − V (−) = − ∫ Estatic ⋅ d s = ∫ fs ⋅ d s − − 4) Extend path through external circuit where fs = 0 + V (+) − V (−) = ∫ fs ⋅ d s = ∫ fs ⋅ d s = ε − 8 Kirchhoff’s Loop Rules 9 Class 12 3 Charge Conservation Sum of currents entering any junction in a circuit must equal sum of currents leaving that junction. I1 = I 2 + I 3 10 Sum of Potential Differences Around a Closed Path Sum of potential differences across all elements around any closed circuit loop must be zero. ∑ ΔVi = − ∫ Estatic ⋅ d s = 0 i Closed Path 11 DC Circuits Rules for Batteries and Resistors 12 Class 12 4 Reference System for Circuit Analysis 1. Simplify resistors in series/parallel. 2. Assign current and current direction in each branch 3. Assign circulation direction for each loop. 4. Circulation direction across each element defines “before” and “after” side of element. 5. Define electric potential difference across a circuit element by ΔV ≡ V (after) − V (before) ≡ V (a) − V (b) 13 Sign Conventions - Battery Circulating from the negative to positive terminal of a battery increases your potential ΔV = +ε Circulating from the positive to negative terminal of a battery decreases your potential ΔV = −ε 14 Sign Conventions - Resistor Direction of current is the same as direction of electric field which points to lower electric potential Circulating across a resistor in the direction of current decreases the potential ΔV = − IR Circulating across a resistor in the opposite direction of current increases your potential ΔV = + IR 15 Class 12 5 Series vs. Parallel Series Parallel 16 Resistors In Series The same current I must flow through both resistors Circulate Clockwise: ΔV − I R1 + I R2 = 0 ⇒ ΔV = I(R1 + R2 ) = I Req Req = R1 + R2 17 Resistors In Parallel Voltage drop across the resistors must be the same ΔV = ΔV1 = ΔV2 = I1 R1 = I 2 R2 = IReq I = I1 + I 2 = ΔV ΔV ΔV 1 1 1 + = ⇒ = + R1 R2 Req Req R1 R2 18 Class 12 6 Concept Q: Resistors In Parallel Suppose that R1 >> R2 . Then the equivalent resistance 1. Req R2 2. Req R1 3. Req R2 / 2 4. Req R2 / 2 19 Group Problem: Four Resistors Four resistors are connected to a battery as shown in the figure. The current in the battery is I, the battery emf is ε, and the resistor values are R1 = R, R2 = 2R, R3 = 4R, R4 = 3R. Determine the current in each resistor in terms of I. 20 Internal Resistance Real batteries have an internal resistance, r, which is small but non-zero Circulate clockwise: Terminal voltage: ΔV = Vb − Va = ε − I r (Even if you short the leads you don’t get infinite current) Class 12 7 Measuring Voltage & Current 22 Measuring Potential Difference A voltmeter must be hooked in parallel across the element you want to measure the potential difference across 1 1 1 = + Reffective R RVoltmeter 1 R Voltmeters have a very large resistance, so that they don’t affect the circuit too much 23 Measuring Current An ammeter must be hooked in series with the element you want to measure the current through Reffective = R + Rammeter R Ammeters have a very low resistance, so that they don’t affect the circuit too much Class 12 24 8 Concept Question: Measuring Current If R1 > R2, compare the currents measured by the three ammeters: 1. 2. 3. 4. 5. 6. 7. I1 > I2 > I3 I2 > I1 > I3 I3 > I1 > I2 I3 > I2 > I1 I3 > I1 = I2 None of the above Not enough information is given. P18- 25 Measuring Resistance An ohmmeter must be hooked in parallel across the element you want to measure the resistance of Here we are measuring R1 Ohmmeters apply a voltage and measure the current that flows. They typically won’t work if the resistor is powered (connected to a battery) 26 Concept Question: Bulbs & Batteries An ideal battery is hooked to a light bulb with wires. A second identical light bulb is connected in parallel to the first light bulb. After the second light bulb is connected, the current from the battery compared to when only one bulb was connected 1. is higher. 2. is lower. 3. is the same. P18- 27 Class 12 9 Concept Question: Bulbs & Batteries An ideal battery is hooked to a light bulb with wires. A second identical light bulb is connected in series with the first light bulb. After the second light bulb is connected, the current from the battery compared to when only one bulb was connected 1. is higher. 2. is lower. 3. is the same. P18- 28 Electrical Power Power is change in energy per unit time So power to move current through circuit elements: P= d d dq ΔU ) = ( qΔV ) = ΔV ( dt dt dt P = I ΔV 29 Power - Battery Moving from the negative to positive terminal of a battery increases your potential. If current flows in that direction the battery supplies power I Psupplied = I ΔV = I ε 30 Class 12 10 Power – Resistor (Joule Heating) Moving across a resistor in the direction of current decreases your potential. Resistors always dissipate power Pdissipated = I ΔV = I 2 R = ΔV 2 R 31 Concept Question: Power An ideal battery is hooked to a light bulb with wires. A second identical light bulb is connected in parallel to the first light bulb. After the second light bulb is connected, the power output from the battery (compared to when only one bulb was connected) 1. 2. 3. 4. 5. Is four times higher Is twice as high Is the same Is half as much Is ¼ as much P18- 32 Concept Question: Power An ideal battery is hooked to a light bulb with wires. A second identical light bulb is connected in series with the first light bulb. After the second light bulb is connected, the light (power) from the first bulb (compared to when only one bulb was connected) 1. 2. 3. 4. 5. Is four times higher Is twice as high Is the same Is half as much Is ¼ as much P18- 33 Class 12 11 Demonstration: Five Different Types of Resistance F13 http://tsgphysics.mit.edu/front/?page=demo.php&letnum=F 13&show=0 34 Worked Example: Circuit What is current through each branch of the circuit shown in the figure below? 35 Worked Example: Simple Circuit Current conservation at a: I1 = I 2 + I 3 Lower Loop: Start at a and circulate clockwise. Then − I 2 2R1 + I 3 3R1 + ε = 0 ⇒ I 3 = (2 / 3)I 2 − (ε / 3R1 ) Upper Loop: Start at a and circulate counterclockwise. Then − I 2 2R1 − I1 R1 + 2ε = 0 ⇒ I1 = (2ε / R1 ) − 2I 2 I1 = I 2 + I 3 ⇒ (2ε / R1 ) − I 2 = I 2 + (2 / 3)I 2 − (ε / 3R1 ) Solve for I2: I 2 = 7ε / 11R1 ⇒ I 3 = ε / 11R1 and I1 = 8ε / 11R1 Class 12 36 12 Demonstration: Wheatstone Bridge F14 http://tsgphysics.mit.edu/front/?page=demo.php&letnum=F 14&show=0 37 Group Problem: Wheatstone Bridge A circuit consisting of two resistors with R1=6.0 ohms and R2=1.5 ohms, a variable resistor, with resistance Rvar, a resistor of unknown value Ru, and 9.0 volt battery, are connected as shown in the figure. When Rvar is adjusted to 12 ohms, there is zero current through the ammeter. What is the unknown resistance Ru? 38 Class 12 13