Summary of Class 10 8.02 Wednesday 2/23/05 / Thursday 2/24/05 Topics: Current, Resistance, and DC Circuits Related Reading: Course Notes (Liao et al.): Chapter 6; Sections 7.1 through 7.4 Serway and Jewett: Chapter 27; Sections 28.1 through 28.3 Giancoli: Chapter 25; Sections 26-1 through 26-3 Topic Introduction In today's class we will define current, current density, and resistance and discuss how to analyze simple DC (constant current) circuits using Kirchhoff’s Circuit Rules. Current and Current Density Electric currents are flows of electric charge. Suppose a collection of charges is moving perpendicular to a surface of area A, as shown in the figure The electric current I is defined to be the rate at which charges flow across the area A. If is given by I ∆Q Q Ian amount of charge ∆ passes through a surface in a time interval ∆ , then the current tGJ (coulombs per second, or amps). The current density (amps per = ∆t GI JThe current is a scalar, but GJ square meter) is a concept closely related to current. The magnitude of the current at any point in space is the amount of charge per unit time per unit area GJdensity ∆Qflowing pass that point. That is, is a vector.= . ∆tA∆ Microscopic Picture of Current Density If charge carriers in a conductor have number density , charge , and a drift velocityn qGE of the charge carriers is proportional to the electric field GJ, then the current density G vd is the product of n, q, and . In Ohmic conductors, theG vd Gvddrift velocity in the conductor. This proportionality arises from a balance between the acceleration due the electric field and the deceleration due to collisions between the charge carriers and the “lattice”. In steady state these two terms balance each other, leading to a steady drift G Evelocity (a “terminal” velocity) proportional to GJthe “microscopic” Ohm’s Law, which states that the current density GEelectric field . This proportionality leads directly to is equal to the times the conductivity σ. The conductivity σ of a material is equal to the inverse of its resistivity ρ. Summary for Class 10 p. 1Summary of Class 10 8.02 Wednesday 2/23/05 / Thursday 2/24/05 Electromotive Force A source of electric energy is referred to as an electromotive force, or emf (symbol ε). Batteries are an example of an emf source. They can be thought of as a “charge pump” that moves charges from lower potential to the higher one, opposite the direction they would normally flow. In doing this, the emf creates electric energy, which then flows to other parts of the circuit. The emf ε is defined as the work done to move a unit charge in the direction of higher potential. The SI unit for ε is the volt (V), i.e. Joules/coulomb. Kirchhoff’s Circuit Rules In analyzing circuits, there are two fundamental (Kirchhoff’s) rules: (1) The junction rule states that at any point where there is a junction between various current carrying branches, the sum of the currents into the node must equal the sum of the currents out of the node (otherwise charge would build up at the junction); (2) The loop rule states that the sum of the voltage drops ∆V across all circuit elements that form a closed loop is zero (this is the same as saying the electrostatic field is conservative). If you travel through a battery from the negative to the positive terminal, the voltage drop ∆V is + ε, because you are moving against the internal electric field of the battery; otherwise ∆V is -ε. If you travel through a resistor in the direction of the assumed flow of current, the voltage drop is –IR, because you are moving parallel to the electric field in the resistor; otherwise ∆V is +IR. Steps for Solving Multi-loop DC Circuits 1) Draw a circuit diagram, and label all the quantities; 2) Assign a direction to the current in each branch of the circuit--if the actual direction is opposite to what you have assumed, your result at the end will be a negative number; 3) Apply the junction rule to the junctions; 4) Apply the loop rule to the loops until the number of independent equations obtained is the same as the number of unknowns. and I: IImportant EquationsGJRelation between = GJRelation between GG ∫∫ JA⋅ d G and charge carriers: J = nq G G v G dG Microscopic Ohm’s Law: Macroscopic Ohm’s Law: Resistance of a conductor with resistivity ρ, cross-sectional area A, and length l: Resistors in series: Resistors in parallel: Power: J =σE = E/ρ VIR = /R =ρlAR = RR+eq 1 2 eq 1 R = 1 1 R + 2 1 R P =∆V I Summary for Class 10 p.
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