Phy 213: General Physics IIIElectric CurrentConduction Model of Electric Current (through a constant area pathway)Conduction of Electric Current (cont.)Current Density & Drift VelocityOhm’s LawResistanceTable of Selected Resistivities (@ 20oC)Relation between Current Density & ResistancePowerPhy 213: General Physics IIIChapter 26: Electric CurrentLecture NotesElectric Current1. An electric potential causes electric charges to move2. The flow of electric charge is called electric currenta. Positive charge accelerates toward lower electric potentialb. Negative charge accelerates toward higher electric potential3. The rate of flow of electric charge (i) through a conducting material is4. The SI units are coulombs per second (C/s), called amperes (A): 1 C/s = 1 A5. The quantity of charge movement (q) is related to the electric current (i):Note: By convention, electric current is defined as the flow of positive charge carriers flowing from high potential (+) to low potential (-)dqi = dt2 21 1t tt tq = dq = idt� �Conduction Model of Electric Current(through a constant area pathway)1. Conduction depends on potential difference between 2 regions & how far apart those regions are separated2. Increasing the cross-sectional area increases amount of charge that can flow through in a given time, for constant J3. Of course, the relative ability to conduct charge is an intrinsic property of different materials !!VBLVAiLVAAiVBConduction of Electric Current (cont.)1. The rate of charge flow (current) w/in a conductor depends ona. The potential difference between 2 regions along the conducting pathway material (V)b. The cross sectional area of the conducting pathway (A)c. The ability of the conductor to conduct charge () {the conductivity}d. The length of conducting pathway (L)2. For a uniform cylindrical conductor, combining these elements leads to the conduction equation:The quantity, , is called the conductivity (g):3. Conductivity is more commonly expressed as the “resistance” (R) of the conducting pathway:where r is the “resistivity “ (in units of or )dq A = i = V = g Vdt LsD DALs1 L LR = = = g A ArsAg = LsV mA�mW�2. The current density of charge flow through a cylindrical region (area, A and length L) is related to the number of charge carriers (n) & their average drift velocity (vdrift):For a 0.1A current flowing through a copper wire (n = 8.49x1028m-3 & A = 1x10-6 m2):Current Density & Drift Velocity1. For a steady state uniformly distributed electric current, the current can be expressed in terms of its associated current density vector (J).where is the area vector, perpendicular to the cross sectional area through which the current flows( )i = J dA = J cos dA f�� �r rdrift drifti NJ = = e v =ne vVA� �� �� �rr rrdArLAq nei= =t t-6mdriftsJv = =7.4x10neOhm’s Law1. The electric current can be re-expressed as:where V = V = the potential difference across the conductive pathway2. Thus, the current through any conducting pathway can be described by dividing the potential across the pathway by the effective resistance of the pathway…OrThe resistance of a conducting pathway is defined as the potential difference divided by the current flow:3. When the ratio, V/i, is a constant value for all values of V the conductor is said to be an “Ohmic” material:V/i = R = constant {Ohm’s Law}4. When R is not constant, the conductor is non-Ohmic5. Ohm’s Law is more commonly expressed as: V = iRVi = gV =RVR =iResistance1. The resistance (R) of a substance depends on:a. length (L)b. Cross-sectional area (A)c. Resistivity ()  units are .m2. Units of resistance are V/A, called ohms ()1 V/A = 1  3. The intrinsic physical property, resistivity () depends on temperature. Over a limited temperature range the temperature dependence is given by:a. For conductors: resistivity increases with T ( > 0)b. For semi-conductors: resistivity decreases with T ( < 0)LR = Ar[ ]0 0 = (1 + (T-T )r r aTable of Selected Resistivities (@ 20oC)Material ( m)  oC)Material ( m)oC)Silver 1.59x10-8.0061Carbon*(graphite)3-60x10-5-.0005Copper 1.68x10-8.0068 Germanium* 10-3-10-1-.05Aluminum 2.65x10-8.00429 Silicon* 0.1-60 -.07Tungsten 5.6x10-8.0045 Glass 109-1013...Iron 9.71x10-8.00651 Quartz (fused) 7.5x1017...Platinum 10.6x10-8.003927 Hard rubber 1013-1015...Manganin 48.2x10-8.000002Lead 22x10-80.0039Mercury 98x10-8.0009Table reproduced from: http://hyperphysics.phy-astr.gsu.eduRelation between Current Density & ResistanceThe resistivity of a conducting material, reflects the ability of the material to resist current flow and thus limit current density, for a given potential difference:where  = V/L (the potential difference per unit length)Semi-Obvious Consequence:For steady state current flow, as the current density increases and surface area decreases: =constant→V/L must increase→ V will increase→R must increaseL V V V 1R = = = = = A i J A L J Jr nr� ��� �� �Power1. It requires energy to “push” charge through an electrical device. This should be obvious given that the charge flows from high potential (Uhigh) to lower potential (Ulow).2. The energy must go somewhere if the charge flows at constant drift velocity (K=0). It is radiated out as heat energy.3. The energy transfer associated with moving a charge dq across a potential difference, V is: 4. The rate of energy transfer, in Watts, is given by:5. Applying Ohm’s Law, the power can be alternatively expressed to describe “resistive” dissipation of energy:dU dq = P = V = iVdt dt�22VP = i R = R-dW = dU = dq