Chapters 22/23: Potential/Capacitance Tuesday September 20 th

Transcription

1 Chapters 22/23: Potential/Capacitance Tuesday September 20 th Mini Exam 2 on Thursday: Covers Chs. 21 and 22 (Gauss law and potential) Covers LONCAPA #3 to #6 (due this Wed.) No formula sheet allowed!! Review: Electrostatic potential energy Review and continuation: Electrostatic potential Relationship between V and E Capacitance Definition Examples Equipotential surfaces Conductors Relationship between E and V Reading: up to page 386 in the text book (Chs. 22/23)

2 Electrostatic Potential Energy The electrostatic (Coulomb) force is conservative. It is this property that allows us to define a scalar potential energy (one cannot do this for non conservative forces). b!!u = " $ F # d r! = 1 ' 1 q a 4%& 1 q 2 ) " 1 o ( r b r a *, One can then apply energy conservation (PHY2048).

3 Electrostatic Potential Energy The potential energy is a property of both of the charges, not one or the other. If we choose a reference such that U = 0 when the charges are infinitely far apart, then we can simplify the expression for the potential energy as follows. r! U (r) =! $ F " d r! = 1 ' 1 q # 4%& 1 q 2 o r! 1 * ( ) #, = 1 q 1 q 2 4%& o r Again, the sign of U is not a problem. It is taken care of by the signs of the charges q 1 and q 2.

4 The Electrostatic Potential We define a new quantity known as the Electrostatic Potential V, simply by dividing out the test charge q o : i.e., U = q o V b!! "V = #% E$ d r! = q ( 1 # 1 a 4&' * o ) r b r a, This scalar potential depends only on the details of the source charge distribution (in this case, q). r! V (r) =! $ E" d r! = q 1 # 4%& o r = k q r The absolute value of the potential is not important. As we shall see, it is only potential differences that really matter.

5 Calculating Potential Difference from E x V (r) = k q r 0 d Two parallel conducting plates Cannot really use:!v = "! E# d! r r 1 r 2 $ Can always use definition: Area A!V = " E x dx 0 x # As usual, exploit the symmetry: E x =! " o

6 Calculating Potential Difference from E Area A E x =! " o Two parallel conducting plates Cannot really use: V (r) = k q r Can always use definition:!v = " V $ r 2 r 1! E# d! r As usual, exploit the symmetry:!v = "E x!x = " # $ o d

7 Capacitors Used to store energy in electromagnetic fields [in contrast to batteries (chemical cells) that store chemical energy]. Capacitors can release electromagnetic energy much, much faster than chemical cells. They are thus very useful for applications requiring very rapid responses. q q q q

8 Capacitors The transfer of charge from one terminal of the capacitor to the other creates the electric field. Where there is a field, there must be a potential difference, i.e., a voltage difference between terminals. This leads to the definition of capacitance C: Q = C!V Q represents the magnitude of the excess charge on either plate. Another way of thinking of it is the charge that was transferred between the plates. SI unit of capacitance: (after Michael Faraday) 1 farad (F) = 1 coulomb/volt Capacitances more often have units of picofarad (pf) and microfarad ( µ F)

9 Capacitors The transfer of charge from one terminal of the capacitor to the other creates the electric field. Where there is a field, there must be a potential difference, i.e., a voltage difference between terminals. This leads to the definition of capacitance C: Q = C!V

10 Our Example Involving Parallel Plates V 0 8 Two parallel conducting plates Area A!V = "E x!x = " # $ o d E x =! " o Q Q! = Q A! "V = # Q A$ o d

11 Our Example Involving Parallel Plates Area A E x =! " o Q Q Two parallel conducting plates!v = "E x!x = " # $ o d When defining capacitance, we do not worry about sign of potential, i.e., capacitance is always positive V!V = Q d A" o = Q C # C = " o A d

12 Another Example: Concentric Spheres Can use both V (r) = k q r Q Q and!v = " $ r 2 r 1! E# d! r! E(r) = k q r 2 ˆr

13 Some sophisticated vector calculus The fundamental theorem of calculus: x 2 df dx = f x f x dx x 1 ( ) ( ) 2 1 Recall the 1D example involving the parallel plates: r!!v = " $ E# d r! 2 x = $ 2 ("E x )dx = V 2 "V 1 r 1 x 1! E x = " dv dx # " $V $x

14 Potential Does Not Kill You

15 Some more sophisticated vector calculus The fundamental theorem of calculus: In 3D:! r 2!V = $ "V # d r! = V ( r! ) 2 %V r! 1! r 1 ( )! $ E =!"V =! #V % & #x î #V # y ĵ #V #z ' ˆk ( )

16 Equipotential lines/surfaces E r! " #V #r

17 Equipotential surfaces b W ext = q!v q# b! W E" q( V a b $V ) field =!q"v =!q$ E# d r! =!q V b!v a a Efield lines perpendicular to equipotential surfaces Field does positive work when q accelerated by field a ( )

18 Equipotential surfaces Here are some example surfaces including field lines (point charge, infinite charged plane and a dipole). By spacing the equipotential surfaces by the same potential difference (! V), one can get a feel for the electric field strength (E = dv/dr), i.e. the closer the spacing, the stronger the field.