Lecture 4 Electric Potential and/ Potential Energy Ch. 25

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1 Lecture 4 Electric Potential and/ Potential Energy Ch. 5 Review from Lecture 3 Cartoon - There is an electric energy associated with the position of a charge. Opening Demo - Warm-up problems Physlet Topics Electric potential energy and electric potential Calculation of potential from field Potential from a point charge Potential due to a group of point charges, electric dipole Potential due to continuous charged distributions Calculating the filed from the potential Electric potential energy from a system of point charge Equipotential Surface Potential of a charged isolated conductor Demos teflon and silk Charge Tester, non-spherical conductor, compare charge density at Radii Van de Graaff generator with pointed objects 1

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5 Potential Energy and Electric potential The electric force is mathematically the same as gravity so it too must be a conservative force. We will find it useful to define a potential energy as is the case for gravity. Recall that the change in the potential energy in moving from one point a to point b is the negative of the work done by the electric b force. " U = U b U a = - W = -Work done by the electric force = # F " ds Since F = q 0 E, U = q 0 E " ds and b # a Electric Potential difference = Potential energy change/ unit charge V = U SI unit of electric potential is volt (V): q 0 1 Volt = 1 Joule/Coulomb (1 V = 1 J/C) $ V = V # V = # E " ds (independent of path, ds) b a a Joule is too large a unit of energy when working at the atomic or molecular level, so use the electron-volt (ev), the energy obtained when an electron moves through a potential difference of 1 V. 1 ev = 1.6 x J 5

6 U = U f " U i = - Work done by the electric force = F " ds f # i y V = U q x $ V = V # V = # E " ds f i (independent of path, ds) Therefore, electric force is a conservative force. 6

7 V = "W q 0 = " F # d s q 0 $ = " $ E # d s The potential difference is the negative of the work done per unit charge by an electric field on a positive unit charge when it moves from one point to another. V is a scalar not a vector. Simplifies solving problems. We are free to choose V to be 0 at any location. Normally V is chosen to be 0 at the negative terminal of a battery or 0 at infinity for a point charge. 7

8 Example of finding the potential difference in a Uniform Field What is the electric potential difference for a unit positive charge moving in an uniform electric field from a to b? E a d b b E # $ $ x direction V = E " ds = E dx = E( xb xa) a " V = Ed U = q V " U = qed b a dv = Edx E = dv / dx d 8

9 Example for a battery in a circuit In a 9 volt battery, typically used in IC circuits, the positive terminal has a potential 9 v higher than the negative terminal. If one micro-coulomb of positive charge flows through an external circuit from the positive to negative terminal, how much has its potential energy been changed? q " V Potential energy is lower by = " U q " U = 9q # U We also assumed that the potential at b was 0 = Vb Va = ( 0 9) V = ( 9V )" 1" 10 = 9 " 10 9 µj 6 6 C Joules U = " 9 microjoules = " 9 µj 9

10 Example of a proton accelerated in a uniform field A proton is placed in an electric field of E=10 5 V/m and released. After going 10 cm, what is its speed? Use conservation of energy. a + b " V = Vb Va = Ed U = qv = "qed U + K = 0 K = "U K = qed 1 mv = qed E = 10 5 V/m d = 10 cm v v = = qed m "19 C 10 5 V m 0.1m "7 kg v = m s 10

11 What is the electric potential when moving from one point to another in a field due to a point charge? V = " $ E # d r E = kq r ˆr V f V i = f # i E " d r 11

12 Potential of a point charge at a distance R V f V i = # V f V i = E # 1 $ " dˆr = kq cos0 " $ r d r = kq 1 # r R R f # i E " dˆr V f V i = 0 V i = k q R R = kq( 1 # 1 R ) kq V = R 1 k = 4" 0 Replace R with r V = 1 4" 0 q r eqn 5-6 1

13 Electric potential for a positive point charge V(r) = kq r r = x + y V is a scalar V is positive for positive charges, negative for negative charges. r is always positive. For many point charges, the potential at a point in space is the simple algebraic sum (Not a vector sum) 13

Electric potential due to a positive point charge Hydrogen atom. What is the electric potential at a distance of 0.59 A from the proton? 1A= 10-10 m kq R 9 &( 8.99 " 10 Nm #% " 1.6 " 10 ' C $.

14 Electric potential due to a positive point charge Hydrogen atom. What is the electric potential at a distance of 0.59 A from the proton? 1A= m kq R 9 &( 8.99 " 10 Nm #% " 1.6 " 10 ' C $.59 " 10 m V = = 10 V = 7. J C = 7.Volts What is the electric potential energy of the electron at that point? U = qv= (-1.6 x C) (7. V)= x J or - 7. ev where ev stands for electron volts. 19 C r = 0.59 A Total energy of the electron in the ground state of hydrogen is ev Also U= E = -7. ev. This agrees with above formula. 14

15 What is the electric potential due to several point charges? For many point charges, the potential at a point in space is the simple algebraic sum (Not a vector sum) y V = i kq i r i q 1 q r r 1 V = & k$ % q r q r + q r 3 3 # " r 3 q 3 x 15

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17 Potential due to a dipole For two point charges, the total potential is the sum of the potentials of each point charge. So, V = V = V + V dipole dipole = V total a + V b a V b & q (' q) # = k$ + % ra rb " & rb ' ra # = kq$ % rarb " We are interested in the regime where r>>d. As in fig, r a and r b are nearly parallel. And the difference in their length is dcos". Also because r>>d, r a r b is approximately r. V dipole kq d cos r kp cos r where p is the dipole moment. 17

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19 Potential due to a ring of charge Direct integration. Since V is a scalar, it is easier to evaluate V than E. Find V on the axis of a ring of total charge Q. Use the formula for a point charge, but replace q with elemental charge dq and integrate. Point charge V = kq r For an element of charge r is a constant as we integrate. V = = kdq r ( z kdq + R k = dq ( z + R ) ) dq, dv = V kdq r = (z k + R ) Q This is simpler than finding E because V is not a vector. 19

20 Potential due to a line charge We know that for an element of charge dq dq the potential is dv = k r For the line charge let the charge density be #. Then dq=#dx So, Then, dx dv = k r dv = k dx x + d But, r = x + Now, we can find the total potential V produced by the rod at point P by integrating along the length of the rod from x=0 to x=l L L L " dx dx V = dv = k = k" V = k" ln(x + x + d ) 0 0 x + d 0 x + d So, d " V = k" (ln(l + L + d ) lnd) Or, V = k ln L + L + d % $ ' # d & 0 L 0

21 A new method to find E if the potential is known. If we know V, how do we find E? V = " E # d s $ dv = E " d s E E E x y z dv = dx dv = dy dv = dz E = E x î + E y ĵ + E z ˆk d s = îdx + ĵdy + ˆkdz dv = Ex dx Eydy E z dz So the x component of E is the derivative of V with respect to x, etc. If V = a constant, then E x = 0. The lines or surfaces on which V remains constant are called equipotential lines or surfaces. See example on next slide 1

22 Three examples Equipotential Surfaces What is the obvious equipotential surface and equipotential volume for an arbitrary shaped charged conductor? See physlet 9.3. Which equipotential surfaces fit the field lines?

x Blue lines are the electric field lines Orange dotted lines represent the equipotential surfaces a) Electric Dipole (ellipsoidal concentric

23 x Blue lines are the electric field lines Orange dotted lines represent the equipotential surfaces a) Electric Dipole (ellipsoidal concentric shells) b) Point charge (concentric shells) c) Uniform E field E = E x, E y = 0, E z = 0 E x = dv dx V = E x d V = constant in y and z directions 3

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26 Dielectric Breakdown: Application of Gauss s Law If the electric field in a gas exceeds a certain value, the gas breaks down and you get a spark or lightning bolt if the gas is air. In dry air at STP, you get a spark when E 3 " 10 4 V cm V = constant on surface of conductor Radius r r 1 1 6

27 This explains why: Sharp points on conductors have the highest electric fields and cause corona discharge or sparks. Pick up the most charge with charge tester from the pointy regions of the non-spherical conductor. Use non-spherical metal conductor charged with teflon rod. Show variation of charge across surface with charge tester. Radius R V = constant on surface of conductor Van de Graaff 1 Cloud

How does a conductor shield the interior from an exterior electric field? Start out with a uniform electric field with no excess charge on conductor.

28 How does a conductor shield the interior from an exterior electric field? Start out with a uniform electric field with no excess charge on conductor. Electrons on surface of conductor adjust so that: 1. E=0 inside conductor. Electric field lines are perpendicular to the surface. Suppose they weren t? 3. Does E = just outside the conductor 4. Is $ uniform over the surface? 5. Is the surface an equipotential? 6. If the surface had an excess charge, how would your answers change? " 0 8

29 A metal slab is put in a uniform electric field of 10 6 N/C with the field perpendicular to both surfaces. Show how the charges are distributed on the conductor. Draw the appropriate pill boxes. What is the charge density on each face of the slab? Apply Gauss s Law. E " da = q in # 0 9

30 What is the electric potential of a uniformly charged circular disk? We can treat the disk as a set of ring charges. The ring of radius R and thickness dr has an area of %R dr and it s charge is dq = $da = $(%R )dr where $=Q/(%R ), the surface charge density. The potential due to the charge on this ring at point P given by k V = Q (z + (R' ) ) The potential dv at a point P due to the charged ring of radius R is kdq k" R' dr' dv = = (z + (R' ) ) (z + (R' ) ) Integrating R from R =0 to R =R V = R 0 k# " R' dr' (z + (R' ) ) $ V = k"# ( z + R z) 30

Lecture 2 Electric Fields Chp. 22 Ed. 7

Lecture 2 Electric Fields Chp. 22 Ed. 7 Lecture Electric Fields Chp. Ed. 7 Cartoon - Analogous to gravitational field Warm-up problems, Physlet Topics Electric field Force per unit Charge Electric Field Lines Electric field from more than 1