Chapter 3: Electric Potential

Chapter 3 Electric Potential 3.1 Potential and Potential Energy................................................................................. 1 3.2 Electric Potential in a Uniform Field....................................................................... 4 3.3 Electric Potential due to Point Charges ................................................................... 5 3.3.1 Potential Energy in a System of Charges.......................................................... 7 3.4 Continuous Charge Distribution .............................................................................. 8 3.5 Deriving Electric Field from the Electric Potential ................................................. 9 3.5.1 Gradient and Equipotentials............................................................................ 10 Example 3.1: Uniformly Charged Rod .................................................................... 12 Example 3.2: Uniformly Charged Ring ................................................................... 14 Example 3.3: Uniformly Charged Disk ................................................................... 15 Example 3.4: Calculating Electric Field from Electric Potential............................. 17 3.6 Summary................................................................................................................ 17 3.7 Problem-Solving Strategy: Calculating Electric Potential..................................... 19 3.8 Solved Problems .................................................................................................... 21 3.8.1 3.8.2 3.8.3 3.8.4 Electric Potential Due to a System of Two Charges....................................... 21 Electric Dipole Potential ................................................................................. 22 Electric Potential of an Annulus ..................................................................... 23 Charge Moving Near a Charged Wire ............................................................ 24 3.9 Conceptual Questions ............................................................................................ 25 3.10 Additional Problems ............................................................................................ 26 3.10.1 Cube .............................................................................................................. 26 3.10.2 Three Charges ............................................................................................... 26 3.10.3 Work Done on Charges................................................................................. 26 3.10.4 Calculating E from V .................................................................................... 27 3.10.5 Electric Potential of a Rod ............................................................................ 27 3.10.6 Electric Potential........................................................................................... 28 3.10.7 Calculating Electric Field from the Electric Potential .................................. 28 3.10.8 Electric Potential and Electric Potential Energy........................................... 29 3.10.9. Electric Field, Potential and Energy ............................................................. 29 0 Electric Potential 3.1 Potential and Potential Energy In the introductory mechanics course, we have seen that gravitational force from the Earth on a particle of mass m located at a distance r from Earth’s center has an inversesquare form: Fg = −G Mm rˆ r2 (3.1.1) where G = 6.67 ×10− 11 N ⋅ m 2 /kg 2 is the gravitational constant and r̂ is a unit vector pointing radially outward. The Earth is assumed to be a uniform sphere of mass M. The corresponding gravitational field g , defined as the gravitational force per unit mass, is given by g= Fg m =− GM rˆ r2 (3.1.2) Notice that g only depends on M, the mass which creates the field, and r, the distance from M. Figure 3.1.1 Consider moving a particle of mass m under the influence of gravity (Figure 3.1.1). The work done by gravity in moving m from A to B is ⎡ GMm GMm Wg = ∫ Fg ⋅ d s = ∫ ⎛⎜ − 2 ⎞⎟ dr = rA ⎝ r ⎠ ⎣⎢ rB r ⎤ ⎦⎥ rB rA ⎛ 1 1 ⎞ = GMm ⎜ − ⎟ ⎝ rB rA ⎠ (3.1.3) The result shows that Wg is independent of the path taken; it depends only on the endpoints A and B. It is important to draw distinction between Wg , the work done by the 1 field and Wext , the work done by an external agent such as you. They simply differ by a negative sign: Wg = −Wext . Near Earth’s surface, the gravitational field g is approximately constant, with a magnitude g = GM / rE 2 ≈ 9.8 m/s 2 , where rE is the radius of Earth. The work done by gravity in moving an object from height y A to yB (Figure 3.1.2) is B B yB A A yA Wg = ∫ Fg ⋅ d s = ∫ mg cos θ ds = − ∫ mg cos φ ds = − ∫ mg dy = − mg ( yB − y A ) (3.1.4) Figure 3.1.2 Moving a mass m from A to B. The result again is independent of the path, and is only a function of the change in vertical height yB − y A . In the examples above, if the path forms a closed loop, so that the object moves around and then returns to where it starts off, the net work done by the gravitational field would be zero, and we say that the gravitational force is conservative. More generally, a force F is said to be conservative if its line integral around a closed loop vanishes: v∫ G G F⋅d s = 0 (3.1.5) When dealing with a conservative force, it is often convenient to introduce the concept of potential energy U. The change in potential energy associated with a conservative force F acting on an object as it moves from A to B is defined as: B ∆U = U B − U A = − ∫ F ⋅ d s = −W A (3.1.6) where W is the work done by the force on the object. In the case of gravity, W = Wg and from Eq. (3.1.3), the potential energy can be written as Ug = − GMm + U0 r (3.1.7) 2 where U 0 is an arbitrary constant which depends on a reference point. It is often convenient to choose a reference point where U 0 is equal to zero. In the gravitational case, we choose infinity to be the reference point, with U 0 (r = ∞) = 0 . Since U g depends on the reference point chosen, it is only the potential energy difference ∆U g that has physical importance. Near Earth’s surface where the gravitational field g is approximately constant, as an object moves from the ground to a height h, the change in potential energy is ∆U g = + mgh , and the work done by gravity is Wg = − mgh . A concept which is closely related to potential energy is “potential.” From ∆U , the gravitational potential can be obtained as ∆Vg = ∆U g m B B A A = − ∫ (Fg / m) ⋅ d s = − ∫ g ⋅ d s (3.1.8) Physically ∆Vg represents the negative of the work done per unit mass by gravity to move a particle from A to B . Our treatment of electrostatics is remarkably similar to gravitation. The electrostatic force JG F e given by Coulomb’s law also has an inverse-square form. In addition, it is also conservative. In the presence of an electric field E , in analogy to the gravitational field g , we define the electric potential difference between two points A and B as B B A A ∆V = − ∫ (Fe / q0 ) ⋅ d s = − ∫ E ⋅ d s (3.1.9) where q0 is a test charge. The potential difference ∆V represents the amount of work done per unit charge to move a test charge q0 from point A to B, without changing its kinetic energy. Again, electric potential should not be confused with electric potential energy. The two quantities are related by ∆ U = q0 ∆ V (3.1.10) The SI unit of electric potential is volt (V): 1volt = 1 joule/coulomb (1 V= 1 J/C) (3.1.11) When dealing with systems at the atomic or molecular scale, a joule (J) often turns out to be too large as an energy unit. A more useful scale is electron volt (eV), which is defined as the energy an electron acquires (or loses) when moving through a potential difference of one volt: 3 1eV = (1.6 × 10−19 C)(1V) = 1.6 ×10−19 J (3.1.12) 3.2 Electric Potential in a Uniform Field Consider a charge + q moving in the direction of a uniform electric field E = E0 (−ˆj) , as shown in Figure 3.2.1(a). (b) (a) Figure 3.2.1 (a) A charge q which moves in the direction of a constant electric field E . (b) A mass m that moves in the direction of a constant gravitational field g . Since the path taken is parallel to E , the potential difference between points A and B is given by B B A A ∆V = VB − VA = − ∫ E ⋅ d s = − E0 ∫ ds = − E0 d < 0 (3.2.1) implying that point B is at a lower potential compared to A. In fact, electric field lines always point from higher potential to lower. The change in potential energy is ∆ U = U B − U A = − qE0 d . Since q > 0, we have ∆U < 0 , which implies that the potential energy of a positive charge decreases as it moves along the direction of the electric field. The corresponding gravitational analogy, depicted in Figure 3.2.1(b), is that a mass m loses potential energy ( ∆ U = − mgd ) as it moves in the direction of the gravitational field g . Figure 3.2.2 Potential difference due to a uniform electric field What happens if the path from A to B is not parallel to E , but instead at an angle θ, as shown in Figure 3.2.2? In that case, the potential difference becomes 4 B ∆V = VB − VA = − ∫ E ⋅ d s = −E ⋅ s = − E0 s cos θ = − E0 y A (3.2.2) Note that y increase downward in Figure 3.2.2. Here we see once more that moving along the direction of the electric field E leads to a lower electric potential. What would the change in potential be if the path were A → C → B ? In this case, the potential difference consists of two contributions, one for each segment of the path: ∆V = ∆VCA + ∆VBC (3.2.3) When moving from A to C, the change in potential is ∆VCA = − E0 y . On the other hand, when going from C to B, ∆VBC = 0 since the path is perpendicular to the direction of E . Thus, the same result is obtained irrespective of the path taken, consistent with the fact that E is conservative. Notice that for the path A → C → B , work is done by the field only along the segment AC which is parallel to the field lines. Points B and C are at the same electric potential, i.e., VB = VC . Since ∆U = q∆V , this means that no work is required in moving a charge from B to C. In fact, all points along the straight line connecting B and C are on the same “equipotential line.” A more complete discussion of equipotential will be given in Section 3.5. 3.3 Electric Potential due to Point Charges Next, let’s compute the potential difference between two points A and B due to a charge +Q. The electric field produced by Q is E = (Q / 4πε 0 r 2 )rˆ , where r̂ is a unit vector pointing toward the field point. Figure 3.3.1 Potential difference between two points due to a point charge Q. From Figure 3.3.1, we see that rˆ ⋅ d s = ds cos θ = dr , which gives ∆ V = VB − VA = − ∫ B A Q 4πε 0 r 2 rˆ ⋅ d s = − ∫ B A Q 4πε 0 r 2 dr = Q ⎛ 1 1 ⎞ ⎜ − ⎟ 4πε 0 ⎝ rB rA ⎠ (3.3.1) 5 Once again, the potential difference ∆V depends only on the endpoints, independent of the choice of path taken. As in the case of gravity, only the difference in electrical potential is physically meaningful, and one may choose a reference point and set the potential there to be zero. In practice, it is often convenient to choose the reference point to be at infinity, so that the electric potential at a point P becomes P VP = − ∫ E ⋅ d s (3.3.2) ∞ With this reference, the electric potential at a distance r away from a point charge Q becomes 1 Q 4πε 0 r V (r ) = (3.3.3) When more than one point charge is present, by applying the superposition principle, the total electric potential is simply the sum of potentials due to individual charges: V (r ) = 1 4πε 0 qi ∑r i i = ke ∑ i qi ri (3.3.4) A summary of comparison between gravitation and electrostatics is tabulated below: Gravitation Electrostatics Mass m Charge q Gravitational force Fg = −G Mm rˆ r2 Gravitational field g = Fg / m B Potential energy change ∆ U = − ∫ Fg ⋅ d s A B Gravitational potential Vg = − ∫ g ⋅ d s A For a source M: Vg = − GM r | ∆ U g | = mg d (constant g ) Coulomb force Fe = ke Qq rˆ r2 Electric field E = Fe / q B Potential energy change ∆ U = − ∫ Fe ⋅ d s A B Electric Potential V = − ∫ E ⋅ d s A For a source Q: V = ke Q r | ∆ U | = qEd (constant E ) 6 3.3.1 Potential Energy in a System of Charges If a system of charges is assembled by an external agent, then ∆ U = −W = +Wext . That is, the change in potential energy of the system is the work that must be put in by an external agent to assemble the configuration. A simple example is lifting a mass m through a height h. The work done by an external agent  you, is + mgh (The gravitational field does work − mgh ). The charges are brought in from infinity without acceleration i.e. they are at rest at the end of the process. Let’s start with just two charges q1 and q2 . Let the potential due to q1 at a point P be V1 (Figure 3.3.2). Figure 3.3.2 Two point charges separated by a distance r12 . The work W2 done by an agent in bringing the second charge q2 from infinity to P is then W2 = q2V1 . (No work is required to set up the first charge and W1 = 0 ). Since V1 = q1 / 4πε 0 r12 , where r12 is the distance measured from q1 to P, we have U12 = W2 = 1 q1q2 4πε 0 r12 (3.3.5) If q1 and q2 have the same sign, positive work must be done to overcome the electrostatic repulsion and the potential energy of the system is positive, U12 > 0 . On the other hand, if the signs are opposite, then U12 < 0 due to the attractive force between the charges. Figure 3.3.3 A system of three point charges. To add a third charge q3 to the system (Figure 3.3.3), the work required is 7 W3 = q3 ( V1 + V2 ) = q3 ⎛ q1 q2 ⎞ ⎜ + ⎟ 4πε 0 ⎝ r13 r23 ⎠ (3.3.6) The potential energy of this configuration is then U = W2 + W3 = 1 ⎛ q1q2 q1q3 q2 q3 + + ⎜ 4πε 0 ⎝ r12 r13 r23 ⎞ ⎟ = U12 + U13 + U 23 ⎠ (3.3.7) The equation shows that the total potential energy is simply the sum of the contributions from distinct pairs. Generalizing to a system of N charges, we have U= 1 4πε 0 N N ∑∑ i =1 j =1 j >i qi q j rij (3.3.8) where the constraint j > i is placed to avoid double counting each pair. Alternatively, one may count each pair twice and divide the result by 2. This leads to U= 1 8πε 0 N N ∑∑ i =1 j =1 j ≠i qi q j rij ⎛ 1 N ⎜ 1 = ∑ qi 2 i =1 ⎜⎜ 4πε 0 ⎝ ⎞ qj ⎟ 1 N qiV (ri ) = ∑ ⎟ 2∑ j =1 rij ⎟ i =1 j ≠i ⎠ N (3.3.9) where V (ri ) , the quantity in the parenthesis, is the potential at ri (location of qi) due to all the other charges. 3.4 Continuous Charge Distribution If the charge distribution is continuous, the potential at a point P can be found by summing over the contributions from individual differential elements of charge dq . Figure 3.4.1 Continuous charge distribution 8 Consider the charge distribution shown in Figure 3.4.1. Taking infinity as our reference point with zero potential, the electric potential at P due to dq is dV = 1 dq 4πε 0 r (3.4.1) Summing over contributions from all differential elements, we have V= 1 4πε 0 ∫ dq r (3.4.2) 3.5 Deriving Electric Field from the Electric Potential In Eq. (3.1.9) we established the relation between E and V. If we consider two points which are separated by a small distance ds , the following differential form is obtained: dV = −E ⋅ d s (3.5.1) In Cartesian coordinates, E = Ex ˆi + E y ˆj + Ez kˆ and d s = dx ˆi + dyˆj + dz kˆ , we have ( )( ) dV = Ex ˆi + E y ˆj + Ez kˆ ⋅ dx ˆi + dyˆj + dz kˆ = Ex dx + E y dy + Ez dz (3.5.2) which implies Ex = − ∂V ∂V ∂V , Ey = − , Ez = − ∂x ∂y ∂z (3.5.3) By introducing a differential quantity called the “del (gradient) operator” ∇≡ ∂ ˆ ∂ ˆ ∂ ˆ j+ k i+ ∂x ∂y ∂z (3.5.4) the electric field can be written as ⎛ ∂V ˆ ∂V ˆ ∂V ˆ ⎞ ⎛ ∂ ˆ ∂ ˆ ∂ ˆ⎞ E = Ex ˆi + E y ˆj + Ez kˆ = − ⎜ i+ j+ k ⎟ = −⎜ i+ j + k ⎟ V = −∇ V ∂y ∂z ⎠ ∂y ∂z ⎠ ⎝ ∂x ⎝ ∂x E = −∇ V (3.5.5) Notice that ∇ operates on a scalar quantity (electric potential) and results in a vector quantity (electric field). Mathematically, we can think of E as the negative of the gradient of the electric potential V . Physically, the negative sign implies that if 9 V increases as a positive charge moves along some direction, say x, with ∂V / ∂x > 0 , then there is a non-vanishing component of E in the opposite direction (− Ex ≠ 0) . In the case of gravity, if the gravitational potential increases when a mass is lifted a distance h, the gravitational force must be downward. If the charge distribution possesses spherical symmetry, then the resulting electric field is a function of the radial distance r, i.e., E = Er rˆ . In this case, dV = − Er dr. If V ( r ) is known, then E may be obtained as ⎛ dV ⎞ E = Er rˆ = − ⎜ ⎟ r̂ ⎝ dr ⎠ (3.5.6) For example, the electric potential due to a point charge q is V (r ) = q / 4πε 0 r . Using the above formula, the electric field is simply E = (q / 4πε 0 r 2 )rˆ . 3.5.1 Gradient and Equipotentials Suppose a system in two dimensions has an electric potential V ( x, y ) . The curves characterized by constant V ( x, y ) are called equipotential curves. Examples of equipotential curves are depicted in Figure 3.5.1 below. Figure 3.5.1 Equipotential curves In three dimensions we have equipotential surfaces and they are described by V ( x, y , z ) =constant. Since E = −∇ V , we can show that the direction of E is always perpendicular to the equipotential through the point. Below we give a proof in two dimensions. Generalization to three dimensions is straightforward. Proof: Referring to Figure 3.5.2, let the potential at a point P ( x, y ) be V ( x, y ) . How much is V changed at a neighboring point P ( x + dx, y + dy ) ? Let the difference be written as 10 dV = V ( x + dx, y + dy ) − V ( x, y ) ⎡ ∂V ∂V = ⎢ V ( x, y ) + dx + dy + ∂x ∂y ⎣ ⎤ ∂V ∂V ⎥ − V ( x, y ) ≈ ∂ x dx + ∂ y dy ⎦ (3.5.7) Figure 3.5.2 Change in V when moving from one equipotential curve to another With the displacement vector given by d s = dx ˆi + dy ĵ , we can rewrite dV as ⎛ ∂V ˆ ∂V dV = ⎜ i+ ∂y ⎝ ∂x ˆj ⎞ ⋅ dx ˆi + dyˆj = (∇ V ) ⋅ d s = −E ⋅ d s ⎟ ⎠ ( ) (3.5.8) If the displacement ds is along the tangent to the equipotential curve through P(x,y), then dV = 0 because V is constant everywhere on the curve. This implies that E ⊥ d s along the equipotential curve. That is, E is perpendicular to the equipotential. In Figure 3.5.3 we illustrate some examples of equipotential curves. In three dimensions they become equipotential surfaces. From Eq. (3.5.8), we also see that the change in potential dV attains a maximum when the gradient ∇ V is parallel to d s : ⎛ dV ⎞ max ⎜ ⎟ = ∇V ⎝ ds ⎠ (3.5.9) Physically, this means that ∇ V always points in the direction of maximum rate of change of V with respect to the displacement s. Figure 3.5.3 Equipotential curves and electric field lines for (a) a constant E field, (b) a point charge, and (c) an electric dipole. 11 The properties of equipotential surfaces can be summarized as follows: (i) The electric field lines are perpendicular to the equipotentials and point from higher to lower potentials. (ii) By symmetry, the equipotential surfaces produced by a point charge form a family of concentric spheres, and for constant electric field, a family of planes perpendicular to the field lines. (iii) The tangential component of the electric field along the equipotential surface is zero, otherwise non-vanishing work would be done to move a charge from one point on the surface to the other. (iv) No work is required to move a particle along an equipotential surface. A useful analogy for equipotential curves is a topographic map (Figure 3.5.4). Each contour line on the map represents a fixed elevation above sea level. Mathematically it is expressed as z = f ( x, y ) = constant . Since the gravitational potential near the surface of Earth is Vg = gz , these curves correspond to gravitational equipotentials. Figure 3.5.4 A topographic map Example 3.1: Uniformly Charged Rod Consider a non-conducting rod of length having a uniform charge density λ . Find the electric potential at P , a perpendicular distance y above the midpoint of the rod. Figure 3.5.5 A non-conducting rod of length and uniform charge density λ . 12 Solution: Consider a differential element of length dx′ which carries a charge dq = λ dx′ , as shown in Figure 3.5.5. The source element is located at ( x′, 0) , while the field point P is located on the y-axis at (0 , y ) . The distance from dx′ to P is r = ( x′2 + y 2 )1/ 2 . Its contribution to the potential is given by dq 1 λ dx′ = 4πε 0 r 4πε 0 ( x′2 + y 2 )1/ 2 1 dV = Taking V to be zero at infinity, the total potential due to the entire rod is V= λ 4πε 0 ∫ /2 − /2 dx′ x ′2 + y 2 = λ ln ⎡ x′ + x′2 + y 2 ⎤ ⎦ 4πε 0 ⎣ ⎡ ( / 2) + ( / 2) 2 + y 2 λ = ln ⎢ 4πε 0 ⎢ −( / 2) + ( / 2) 2 + y 2 ⎣ ⎤ ⎥ ⎥⎦ /2 − /2 (3.5.10) where we have used the integration formula ∫ dx′ x′ + y 2 2 ( = ln x′ + x′2 + y 2 A plot of V ( y ) / V0 , where V0 = λ / 4πε 0 , as a function of y / ) is shown in Figure 3.5.6 Figure 3.5.6 Electric potential along the axis that passes through the midpoint of a nonconducting rod. In the limit  y , the potential becomes 13 ⎡ ( / 2) + / 2 1 + (2 y / ) 2 ⎤ ⎡ 1 + 1 + (2 y / ) 2 λ λ V= ln ⎢ ln ⎢ ⎥= 4πε 0 ⎢ −( / 2) + / 2 1 + (2 y / ) 2 ⎥ 4πε 0 ⎢ − 1 + 1 + (2 y / ) 2 ⎣ ⎦ ⎣ ≈ ⎛ 2 λ ln ⎜ 2 4πε 0 ⎝ 2 y / = ⎛ ⎞ λ ln ⎜ ⎟ 2πε 0 ⎝ y ⎠ 2 ⎛ 2 ⎞ ⎞ λ ln = ⎜ 2⎟ ⎟ ⎠ 4πε 0 ⎝ y ⎠ ⎤ ⎥ ⎥⎦ (3.5.11) The corresponding electric field can be obtained as Ey = − ∂V λ = ∂ y 2πε 0 y /2 ( / 2) 2 + y 2 in complete agreement with the result obtained in Eq. (2.10.9). Example 3.2: Uniformly Charged Ring Consider a uniformly charged ring of radius R and charge density λ (Figure 3.5.7). What is the electric potential at a distance z from the central axis? Figure 3.5.7 A non-conducting ring of radius R with uniform charge density λ . Solution: Consider a small differential element d = R dφ ′ on the ring. The element carries a charge dq = λ d = λ R dφ ′ , and its contribution to the electric potential at P is dV = dq 1 λ R dφ ′ = 4πε 0 r 4πε 0 R 2 + z 2 1 The electric potential at P due to the entire ring is 14 V = ∫ dV = λR 1 4πε 0 2πλ R 1 R2 + z2 ∫ dφ ′ = 4πε 0 R2 + z2 = 1 4πε 0 Q R2 + z2 (3.5.12) where we have substituted Q = 2π Rλ for the total charge on the ring. In the limit z the potential approaches its “point-charge” limit: V≈ R, 1 Q 4πε 0 z From Eq. (3.5.12), the z-component of the electric field may be obtained as Ez = − ∂V ∂ ⎛ 1 =− ⎜ ∂z ∂ z ⎝ 4πε 0 ⎞ 1 Qz ⎟= 2 2 3/ 2 2 2 R + z ⎠ 4πε 0 ( R + z ) Q (3.5.13) in agreement with Eq. (2.10.14). Example 3.3: Uniformly Charged Disk Consider a uniformly charged disk of radius R and charge density σ lying in the xyplane. What is the electric potential at a distance z from the central axis? Figure 3.4.3 A non-conducting disk of radius R and uniform charge density σ. Solution: Consider a circular ring of radius r ′ and width dr ′ . The charge on the ring is dq′ = σ dA′ = σ (2π r ′dr ′). The field point P is located along the z -axis a distance z from the plane of the disk. From the figure, we also see that the distance from a point on the ring to P is r = (r ′2 + z 2 )1/ 2 . Therefore, the contribution to the electric potential at P is dV = dq 1 σ (2π r ′dr ′) = 4πε 0 r 4πε 0 r ′2 + z 2 1 15 By summing over all the rings that make up the disk, we have V= In the limit | z | σ 4πε 0 ∫ R 2π r ′dr ′ r ′2 + z 2 0 = σ ⎡ 2 2⎤ r′ + z ⎦ 2ε 0 ⎣ R = 0 σ ⎡ 2 2 R + z − | z |⎤ ⎦ 2ε 0 ⎣ (3.5.14) R, 1/ 2 ⎛ R2 ⎞ R + z =| z | ⎜ 1 + 2 ⎟ z ⎠ ⎝ 2 2 ⎛ R2 =| z | ⎜ 1 + 2 + 2z ⎝ ⎞ ⎟, ⎠ and the potential simplifies to the point-charge limit: V≈ σ R2 1 σ (π R 2 ) 1 Q ⋅ = = 2ε 0 2 | z | 4πε 0 | z | 4πε 0 | z | As expected, at large distance, the potential due to a non-conducting charged disk is the same as that of a point charge Q. A comparison of the electric potentials of the disk and a point charge is shown in Figure 3.4.4. Figure 3.4.4 Comparison of the electric potentials of a non-conducting disk and a point charge. The electric potential is measured in terms of V0 = Q / 4πε 0 R . Note that the electric potential at the center of the disk ( z = 0 ) is finite, and its value is Vc = σR Q R 1 2Q = ⋅ = = 2V0 2 2ε 0 π R 2ε 0 4πε 0 R (3.5.15) This is the amount of work that needs to be done to bring a unit charge from infinity and place it at the center of the disk. The corresponding electric field at P can be obtained as: Ez = − σ ∂V = ∂ z 2ε 0 ⎡ z ⎤ z − ⎢ ⎥ R2 + z 2 ⎦ ⎣| z| (3.5.16) 16 which agrees with Eq. (2.10.18). In the limit R  z , the above equation becomes Ez = σ / 2ε 0 , which is the electric field for an infinitely large non-conducting sheet. Example 3.4: Calculating Electric Field from Electric Potential Suppose the electric potential due to a certain charge distribution can be written in Cartesian Coordinates as V ( x, y, z ) = Ax 2 y 2 + Bxyz where A , B and C are constants. What is the associated electric field? Solution: The electric field can be found by using Eq. (3.5.3): ∂V = −2 Axy 2 − Byz ∂x ∂V Ey = − = −2 Ax 2 y − Bxz ∂y ∂V Ez = − = − Bxy ∂z Ex = − Therefore, the electric field is E = ( −2 Axy 2 − Byz ) ˆi − (2 Ax 2 y + Bxz ) ˆj − Bxy kˆ . 3.6 Summary • A force F is conservative if the line integral of the force around a closed loop vanishes: ∫ F⋅d s = 0 • The change in potential energy associated with a conservative force F acting on an object as it moves from A to B is B ∆U = U B − U A = − ∫ F ⋅ d s A 17 • The electric potential difference ∆V between points A and B in an electric field E is given by ∆V = VB − VA = B ∆U = −∫ E ⋅ ds A q0 The quantity represents the amount of work done per unit charge to move a test charge q0 from point A to B, without changing its kinetic energy. • The electric potential due to a point charge Q at a distance r away from the charge is V= 1 Q 4πε 0 r For a collection of charges, using the superposition principle, the electric potential is V= • 1 4πε 0 Qi ∑r i i The potential energy associated with two point charges q1 and q2 separated by a distance r12 is U= • 1 q1q2 4πε 0 r12 From the electric potential V , the electric field may be obtained by taking the gradient of V : E = −∇V In Cartesian coordinates, the components may be written as Ex = − • ∂V ∂V ∂V , Ey = − , Ez = − ∂x ∂y ∂z The electric potential due to a continuous charge distribution is V= 1 4πε 0 ∫ dq r 18 3.7 Problem-Solving Strategy: Calculating Electric Potential In this chapter, we showed how electric potential can be calculated for both the discrete and continuous charge distributions. Unlike electric field, electric potential is a scalar quantity. For the discrete distribution, we apply the superposition principle and sum over individual contributions: V = ke ∑ i qi ri For the continuous distribution, we must evaluate the integral V = ke ∫ dq r In analogy to the case of computing the electric field, we use the following steps to complete the integration: (1) Start with dV = ke dq . r (2) Rewrite the charge element dq as ⎧λ dl ⎪ dq = ⎨σ dA ⎪ ρ dV ⎩ (length) (area) (volume) depending on whether the charge is distributed over a length, an area, or a volume. (3) Substitute dq into the expression for dV . (4) Specify an appropriate coordinate system and express the differential element (dl, dA or dV ) and r in terms of the coordinates (see Table 2.1.) (5) Rewrite dV in terms of the integration variable. (6) Complete the integration to obtain V. Using the result obtained for V , one may calculate the electric field by E = −∇V . Furthermore, the accuracy of the result can be readily checked by choosing a point P which lies sufficiently far away from the charge distribution. In this limit, if the charge distribution is of finite extent, the field should behave as if the distribution were a point charge, and falls off as 1/ r 2 . 19 Below we illustrate how the above methodologies can be employed to compute the electric potential for a line of charge, a ring of charge and a uniformly charged disk. Charged Rod Charged Ring Charged disk dq = λ dx′ dq = λ dl dq = σ dA Figure (2) Express dq in terms of charge density (3) Substitute dq into expression for dV (4) Rewrite r and the differential element in terms of the appropriate coordinates V= (6) Integrate to get V Derive E from V Point-charge for E limit dV = ke r λ dl dV = ke r σ dA r dx′ dl = R dφ ′ dA = 2π r ′ dr ′ r = x′2 + y 2 r = R2 + z2 r = r ′2 + z 2 dV = ke (5) Rewrite dV λ dx′ dV = ke λ 4πε0 ∫− /2 /2 λ dx′ 2 1/ 2 V = ke dx′ x′2 + y2 ⎡ ( / 2) + ( / 2)2 + y2 λ ln ⎢ = 4πε0 ⎢ −( / 2) + ( / 2)2 + y2 ⎣ Ey = − ∂V ∂y λ /2 = 2πε 0 y ( / 2) 2 + y 2 Ey ≈ dV = ke ( x′ + y ) 2 ke Q y2 y ⎤ ⎥ ⎥⎦ = ke = ke Ez = − Ez ≈ λ R dφ ′ (R + z ) 2 2 1/ 2 Rλ ( R + z 2 )1/ 2 (2π Rλ ) 2 ∫ dφ ′ R +z keQz ∂V = ∂z ( R 2 + z 2 )3/ 2 ke Q z2 z R R 0 = 2 2πσ r ′ dr ′ (r ′2 + z 2 )1/ 2 V = ke 2πσ ∫ = 2keπσ R2 + z 2 Q 2 dV = ke Ez = − ( r′ dr′ (r′ + z2 )1/2 2 ) z2 + R2 − | z | ) ( 2keQ 2 2 z + R −| z | R2 ⎞ ∂V 2keQ ⎛ z z = 2 ⎜ − ⎟ R ⎝| z | ∂z z 2 + R2 ⎠ Ez ≈ ke Q z2 z R 20 3.8 Solved Problems 3.8.1 Electric Potential Due to a System of Two Charges Consider a system of two charges shown in Figure 3.8.1. Figure 3.8.1 Electric dipole Find the electric potential at an arbitrary point on the x axis and make a plot. Solution: The electric potential can be found by the superposition principle. At a point on the x axis, we have V ( x) = 1 (−q ) 1 ⎤ q q ⎡ 1 + = − ⎢ 4πε 0 | x − a | 4πε 0 | x + a | 4πε 0 ⎣ | x − a | | x + a | ⎥⎦ 1 The above expression may be rewritten as V ( x) 1 1 = − V0 | x / a − 1| | x / a + 1| where V0 = q / 4πε 0 a . The plot of the dimensionless electric potential as a function of x/a. is depicted in Figure 3.8.2. Figure 3.8.2 21 As can be seen from the graph, V ( x ) diverges at x / a = ±1 , where the charges are located. 3.8.2 Electric Dipole Potential Consider an electric dipole along the y-axis, as shown in the Figure 3.8.3. Find the electric potential V at a point P in the x-y plane, and use V to derive the corresponding electric field. Figure 3.8.3 By superposition principle, the potential at P is given by V = ∑ Vi = i 1 ⎛ q q ⎞ ⎜ − ⎟ 4πε 0 ⎝ r+ r− ⎠ where r± 2 = r 2 + a 2 ∓ 2ra cos θ . If we take the limit where r a, then −1/ 2 1 1 1⎡ 1 = ⎡⎣ 1 + (a / r ) 2 ∓ 2(a / r ) cos θ ⎤⎦ = ⎢ 1 − (a / r ) 2 ± (a / r ) cos θ + r± r r⎣ 2 ⎤ ⎥ ⎦ and the dipole potential can be approximated as 1 ⎡ 1 1 − (a / r ) 2 + (a / r ) cos θ − 1 + (a / r ) 2 + (a / r ) cos θ + ⎢ 4πε 0 r ⎣ 2 2 q p ⋅ rˆ 2a cos θ p cos θ ≈ ⋅ = = 2 r 4πε 0 r 4πε 0 r 4πε 0 r 2 V= q ⎤ ⎥⎦ where p = 2aq ˆj is the electric dipole moment. In spherical polar coordinates, the gradient operator is ∇= ∂ 1 ∂ ˆ 1 ∂ rˆ + θ+ φˆ ∂r r ∂θ r sin θ ∂ φ 22 Since the potential is now a function of both r and θ , the electric field will have components along the r̂ and θ̂ directions. Using E = −∇V , we have Er = − ∂ V p cos θ 1 ∂ V p sin θ = , Eθ = − = , Eφ = 0 3 ∂ r 2πε 0 r r ∂ θ 4πε 0 r 3 3.8.3 Electric Potential of an Annulus Consider an annulus of uniform charge density σ , as shown in Figure 3.8.4. Find the electric potential at a point P along the symmetric axis. Figure 3.8.4 An annulus of uniform charge density. Solution: Consider a small differential element dA at a distance r away from point P. The amount of charge contained in dA is given by dq = σ dA = σ ( r ' dθ ) dr ' Its contribution to the electric potential at P is dV = dq 1 σ r ' dr ' dθ = 4πε 0 r 4πε 0 r '2 + z 2 1 Integrating over the entire annulus, we obtain V= σ 4πε 0 b 2π a 0 ∫∫ r ' dr ' dθ r '2 + z 2 = 2πσ 4πε 0 ∫ b a r ' ds r '2 + z 2 = σ ⎡ 2 2 b + z − a2 + z2 ⎤ ⎣ ⎦ 2ε 0 where we have made used of the integral 23 ds s ∫ s +z 2 2 = s2 + z 2 Notice that in the limit a → 0 and b → R , the potential becomes V= σ ⎡ 2 2 R + z − | z |⎤ ⎦ 2ε 0 ⎣ which coincides with the result of a non-conducting disk of radius R shown in Eq. (3.5.14). 3.8.4 Charge Moving Near a Charged Wire A thin rod extends along the z-axis from z = −d to z = d . The rod carries a positive charge Q uniformly distributed along its length 2d with charge density λ = Q / 2d . (a) Calculate the electric potential at a point z > d along the z-axis. (b) What is the change in potential energy if an electron moves from z = 4d to z = 3d ? (c) If the electron started out at rest at the point z = 4d , what is its velocity at z = 3d ? Solutions: (a) For simplicity, let’s set the potential to be zero at infinity, V (∞) = 0 . Consider an infinitesimal charge element dq = λ dz ′ located at a distance z ' along the z-axis. Its contribution to the electric potential at a point z > d is dV = λ dz ' 4πε 0 z − z ' Integrating over the entire length of the rod, we obtain V ( z) = λ z −d dz' λ ⎛ z+d ⎞ ln ⎜ = ⎟ ∫ 4πε 0 z + d z − z' 4πε 0 ⎝ z − d ⎠ (b) Using the result derived in (a), the electrical potential at z = 4d is V ( z = 4d ) = λ λ ⎛ 4d + d ⎞ ⎛5⎞ ln ⎜ ln ⎜ ⎟ ⎟= 4πε 0 ⎝ 4d − d ⎠ 4πε 0 ⎝ 3 ⎠ Similarly, the electrical potential at z = 3d is 24 V ( z = 3d ) = λ λ ⎛ 3d + d ⎞ ln ⎜ ln 2 ⎟= 4πε 0 ⎝ 3d − d ⎠ 4πε 0 The electric potential difference between the two points is ∆V = V ( z = 3d ) − V ( z = 4d ) = λ ⎛6⎞ ln ⎜ ⎟ > 0 4πε 0 ⎝ 5 ⎠ Using the fact that the electric potential difference ∆V is equal to the change in potential energy per unit charge, we have ∆U = q∆V = − |e|λ ⎛6⎞ ln ⎜ ⎟ < 0 4πε 0 ⎝ 5 ⎠ where q = − | e | is the charge of the electron. (c) If the electron starts out at rest at z = 4d then the change in kinetic energy is 1 ∆K = mv f 2 2 By conservation of energy, the change in kinetic energy is ∆K = −∆U = |e|λ ⎛6⎞ ln ⎜ ⎟ > 0 4πε 0 ⎝ 5 ⎠ Thus, the magnitude of the velocity at z = 3d is vf = 2|e| λ ⎛ 6⎞ ln ⎜ ⎟ 4πε 0 m ⎝ 5 ⎠ 3.9 Conceptual Questions 1. What is the difference between electric potential and electric potential energy? 2. A uniform electric field is parallel to the x-axis. In what direction can a charge be displaced in this field without any external work being done on the charge? 3. Is it safe to stay in an automobile with a metal body during severe thunderstorm? Explain. 25 4. Why are equipotential surfaces always perpendicular to electric field lines? 5. The electric field inside a hollow, uniformly charged sphere is zero. Does this imply that the potential is zero inside the sphere? 3.10 Additional Problems 3.10.1 Cube How much work is done to assemble eight identical point charges, each of magnitude q, at the corners of a cube of side a? 3.10.2 Three Charges Three charges with q = 3.00 × 10−18 C and q1 = 6 × 10 −6 C are placed on the x-axis, as shown in the figure 3.10.1. The distance between q and q1 is a = 0.600 m. Figure 3.10.1 (a) What is the net force exerted on q by the other two charges q1? (b) What is the electric field at the origin due to the two charges q1? (c) What is the electric potential at the origin due to the two charges q1? 3.10.3 Work Done on Charges Two charges q1 = 3.0 µ C and q2 = −4.0 µ C initially are separated by a distance r0 = 2.0 cm . An external agent moves the charges until they are rf = 5.0 cm apart. (a) How much work is done by the electric field in moving the charges from r0 to rf ? Is the work positive or negative? (b) How much work is done by the external agent in moving the charges from r0 to rf ? Is the work positive or negative? 26 (c) What is the potential energy of the initial state where the charges are r0 = 2.0 cm apart? (d) What is the potential energy of the final state where the charges are rf = 5.0 cm apart? (e) What is the change in potential energy from the initial state to the final state? 3.10.4 Calculating E from V Suppose in some region of space the electric potential is given by V ( x, y, z ) = V0 − E0 z + E0 a 3 z ( x 2 + y 2 + z 2 )3/ 2 where a is a constant with dimensions of length. Find the x, y, and the z-components of the associated electric field. 3.10.5 Electric Potential of a Rod A rod of length L lies along the x-axis with its left end at the origin and has a nonuniform charge density λ = α x ,where α is a positive constant. Figure 3.10.2 (a) What are the dimensions of α ? (b) Calculate the electric potential at A. (c) Calculate the electric potential at point B that lies along the perpendicular bisector of the rod a distance b above the x-axis. 27 3.10.6 Electric Potential Suppose that the electric potential in some region of space is given by V ( x, y, z ) = V0 exp(− k | z |) cos kx . Find the electric field everywhere. Sketch the electric field lines in the x − z plane. 3.10.7 Calculating Electric Field from the Electric Potential Suppose that the electric potential varies along the x-axis as shown in Figure 3.10.3 below. Figure 3.10.3 The potential does not vary in the y- or z -direction. Of the intervals shown (ignore the behavior at the end points of the intervals), determine the intervals in which Ex has (a) its greatest absolute value. [Ans: 25 V/m in interval ab.] (b) its least. [Ans: (b) 0 V/m in interval cd.] (c) Plot Ex as a function of x. (d) What sort of charge distributions would produce these kinds of changes in the potential? Where are they located? [Ans: sheets of charge extending in the yz direction located at points b, c, d, etc. along the x-axis. Note again that a sheet of charge with charge per unit area σ will always produce a jump in the normal component of the electric field of magnitude σ / ε 0 ]. 28 3.10.8 Electric Potential and Electric Potential Energy A right isosceles triangle of side a has charges q, +2q and −q arranged on its vertices, as shown in Figure 3.10.4. Figure 3.10.4 (a) What is the electric potential at point P, midway between the line connecting the +q and − q charges, assuming that V = 0 at infinity? [Ans: q/ 2 πεoa.] (b) What is the potential energy U of this configuration of three charges? What is the significance of the sign of your answer? [Ans: −q2/4 2 πεoa, the negative sign means that work was done on the agent who assembled these charges in moving them in from infinity.] (c) A fourth charge with charge +3q is slowly moved in from infinity to point P. How much work must be done in this process? What is the significance of the sign of your answer? [Ans: +3q2/ 2 πεoa, the positive sign means that work was done by the agent who moved this charge in from infinity.] 3.10.9. Electric Field, Potential and Energy Three charges, +5Q, −5Q, and +3Q are located on the y-axis at y = +4a, y = 0, and y = −4a , respectively. The point P is on the x-axis at x = 3a. (a) How much energy did it take to assemble these charges? (b) What are the x, y, and z components of the electric field E at P? (c) What is the electric potential V at point P, taking V = 0 at infinity? (d) A fourth charge of +Q is brought to P from infinity. What are the x, y, and z components of the force F that is exerted on it by the other three charges? (e) How much work was done (by the external agent) in moving the fourth charge +Q from infinity to P? 29