1. Chapter 18 Electrical Energy and Capacitance

2. Chapter 18 Objectives Electrical potential Electric Potential from a Point Charge Capacitance Parallel Plate Capacitor Dielectrics

3. Electrostatic Force Because the Coulomb force is the same as the gravitational force, it must also be conservative So it fits the rules of conservative energies –Δ PE + Δ KE = 0 Solving you see that change in potential is opposite to change in kinetic –Δ KE = - Δ PE Apply Work-Kinetic Energy Theorem –W = Δ KE –W = - Δ PE = -qEd

4. Electric Potential The electric potential is the change in potential energy of a charged object. –Often referred to as a potential difference. Because it is the difference in potential energies of a charged particle at differing locations. This can vary because of the magnitude of charge. Larger the charge, the more energy it has! –Potential energy divided by charge SI unit is Volt –V 1 V = 1 J / C –denoted by  V So the voltage is the measurement of the ability of the charge to be moved, not the actual motion itself. Δ V =V 2 -V 1 = Δ PE / q = -Ed or

5. Electric Potential Between Two Points Recall that in an electric field, electrons are transferred from positive to negative. So particles move from positive locations to negative locations. –So a positive charge gains electric potential energy when it is moved in a direction opposite the electric field. Because it is being pulled away from the “attractive” point, much like lifting a rock off the ground gives it more potential energy. –So a negative charge loses electric potential energy when it moves in a direction opposite the electric field. Because it is traveling away from the negative center which is what it wants to do anyways.

6. Potential Energy Between Points The potential energy created from those two points depends on the work done to move the charges –Opposite sign charges attract and work is negative –If the work is directly proportional to the separation between the charges. »So if the separation gets smaller, the work is negative. –Meaning the charges give off energy Same sign produces positive potential energy –Meaning energy added to system PE electric =kCkC q1q2q1q2 r This shows the electric potential energy due to point 1 created on point 2.

7. Electric Potential from Point Charge Every point in space has an electric potential, no matter what charge. The potential depends on the size of the charge and how far the charge is from the reference point. – Electric potential is a scalar quantity, so direction does not matter. But the sign does. –So when asked to find the net electric potential, simply find the algebraic sum of the individual potentials. V = As distance increases, potential decreases kCkC q r

8. Equipotential Surfaces A surface on which all points have the same potential is called an equipotential surface. –No work is required to move a charge at constant speed while on the surface. –The electric field at every point on the surface acts perpendicular to that point on the surface. This really tells us that no matter the surface characteristics, a diagram can be drawn using each surface as a single point source.

9. Capacitance We can now set two conducting surfaces, each being a equipotential surface, close enough to each other to create an electric field. The two surfaces do not have the same potential difference, therefore work can be done between the two. –As the two surfaces are charging by an outside voltage source, electrons are being taken from one surface and transferred to the other surface through the battery. The charging will stop once the plates reach the same potential difference with each other that the terminals of the voltage source endure. –When the voltage source is removed, the capacitor now becomes the primary voltage source for the circuit. So capacitance is defined as the ratio of the charge between the conducting surfaces and the potential difference between surfaces. –Denoted by C –Measured in Farads, F But a Farad is actually a very large number –so we typically measure in the range of  F to pF. C = Q VV

10. Parallel-Plate Capacitor The most common design for a capacitor is to place two conducting plates parallel to each other and separated by a small distance. Distances of millimeters and smaller! By connecting opposite leads of a power source to each plate, the charges begin to line themselves up according to the potential difference of the battery. –Remember, the capacitor stops charging once it reaches the same voltage as the battery. Even when the battery is disconnected, the capacitor will maintain the potential difference of the battery until the two plates are again connected by a conducting material. C = 00 A d  0 = 8.85 x 10 -12 C 2 /(Nm 2 ) separation between the plates surface area of one plate permittivity of free space

11. Dielectrics The material between the plates of a parallel plate capacitor can effect the capacitance of the system. A dielectric is an insulating material that is placed in between plates of a capacitor to increase its capacitance. –Insulators are used because the plates can realign the charges on the surface of the insulator space for the charge to be stored. –That gives the opportunity for more charge to be transferred to the plates of the capacitor for more storage. ++++++++++ ---------- ++++++++++ ----------

12. Dielectric Constant Each material is different and has different abilities to give up electrons to help increase the capacitance. –That increase is a multiple factor called the dielectric constant, . So: This differs from the dielectric strength, which is the largest electric field a capacitor can hold. –There is no relationship between larger the constant, stronger the field. C = C0C0

13. Energy Stored in a Capacitor Due to the fact that the energy stored in a capacitor is directly related to the work required to transfer that charge from plate to plate, we see the following: –In order for work to be performed, there must be a potential difference between plates in order to carry the charge across. W =  V  Q –Thanks to the Work-Kinetic Energy Theorem, and seeing that Q is the equivalent of mass in the mechanics world W = ½ Q  V –Similar to kinetic energy in the mechanics world –We combine those to produce a series of equations that would help to find the energy stored in a capacitor PE = ½ Q  V = ½ C(  V) 2 = Q 2 / 2C