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Figure 21-4 Lines of force between unlike charges (a, c) and between like charges (b, d) describe the behavior of a positively charged object in a field The top figures are computer tracings of electric field lines



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Robert Van de Graaff devised the high-voltage electrostatic generator in the 1930s Van de Graaff s machine, shown in Figure 21-3a on the previous page, is a device that transfers large amounts of charge from one part of the machine to a metal terminal at the top of the device Charge is transferred onto a moving belt at the base of the generator, position A, and is transferred off the belt at the metal dome at the top, position B An electric motor does the work needed to increase the electric potential energy A person touching the terminal of a Van de Graaff machine is charged electrically The charges on the person s hairs repel each other, causing the hairs to follow the field lines, as shown in Figure 21-3b Another method of visualizing field lines is to use grass seed in an insulating liquid, such as mineral oil The electric forces cause a separation of charge in each long, thin grass seed The seeds then turn so that they line up along the direction of the electric field The seeds thus form a pattern of the electric field lines, as in Figure 21-4 Field lines do not really exist They are simply a means of providing a model of an electric field Electric fields, on the other hand, do exist Although they provide a method of calculating the force on a charged body, they do not explain why charged bodies exert forces on each other





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There is a running controversy regarding how the antenna compares with other beam antennas, particularly the Yagi Some experts claim that the cubical quad has a gain of about 15 to 2 dB higher than a Yagi (with a comparable boom length between the two elements) In addition, some experts claim that the quad has a lower angle of radiation Most experts agree that the quad seems to work better at low heights above the earth s surface, but the difference disappears at heights greater than a half-wavelength The quad can be used as either a single-element antenna or in the form of a beam Figure 12-9 shows a pair of elements spaced 013 to 022 wavelengths apart One element is the driven element, and it is connected to the coaxial-cable feedline directly The other element is a reflector, so it is a bit longer than the driven element A tuning stub is used to adjust the reflector loop to resonance Because the wire is arranged into a square loop, one wavelength long, the actual length varies from the naturally resonant length by about 3 percent The driven

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11 Measuring Electric Fields Suppose you are asked to measure the electric field in space How do you detect the field at a point How do you determine the magnitude of the field How do you choose the magnitude of the test charge What do you do next 12 Field Strength and Direction A positive test charge of magnitude 240 10 8 C experiences a force of 150 10 3 N toward the east What is the electric field at the position of the test charge

2 public class Swanky { 3 Swanky s; 4 public static void main(String[] args) { 5 Swanky s1 = new Swanky(); 6 s1s = new Swanky(); 7 go(s1s); 8 Swanky s2 = go(s1); 9 if(s2sequals(s1)) Systemoutprint("1 "); 10 if(s2equals(s1)) Systemoutprint("2 "); 11 if(s1sequals(s1)) Systemoutprint("3 "); 12 if(s2sequals(s2)) Systemoutprint("4 "); 13 } 14 static Swanky go(Swanky s) { 15 Swanky gs = new Swanky(); 16 gss = s; 17 return gs; 18 } }

13 Field Lines In Figure 21-4, can you tell which charges are positive and which are negative What would you add to complete the field lines 14 Field Versus Force How does the electric field, E, at the test charge differ from the force, F, on it 15 Critical Thinking Suppose the top charge in Figure 21-2c is a test charge measuring the field resulting from the two negative charges Is it small enough to produce an accurate measure Explain

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