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Wave interference Wave interference can be either constructive or destructive When two pulses with equal but opposite amplitudes meet, the displacement of the medium at each point in the overlap region is reduced The superposition of waves with equal but opposite amplitudes causes destructive interference, as shown in Figure 14-13a When the pulses meet and are in the same location, the displacement is zero Point N, which does not move at all, is called a node The pulses continue to move and eventually resume their original form Constructive interference occurs when wave displacements are in the same direction The result is a wave that has an amplitude greater than those of any of the individual waves Figure 14-13b shows the constructive interference of two equal pulses A larger pulse appears at point A when the two waves meet Point A has the largest displacement and is called the antinode The two pulses pass through each other without changing their shapes or sizes If the pulses have unequal amplitudes, the resultant pulse at the overlap is the algebraic sum of the two pulses, as shown in Figure 14-13c Standing waves You can apply the concept of superimposed waves to the control of the formation of large amplitude waves If you attach one end of a rope or coiled spring to a fixed point, such as a doorknob, and then start to vibrate the other end, the wave leaves your hand, is reflected at the fixed end, is inverted, and returns to your hand When it reaches your hand, the reflected wave is inverted and travels back down the rope Thus, when the wave leaves your hand the second time, its displacement is in the same direction as it was when it left your hand the first time What if you want to increase the amplitude of the wave that you create Suppose you adjust the motion of your hand so that the period of vibration equals the time needed for the wave to make one round-trip from your hand to the door and back Then, the displacement given by your hand to the rope each time will add to the displacement of the reflected wave As a result, the oscillation of the rope in one segment will be much greater than the motion of your hand You would expect this based on your knowledge a of constructive interference This large-amplitude oscillation is an example of mechanical resonance The nodes are at the ends of the rope and an antinode is in the middle, as shown in Figure 14-14a Thus, the wave b appears to be standing still and is called a standing wave You should note, however, that the standing wave is the interference of the two traveling waves moving in opposite directions If you double the frequency of vibration, you can produce one more node and one more antinode in the rope c Then it appears to vibrate in two segments Further increases in frequency produce even more nodes and antinodes, as shown in Figures 14-14b and c.

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The answer to the puzzle arose from a study of magnetism In the 19th century, Michael Faraday developed the concept of a field to explain how a magnet attracts objects Later, the field concept was applied to gravity Any object with mass is surrounded by a gravitational field in which another object experiences a force due to the interaction between its mass and the gravitational field, g, at its location This is expressed by the following equation

GM r2 The gravitational field is equal to the universal gravitational constant times the object s mass, divided by the square of the distance from the object s center The direction is toward the mass s center

To program in C#, you re going to need a way to build C# programs. You can do this with a command-line compiler, VS .NET, or a C# package for a programming editor.

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