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ONCE A SIGNAL HAS LEFT A TRANSMITTER, THE IMPULSES TRAVEL, OR propagate, in a cable, optical fiber, or space In cables, the signals are ac (usually) or dc (sometimes) In fiberoptic systems, the signals are infrared or visible light The signals are confined in cables and fibers; the only important variable is the attenuation per kilometer This depends on the ac frequency, the thickness of wire, or the clarity of optical fiber material In communication via electromagnetic waves, the propagation is affected by several factors

4 3 1 6 x 1 x 1 2x x2 1 4 3 1 6 Denominator factored: x 1 x 1 2x x 1 x 1 LCD 2x x 1 x 1 2x x 1 x 1 4 3 2x x 1 x 1 x 1 x 1 1 6 2x x 1 x 1 2x x 1 x 1 2x x 1 x 1

While I have discussed the existence of this TextView in the xml, I have not yet discussed why it works without any corresponding code I mentioned earlier in this book that there are two ways to design a UI for Android: through the code, and through the mainxml file The preceding code sample creates a TextView in xml and sets the text to Hello World, HelloWorldText Edit this line of the mainxml file to read as follows:

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The orientation of the E flux is the polarization of an EM wave If the E flux lines are parallel to the earth s surface, you have horizontal polarization If the E flux lines are perpendicular to the surface, you have vertical polarization Polarization can be slanted at any angle between horizontal and vertical The orientation of the E flux lines sometimes rotates as the wave travels through space This is circular polarization if the E-field intensity remains constant If the E-field intensity is more intense in some planes than in others, the polarization is said to be elliptical Rotating polarization can be either clockwise or counterclockwise, viewed as the wavefronts approach you This is the sense of polarization

android:text="This is the text of an Android TextView!"

2x x 1 4 2x x 1 3 x 1 x 1 2x 6 8x x 1 6x x 1 x2 1 12x 8x2 8x 6x2 6x x2 12x 1 14x2 2x x2 12x 1 x2 12x 1 x2 12x 1 13x2 14x 1 0 13x 1 x 1 0 13x 1 0 1 1 13x 1 x 1 13 x 1 0 1 1 x 1 But x 1 leads to a zero in a denominator, so x 1 is not a solution

Electromagnetic waves follow straight lines unless something makes them bend Line-of-sight propagation can take place even when the receiving antenna can t be seen 499

Rerun the project, and your results should appear as they do in this illustration Take some time and experiment with the xml TextView Then you can move on to another way of creating a Hello World! application

500 Data reception from the transmitting antenna To some extent, radio waves penetrate nonconducting objects such as trees and frame houses The line-of-sight wave consists of two components: the direct wave and the reflected wave The direct wave The longest wavelengths are least affected by obstructions At very low, low and medium frequencies, direct waves can diffract around things As the frequency rises, especially above about 3 MHz, obstructions have a greater and greater blocking effect The reflected wave Electromagnetic waves reflect from the earth s surface and from conducting objects like wires and steel beams The reflected wave always travels farther than the direct wave (Fig 27-1) The two waves are usually not in phase at the receiving antenna If they re equally strong but 180 degrees out of phase, a dead spot occurs This is most common at the highest frequencies

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1 If x 1 x 5 0, then the solutions are a x 1; 5 d x 1; 5 2 If x2 x 1 0, then x p p p 5 1 5 1 5 c b 1 a 2 2 2 p 2 24 in simpli ed form is 3 2 p p p a 1 24 b 1 6 c 2 6 d cannot be simplified 4 To apply the quadratic formula to 2x2 x 3, a a 2; b 1; c 3 c a 2; b 1; c 3 b a 2; b 1; c 3 d a 2; b 1; c 0 p 5 d 1 2 b x 1; 5 c x 1; 5

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