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nfrared communication via Infrared Data Association (IrDA) is built into many portable computers and PDAs, such as the Palm, Windows CE machines, the old HP200LX, and many laptops. Infrared communication provides a convenient way to download data loggers and to communicate with other mobile platforms as well as for remote control without wires over short distances.

(31.29)

and the phase between the response and the force is = tan 1 2 / n 1 2/ 2 n (31.30)

Now your newly minted particles will all have the right initial conditions. Moving to the next stage of the particle life: the update. This is the update method in the particle emitter. You don t actually need to change the individual particle update method.

When the forcing frequency coincides with the damped natural frequency d, the response amplitude is given by 1 Xmax = F0 /k (4 3 2)1/2 The maximum response or resonance occurs when = n(1 2 2)1/2 and is 1 Xmax = F0 /k 2 (1 2)1/2 (31.32) (31.31)

For structures with low damping, d approximately equals n, and the maximum response is 1 Xmax = F0 /k 2 (31.33)

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The IrDA protocol is very similar to standard RS-232, as illustrated by the diagram in Fig. 5-1. The standard RS-232 protocol uses voltage levels to transmit the data. From left to right on the time-line, the voltage is in a resting low state when a high start bit comes along, followed by 8 data bits, and last at least 1 low stop bit. A new character can start at any time after the conclusion of the previous stop bit(s). There are several conventions. RS232 is an inverted logic, so that a logical 1, or mark, is represented by a low level. This comes from old teletypewriter days when a pen was down to make a mark and lifted up by an electrical current in a magnet to make a space, or zero. Also, by convention, the data is transmitted least significant bit first, and a logical 1 is transmitted as a low level and a logical zero is transmitted as a high level. At 2400 baud, the length of each bit period is 1/2400 417 s.

The response amplitude in Eq. (31.29) is plotted against the forcing frequency in Fig. 31.8. The curves start at unity, reach a maximum in the neighborhood of the system natural frequency, and decay to zero at large values of the forcing frequency. The response is larger for a system with low damping, and vice versa, at any given frequency. The phase difference between the response and the excitation as given in Eq. (31.30) is plotted in Fig. 31.9. For smaller forcing frequencies, the response is nearly in phase with the force; and in the neighborhood of the system natural frequency, the response lags behind the force by approximately 90 . At large values of forcing frequencies, the phase is around 180 .

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

-(void)update:(NSTimeInterval)deltaTime { // update active particles -> move them [super update:deltaTime]; for (BBParticle * kid in childrenParticles) { [kid update:deltaTime]; if (animateColor) { kid.r = BBLerp(startR, endR, (kid.startingLife kid.life)/kid.startingLife); kid.g = BBLerp(startG, endG, (kid.startingLife kid.life)/kid.startingLife); kid.b = BBLerp(startB, endB, (kid.startingLife kid.life)/kid.startingLife); kid.a = BBLerp(startA, endA, (kid.startingLife kid.life)/kid.startingLife);

Steady-State Velocity and Acceleration Response. The steady-state velocity response is obtained by differentiating the displacement response, given by Eq. (31.27), with respect to time: / n xs = F0 n /k [(1 2 / 2 )2 + (2 / n)2]1/2 n (31.34)

And the steady-state acceleration response is obtained by further differentiation and is ( / n)2 s x = 2 2 F0 n /k [(1 / 2 )2 + (2 / n)2]1/2 n (31.35)

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