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8.6.1 Band Brakes A typical design for a band brake is shown in Fig. 8.19. A flexible metal band lined with a friction material contacts the drum over an angle of wrap and exerts a braking torque T on the drum. This particular design is self-energizing, since the moment exerted on the lever by force P1 assists in actuating the brake.

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The radio mailbox centers around three major components: the touch-tone decoder chip, the ISD2590 voice message chip, and of course the BASIC STAMP 2 microprocessor (see Fig. 14-2). We use the original STAMP 2, but you can easily substitute the alternative STAMP 2. The first component we see in the project is the touch-tone decoder. The decoder chip is connected to your amateur radio transceiver s speaker or headphone jack, via capacitor C1 and resistors R1 and R2. The CM8880 touch-tone encoder/decoder is shown in the block diagram in Fig. 14-3. The CM8880 touch-tone decoder looks for a combination of tones for each numerical digit, as seen in Table 14-1. The touch-tone decoder receives and decodes the tone pairs and produces a binary value based on the valid digit received; the binary value is then fed to the STAMP 2. The CM8880 touch-tone IC decodes the incoming touch tones and produces a binary code, as shown in Table 14-2. If the number 4 is pressed on a remote touch-tone keypad, a binary value of 0100 will show up at the outputs D0 through D3 on pins 14, 15, 16, and 17 on the CM8880. This binary value is next sent to the BASIC STAMP 2 at U2. The touch-tone decoder IC is clocked by a 3.579-MHz color burst crystal at pins 6 and 7. The resistor and capacitor at C2 and R3 form a guard/time network that controls the incoming tone duration time limits. The CM8880 must be powered from a 5-Vdc power

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Four basic relationships are needed for analysis or design. For a band wrapped around a drum, the ratio of tensions is P1 = e f P2 (8.42)

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where the notation is indicated in Fig. 8.19. The net torque exerted on the drum by the band is T = (P1 P2 D 2 (8.43)

The maximum contact pressure between the band and the drum occurs at the more taut P1 end of the band: pmax = 2 P1 bD (8.44)

Finally, it is necessary to sum moments on the lever about pivot A to get the relationship involving the actuating force Q:

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(8.45)

After substituting for P1 and P2 in terms of pmax, f, and , we get the following equation for actuating force: Q= bDpmax c a ef 2 (8.46)

For pmax you should use the value suggested by the lining manufacturer. This brake could be self-locking if the designer were to get careless. The actuating force Q should always be positive. If it were zero or negative, the slightest touch on the lever would cause the brake to lock abruptly. The expression in the parentheses in Eq. (8.46) must always be positive. Thus, as a rule, design the brake so that a< c e f (8.47)

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