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Any of the methods above can be used to provide a good to optimal solution to most cam design problems Each method has its advantages and disadvantages The method in Sec 134 can provide a near-optimal design over any given range of operating speeds The method described in Sec 135 only optimizes at one speed at a time and is the most complex to use, but it provides a true optimum, not limited to a linear combination of given trigonometric terms, as in Sec 134 The method in Sec 135 is also the only one that can optimize for nonlinear effects, although the accuracy of nonlinear design is greatly limited by the inability to include preload The method in Sec 136 does not provide a true optimum, but can usually nd a good solution The method in Sec 13.

Router# show ip route Codes: C - connected, S - static, I - IGRP, R - RIP, M - mobile, B - BGP, D - EIGRP, EX - EIGRP external, O - OSPF, IA - OSPF inter area, N1 - OSPF NSSA external type 1, N2 - OSPF NSSA external type 2, E1 - OSPF external type 1, E2 - OSPF external type 2, E - EGP, i - IS-IS, L1 - IS-IS level-1, L2 - IS-IS level-2, * - candidate default, U - per-user static route, o - ODR, T - traffic engineered route Gateway of last resort is not set 10.0.0.0/24 is subnetted, 1 subnets O 10.0.1.0 [110/65] via 192.168.1.100, 00:04:18, Serial0 C 192.168.1.0/24 is directly connected, Serial0 C 192.168.100.0/24 is directly connected, Ethernet0

Comma-Separated Values (CSV)

FIGURE 14-3

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BRI-STARS is a pseudo two-dimensional hydraulic program that (through the use of stream tubes) provides a time and ow dependent two-dimensional sediment routing (aggradation and degradation) in a bridge cross section. UNET: Unlike the riverine ow, this program deals with tidal ow. DYNET: Two-dimensional hydraulic program for tidal ow.

7 can provide a good, but not really optimal solution for any case, and it has the advantage over the other methods of providing good control over the shape of the follower lift curve From the preceding paragraph and the more detailed information presented previously, the designer should be able to nd the best of these methods to use for any particular design problem..

the wire so that it is easy to handle. Temperature causes the resistance to change, so use the wire at room temperature and don t use it so long that it heats up. 1. Place the resistor in series with your robot s battery. 2. Measure the voltage across the resistor (a 6.2-foot-long coil of #12 wire, or the high-wattage resistor) with the robot running in normal battle-like conditions. When measuring this voltage, the value will likely be variable and may appear unstable. Take the maximum reading, and then take a reading that appears to be the nominal or average value. The robot s motors must be loaded to simulate those of a real battle, or else you will measure a value that is much too low up to five to ten times too low than battle-use values. 3. When you have gathered these voltage values, calculate the current by placing the voltage readings into the formula current = voltage / 0.01 ohms. The 0.01 ohms is the resistance of the 6.2-foot-long wire. If you are using a high-wattage resistor, then substitute the 0.01 ohms for the resistance of your resistor. For example, suppose that when running the experiment, you noted a maximum voltage of 1.2 volts and an average of 0.5 volts. Plugging these values into the formula yields a maximum current value of 120 amps (120 amps = 1.2 volts / 0.01 ohms) and a typical current of 50 amps (50 amps = 0.5 volts / 0.01 ohms). After you have found the maximum current value and the typical current value, you have the information that you need to choose the correct battery for your robot.

L 30-6

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