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Figure 9-2 An air bag is inflated during a collision when the force due to the impact triggers the sensor The chemicals in the air bag s inflation system react and produce a gas that rapidly inflates the air bag



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A large change in momentum occurs only when there is a large impulse A large impulse can result either from a large force acting over a short period of time or from a smaller force acting over a long period of time What happens to the driver when a crash suddenly stops a car An impulse is needed to bring the driver s momentum to zero According to the impulse-momentum equation, F t pf pi The final momentum, pf , is zero The initial momentum, pi, is the same with or without an air bag Thus, the impulse, F t, also is the same An air bag, such as the one shown in Figure 9-2, reduces the force by increasing the time interval during which it acts It also exerts the force over a larger area of the person s body, thereby reducing the likelihood of injuries





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Average Force A 2200-kg vehicle traveling at 94 km/h (26 m/s) can be stopped in 21s by gently applying the brakes It can be stopped in 38 s if the driver slams on the brakes, or in 022 s if it hits a concrete wall What average force is exerted on the vehicle in each of these stops

creating Errors As you iterate through your prototypes, one of your sub-goals should be to break stuff You want to understand what causes compiler errors, what throws exceptions, and so on Keeping Errors When you do break something, keep track of it! Instead of deleting the code that breaks, keep it inline and comment it out For example, you ll see examples of questions in this book in which you re meant to determine which of several code fragments compile, or work a certain way It s a good bet that those fragments exist in comments, somewhere in our prototype code And, of course, erroneous code can be a great topic for a flashcard

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Sketch the system Include a coordinate axis and select the positive direction to be the direction of the velocity of the car Draw a vector diagram for momentum and impulse Known:

B, while RF sampling elements are formed by segments A and C Although the original designs were based on a coaxial-cable sensor, later versions used either printed circuit foil transmission line segments or parallel brass rods for A, B, and C The sensor unit is basically a directional coupler with a detector element for both forward and reverse directions For best accuracy, diodes CR1 and CR2 should be matched, as should R1 and R2 The resistance of R1 and R2 should match the transmission line surge impedance, although in many instruments a 68- compromise resistance is used The particular circuit shown in Fig 27-15 uses a single dc meter movement to monitor the output power Many modern designs use two meters (one each for forward and reverse power) One of the latest designs in VSWR meter sensors is the current transformer assembly shown in Fig 27-16 In this instrument, a single-turn ferrite toroid transformer is used as the directional sensor The transmission line passing through the hole in the toroid doughnut forms the primary winding of a broadband RF transformer The secondary, which consists of 10 to 40 turns of small enamel wire, is connected to a measurement bridge circuit (C1 + C2 + load) with a rectified dc output Figures 27-17 and 27-18 show instruments based on the current transformer technique Shown in Fig 27-17 is the Heath model HM-102 high-frequency VSWR/power meter The sensor is a variant on the current transformer method This

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Determine the initial momentum, pi pi mvi (2200 kg)( 26 m/s) Substitute m 57 104 kg m/s Determine the final momentum, pf pf mvf (2200 kg)( 00 m/s) Substitute m 00 kg m/s

Apply the impulse-momentum theorem to obtain the force needed to stop the vehicle F t pf pi F t ( 00 kg m/s) (57 104 kg m/s) Substitute pf 00 kg m/s, pi 57 104 kg m/s 57 104 kg m/s F

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