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University Physics I - Classical Mechanics, 2019

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2.5. EXAMPLES 47<br />

which the rocket reaches the top of its trajectory, and then starts coming down. The corresponding<br />

displacement is, by Eq. (2.16),<br />

so the maximum height it reaches is 30.4 m.<br />

Δy top = v i2 (t top − t i2 ) − 1 2 g(t top − t i2 ) 2 =20.4m<br />

At the end of the full 3-second interval, the rocket’s displacement is<br />

Δy 2 = v i2 Δt 2 − 1 2 g(Δt 2) 2 =15.9m<br />

(so its height is 25.9 m above the ground), and the final velocity is<br />

v f2 = v i2 − gΔt 2 = −9.43 m s .<br />

(c) The acceleration for this part is (v f3 − v i3 )/Δt 3 =(−5+9.43)/1 =4.43 m/s 2 .Notethepositive<br />

sign. The displacement is<br />

so the final height is 25.9 − 7.21 = 18.7 m.<br />

Δy 3 = −9.43 × 1+ 1 2 × 4.43 × 12 = −7.22 m<br />

(d) This is just motion with constant speed to cover 18.7 m at 5 m/s. The time it takes is 3.74 s.<br />

The graphs for this motion are shown earlier in the chapter, in Figure 2.3.

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