A shot putter releases the shot some distance above the level ground with a velocity of 12.0 m/s, 51.0° above the horizontal. The shot hits the ground 2.08 s later. Ignore air resistance. [(c) How far did she throw the shot horizontally?] (d) Why does the expression for R in Example 3.8 not give the correct answer for part (c)? (e) How high was the shot above the ground when she released it? (f) Draw x-t, y-t, vx-t, and vy-t graphs for the motion

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Chapter1: Units, Trigonometry. And Vectors
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A shot putter releases the shot some distance above the level ground with a velocity of 12.0 m/s, 51.0° above the horizontal. The shot hits the ground 2.08 s later. Ignore air resistance. [(c) How far did she throw the shot horizontally?] (d) Why does the expression for R in Example 3.8 not give the correct answer for part (c)? (e) How high was the shot above the ground when she released it? (f) Draw x-t, y-t, vx-t, and vy-t graphs for the motion
EXAMPLE 3.8 Height and range of a projectile II: Maximum height, maximum range
Figure 3.24 A launc"
range. The range is sh
Find the maximum height h and horizontal range R (see Fig. 3.23) of a
projectile launched with speed u, at an initial angle ao between 0 and
90°. For a given vo, what value of ao gives maximum height? What
value gives maximum horizontal range?
A4
othe
IDENTIFY and SET UP This is almost the same as parts (b) and (c) of
Example 3.7, except that now we want general expressions for h and R. We
also want the values of ao that give the maximum values of h and R. In part
(b) of Example 3.7 we found that the projectile reaches the high point of
its trajectory (so that v, = 0) at time t¡ = vo/g, and in part (c) we found
that the projectile returns to its starting height (so that y = yo) at time
2 = 20y/8 = 2t1. We'll use Eq. (3.20) to find the y-coordinate h at fị and
Eq. (3.19) to find the x-coordinate R at time 12. We'll express our answers in
terms of the launch speed vo and launch angle ao by using Eqs. (3.18).
Launch
angle:
do = 30
45°
do = 60
EXECUTE From Eqs. (3.18), vor = vocos ao and voy = vosinao. Hence
we can write the time 1 when v,
2a0 = 90°, or ao
given initial speed if
O as
%3D
Uby
Uo sin ao
EVALUATE Figure 3.
trajectories of a ball p
45°, and 60°. The init
cases. The horizontal
Equation (3.20) gives the height y = h at this time:
%3D
sinao
Uosinao
vf sin² ao
nearly the same for u
given value of the
an initial angle 90°
resistance.)
h = (tosinao)(indo) - ¿|(*
28
For a given launch speed u, the maximum value of h occurs for
sina, = 1 and ao = 90°–that is, when the projectile is launched
straight up. (If it is launched horizontally, as in Example 3.6, ao = 0
and the maximum height is zero!)
The time t2 when the projectile hits the ground is
CAUTION Height
memorizing the abo»
only in the special c
can use the expressic
heights are equal. TE
these equations do na
20oy _ 200sinao
The horizontal range R is the value of x at this time. From Eq. (3.19), this is
20o sin ao
vổ sin 2ao
R = (vocos ao)½ = (vo cos ao)
KEYCONCEPT W
projectile problems i
numbers as far into t
(We used the trigonometric identity 2 sin ao cos ao = sin 2ao, found in
Appendix B.) The maximum value
sin 2a, is 1; this occurs when
explore and understar
Transcribed Image Text:EXAMPLE 3.8 Height and range of a projectile II: Maximum height, maximum range Figure 3.24 A launc" range. The range is sh Find the maximum height h and horizontal range R (see Fig. 3.23) of a projectile launched with speed u, at an initial angle ao between 0 and 90°. For a given vo, what value of ao gives maximum height? What value gives maximum horizontal range? A4 othe IDENTIFY and SET UP This is almost the same as parts (b) and (c) of Example 3.7, except that now we want general expressions for h and R. We also want the values of ao that give the maximum values of h and R. In part (b) of Example 3.7 we found that the projectile reaches the high point of its trajectory (so that v, = 0) at time t¡ = vo/g, and in part (c) we found that the projectile returns to its starting height (so that y = yo) at time 2 = 20y/8 = 2t1. We'll use Eq. (3.20) to find the y-coordinate h at fị and Eq. (3.19) to find the x-coordinate R at time 12. We'll express our answers in terms of the launch speed vo and launch angle ao by using Eqs. (3.18). Launch angle: do = 30 45° do = 60 EXECUTE From Eqs. (3.18), vor = vocos ao and voy = vosinao. Hence we can write the time 1 when v, 2a0 = 90°, or ao given initial speed if O as %3D Uby Uo sin ao EVALUATE Figure 3. trajectories of a ball p 45°, and 60°. The init cases. The horizontal Equation (3.20) gives the height y = h at this time: %3D sinao Uosinao vf sin² ao nearly the same for u given value of the an initial angle 90° resistance.) h = (tosinao)(indo) - ¿|(* 28 For a given launch speed u, the maximum value of h occurs for sina, = 1 and ao = 90°–that is, when the projectile is launched straight up. (If it is launched horizontally, as in Example 3.6, ao = 0 and the maximum height is zero!) The time t2 when the projectile hits the ground is CAUTION Height memorizing the abo» only in the special c can use the expressic heights are equal. TE these equations do na 20oy _ 200sinao The horizontal range R is the value of x at this time. From Eq. (3.19), this is 20o sin ao vổ sin 2ao R = (vocos ao)½ = (vo cos ao) KEYCONCEPT W projectile problems i numbers as far into t (We used the trigonometric identity 2 sin ao cos ao = sin 2ao, found in Appendix B.) The maximum value sin 2a, is 1; this occurs when explore and understar
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