A
non-horizontally launched projectile with an initial vertical velocity of 39.2
m/s will reach its peak in 4 seconds. The process of rising to the peak is a
vertical motion and is again dependent upon vertical motion parameters (the
initial vertical velocity and the vertical acceleration). The height of the
projectile at this peak position can be determined using the equation
y = viy • t + 0.5 • g • t2
where viy is the
initial vertical velocity in m/s, g is the acceleration of gravity (-9.8 m/s/s)
and t is the time in seconds it takes to reach the
peak. This equation can be successfully used to determine the vertical
displacement of the projectile through the first half of its trajectory (i.e.,
peak height) provided that the algebra is properly performed and the proper
values are substituted for the given variables. Special attention should be
given to the facts that the t in the equation is the time up to the peak and
the g has a negative value of -9.8 m/s/s.
Answer
the following questions and click the button to see the answers.
1.
Aaron Agin is resolving velocity
vectors into horizontal and vertical components. For each case, evaluate
whether Aaron's diagrams are correct or incorrect. If incorrect, explain the
problem or make the correction.
A: Aaron is wrong. If v is upwards and rightwards then vy should
be directed upwards. Aaron's is downwards.
B: Aaron is wrong. If v is downwards and leftwards then vx should
be directed leftwards and vy should
be directed downwards. Aaron's components are in the wrong direction.
C: Aaron is wrong. This is a labeling problem. Aaron has labeled the
horizontal component as vy and
the vertical component as vx.
close
2.
Use trigonometric functions to resolve the following velocity vectors into
horizontal and vertical components. Then utilize kinematic equations to
calculate the other motion parameters. Be careful with the equations; be guided
by the principle that "perpendicular components of motion are independent
of each other."
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A: vix = 9.5 m/s
• cos(40 degrees) = 7.28 m/s
B : viy =
9.5 m/s • sin(40 degrees) = 6.11 m/s
C: tup = (6.11
m/s) / (9.8 m/s/s) = 0.623 s
D: ttotal = 2 •
(0.623 s) = 1.25 s
E: x = 7.28 m/s • 1.25 s = 9.07 m
F: y = (6.11
m/s) • (0.623 s) + 0.5*(-9.8 m/s/s) • (0.623 s )2 = 1.90 m
G: vix = 25 m/s •
cos (60 degrees) = 12.5 m/s
H: viy = 25 m/s •
sin (60 degrees) = 21.7 m/s
I: tup = (21.7
m/s) / (9.8 m/s/s) = 2.21 s
J: ttotal = 2 •
2.21 s = 4.42
s
K: x = 12.5 m/s • 4.42 s = 55.2 m
L: y = 21.7 m/s
• 2.21 s + 0.5 • (-9.8 m/s/s) • (2.21 s )2 = 23.9 m
M: vix = 30 m/s •
cos (30 degrees) = 26.0 m/s
N: viy = 30 m/s •
sin (30 degrees) = 15.0 m/s
O: tup = (15.0
m/s) / (9.8 m/s/s) = 1.53 s
P: ttotal = 2 •
1.53 s = 3.06
s
Q: x = 26.0 m/s • 3.06 s = 79.5 m
R: y = 15.0 m/s
• 1.53 s + 0.5 • (-9.8 m/s/s) • (1.53 s )2 = 11.5 m
3.
Utilize kinematic equations and projectile motion concepts to fill in the
blanks in the following tables.
A: 14.9 m
B: 164 m
C: 2.93 s
D: 5.85 s
E: 42.0 m
F: 240 m
G: 19.2 m/s
H: 16.1 m/s
I: 1.64 s
J: 3.28 s
K: 79.9 deg
L: 19.7 m/s
M: 2.01 s
N: 4.02 s
O: 19.7 m/s
P: 3.47 m/s
Q: 0.354 s
R: 0.709 s