I just need the practice problem solved with work shown. The rest of the images provides the information needed to solve the problem. The correct answer is also provided to check work

College Physics
1st Edition
ISBN:9781938168000
Author:Paul Peter Urone, Roger Hinrichs
Publisher:Paul Peter Urone, Roger Hinrichs
Chapter2: Kinematics
Section: Chapter Questions
Problem 33PE: An unwary football player collides with a padded goalpost while running at a velocity of 7.50 m/s...
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I just need the practice problem solved with work shown. The rest of the images provides the information needed to solve the problem. The correct answer is also provided to check work. 

EXAMPLE 2.10 Falling euro in Pisa
Our first example of free-fall motion is very simple. A 2-euro coin is dropped from the Leaning Tower of
Pisa. It starts from rest and falls freely. Ignore the effects of air resistance, and compute its position and
velocity after 1.00 s, 2.00 s, and 3.00 s.
Transcribed Image Text:EXAMPLE 2.10 Falling euro in Pisa Our first example of free-fall motion is very simple. A 2-euro coin is dropped from the Leaning Tower of Pisa. It starts from rest and falls freely. Ignore the effects of air resistance, and compute its position and velocity after 1.00 s, 2.00 s, and 3.00 s.
SOLUTION
SET UP Figure 2.25 shows the diagram we sketch. For a coordinate
system, we choose a vertical axis with the upward direction to be posi-
tive, and we place the origin at the starting point. The position, velocity,
and acceleration have only y components. The initial value yo of the co-
ordinate y and the initial y component of velocity voy are both zero. The
acceleration is downward (in the negative y direction), so the constant
y component of acceleration is ay = -g = -9.80 m/s². (Remember
that, by definition, g itself is always positive.)
SOLVE From Equations 2.13 and 2.12 we have
y = vot + a₂t² = 0 + (−8)t² = (-4.90 m/s²)t²,
SW BOULU05 DIN 100 mort,
+ ayt = 0 + (−g)t = (-9.80 m/s²)t.
Vy
= Voy
og
Amoer - Yel
(alm
2
s, y₁
Using subscript 1 for the first time, we find that when
t = t₁ = 1.00
1.00 s, y₁ = (-4.90 m/s²) (1.00 s)² = -4.90 m and v₁y =
Uly
(-9.80 m/s2)(1.00 s) = -9.80 m/s. The coin is therefore 4.90 m be-
low the origin (because y is negative) and has a downward velocity (uy
is negative) with magnitude 9.80 m/s.
ob
The positions and velocities at 2.00 s and 3.00 s are found in the
same way. The results are -19.6 m and -19.6 m/s at t = 2.00 s and
-44.1 m and -29.4 m/s at t = 3.00 s.
REFLECT All our values of y and v, are negative because we have cho-
sen the positive y axis to be upward. We could just as well have chosen
the downward direction to be positive. In that case, the y component of
acceleration would have been a, = g = +9.80 m/s². The crucial point
+9.80 m/s². The crucial
that you must decide at the start which direction is positive, and then
stick with your decision.
mioq
dgu
point
vizu
odit soulsy ovings
zli tud Jmclzni as ch
at 0195 gr
play
The Leaning Tower
***
sty
din 2.6 Freely Falling Objects 49
CHON
ill
LATION
B
1435
al
FIGURE 2.25
Our sketch for the problem
eft im
Y = 0
Y
0
V₁y = ?
Vzy=?
V3Y
=?
to = 0, yo=0
t₁ = 100 s, y₁= ?
ay=-9--980 m/s²
t₂ = 2.00 s₂ Y₂ = ?
-
13=3.00 S, y3 = ?
Practice Problem: The coin is released 47.0 m above the ground.
How much time is required for the coin to fall to the ground? What
is its velocity just before it strikes the ground? Answers: 3.10 s,
-30.4 m/s.
how of snuf ow ob anoires 18// 39303
Transcribed Image Text:SOLUTION SET UP Figure 2.25 shows the diagram we sketch. For a coordinate system, we choose a vertical axis with the upward direction to be posi- tive, and we place the origin at the starting point. The position, velocity, and acceleration have only y components. The initial value yo of the co- ordinate y and the initial y component of velocity voy are both zero. The acceleration is downward (in the negative y direction), so the constant y component of acceleration is ay = -g = -9.80 m/s². (Remember that, by definition, g itself is always positive.) SOLVE From Equations 2.13 and 2.12 we have y = vot + a₂t² = 0 + (−8)t² = (-4.90 m/s²)t², SW BOULU05 DIN 100 mort, + ayt = 0 + (−g)t = (-9.80 m/s²)t. Vy = Voy og Amoer - Yel (alm 2 s, y₁ Using subscript 1 for the first time, we find that when t = t₁ = 1.00 1.00 s, y₁ = (-4.90 m/s²) (1.00 s)² = -4.90 m and v₁y = Uly (-9.80 m/s2)(1.00 s) = -9.80 m/s. The coin is therefore 4.90 m be- low the origin (because y is negative) and has a downward velocity (uy is negative) with magnitude 9.80 m/s. ob The positions and velocities at 2.00 s and 3.00 s are found in the same way. The results are -19.6 m and -19.6 m/s at t = 2.00 s and -44.1 m and -29.4 m/s at t = 3.00 s. REFLECT All our values of y and v, are negative because we have cho- sen the positive y axis to be upward. We could just as well have chosen the downward direction to be positive. In that case, the y component of acceleration would have been a, = g = +9.80 m/s². The crucial point +9.80 m/s². The crucial that you must decide at the start which direction is positive, and then stick with your decision. mioq dgu point vizu odit soulsy ovings zli tud Jmclzni as ch at 0195 gr play The Leaning Tower *** sty din 2.6 Freely Falling Objects 49 CHON ill LATION B 1435 al FIGURE 2.25 Our sketch for the problem eft im Y = 0 Y 0 V₁y = ? Vzy=? V3Y =? to = 0, yo=0 t₁ = 100 s, y₁= ? ay=-9--980 m/s² t₂ = 2.00 s₂ Y₂ = ? - 13=3.00 S, y3 = ? Practice Problem: The coin is released 47.0 m above the ground. How much time is required for the coin to fall to the ground? What is its velocity just before it strikes the ground? Answers: 3.10 s, -30.4 m/s. how of snuf ow ob anoires 18// 39303
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