Physics 1 Test 1 Solutions
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Physics
Date
Apr 3, 2024
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PHYS 1441 (Fall 2023 White) Test-1 View Basic/Answers
Note: The variables used in the below solutions are not the same as those used in your assignment.
Begin Date:
9/14/2023 5:30:00 PM -- Due Date:
9/14/2023 6:50:00 PM End Date:
9/14/2023 6:50:00 PM
Problem 1 - 1.2.9 :
Suppose you take a deep breath, and your lungs fill with a volume of air equal to 1.75
L.
Part (a)
What is the mass of the breath, in grams, if the density of air is 1.29 × 10
-3
g/cm
3
?
The volume of an object of uniform density is
where m is the mass in kg and is the density in kg/m
. Therefore,
where V is the volume in m
. Plugging in numbers and converting units as needed,
Problem 1 - 1.2.10 :
A straightforward method of finding the density of an object is to measure its mass and then measure its volume by
submerging it in a graduated cylinder filled with water.
Part (a)
What is the density, in grams per cubic centimeter, of a rock that displaces of water?
The volume of an object of uniform density is
where is the mass in kilograms and is the density in kilograms per cubic meter. Therefore,
where is the volume in cubic meters. Plugging in numbers and converting units as needed,
Problem 1 - 1.2.11 :
Suppose you have a coffee mug with a cylindrical shape (the radius is uniform, in other words).
Part (a)
What is its inside radius, in centimeters, if it holds 350
g of coffee when filled to a depth of 5.5
cm? Assume coffee has the same
density as water, 1.00 g/cm
3
.
V =
m
ρ
m
3
ρ
3
m = Vρ
3
m = 1.75
⋅
⋅
1.29
⋅
10
3
cm
3
10
−3
g/cm
3
m = 2.258 g
225
g
87.5
cm
3
V =
m
ρ
m
3
m
ρ
ρ =
m
V
V
ρ =
225 g
87.5 cm
3
ρ = 2.571 g/cm
3
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The volume of an object of uniform density is
where m is the mass in kg and is the density in kg/m
. The volume of a cylinder is
where r is the radius of the cylinder in m
and h is the height of the cylinder in m. Setting the volumes equal,
Plugging in numbers and converting units as needed,
Problem 2 - c3.1.1 :
A particle moves from point A to point B. Let L
be the straight-line distance between A and B, let R
be the magnitude
of the particle's displacement, and let S
be the distance the particle traveled.
Part (a)
Which is always true?
We learn from our textbook that the magnitude of the displacement from A to B equals the straight-line distance between A and B, no matter
what the actual traveled distance is. Thus, by definition.
The correct choice is, therefore, ...
Part (b)
Which is only sometimes true?
The magnitude of the displacement from A to B, , equals the travel distance from A to B, , when and only when the particle's path is
straight. Since the path can be curvy, the equality is not always true.
The correct choice is, therefore, ...
Part (c)
Which can never be true?
The magnitude of the displacement from A to B, , equals the travel distance from A to B, , when and only when the particle's path is
straight. Since the path can be curvy, the equality is not always true. can be smaller than , but it can never be larger, since a
straight path is the shortest path between two points.
The correct choice is, therefore, ...
Problem 3 - 3.1.34 :
The position of a particle moving along the x
axis is given by = (
4.01
m) - (
2.01
m/s) .
Part (a)
At what time (in seconds) does the particle cross the origin?
The origin is where , so we need to solve for time in
V =
m
ρ
m
3
ρ
3
V = π
h
r
2
m
3
2
= π
h
m
ρ
r
2
r =
m
(ρπh)
0.5
r = R =
350 g
1
⋅
5.5 cm
⋅
π
g/cm
3
0.5
R = 4.501 cm
L = R
L = R
R
S
R = S
R = S
R
S
R = S
R
S
R > S
x(t)
t
x = 0
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Solving,
Calculating,
Part (b)
What is the magnitude of the displacement (in meters) of the particle between = 3.00 s and = 6.00 s?
Displacement is a vector whose magnitude is the straight-line distance between the initial and final positions and whose direction is from
the initial toward the final position. The magnitude can be calculated by subtracting the initial position from the final position:
Calculating,
Problem 3 - 3.1.35 :
A cyclist rides 6.1
km east for 17
minutes, then he turns and heads west for 4.1
km in 5.1
minutes. Finally, he rides
east for 12
km, which takes 33
minutes. Take east to be the positive direction.
Part (a)
What is the displacement of the cyclist in km?
Displacement is a vector whose magnitude is the straight-line distance between the initial and final positions and whose direction is from
the initial toward the final position, so
Calculating,
Part (b)
What is his average velocity in km/h?
Average velocity is displacement divided by time, so
Calculating,
Problem 3 - 3.1.36 :
On February 15, 2013, a superbolide meteor (brighter than the Sun) entered Earth’s atmosphere over Chelyabinsk,
Russia, and exploded at an altitude of 23.5 km. Eyewitnesses could feel the intense heat from the fireball, and the
blast wave from the explosion blew out windows in buildings. Suppose the blast wave took 2 minutes and 15
seconds to reach ground level.
Part (a)
What was the average speed of the blast wave in m/s?
Speed is equal to distance divided by time, so
0 = (4.01 m) − (2.01 m/s) t
t =
4.01 m
2.01 m/s
t = 1.995 s
t
t
d =
x (6.00 s) − x (3.00 s)
= [(4.01 m) − (2.01 m/s) (6.00 s)] − [(4.01 m) − (2.01 m/s) (3.00 s)]
d = −6.030 m
d = (6.1 km) − (4.1 km) + (12 km)
t = 14.00 km
=
v
avg
14.00 km
(17 min + 5.1 min + 33 min)
1 h
60 min
= 15.25 km/h
v
avg
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Calculating,
Part (b)
What is the average speed of the blast wave as a fraction of the speed of sound (343 m/s at sea level)?
Dividing by vields
Problem 3 - 3.1.37 :
A woodchuck runs 15
m to the right in 4.01
s, then turns and runs 8.1
m to the left in 2.01
s.
Part (a)
What is the magnitude of the average velocity of the woodchuck in m/s?
Recall that velocity is equal to displacement divided by time. Since displacement includes direction, we have to take into account that the
woodchuck turns around and runs in the opposite direction by applying a negative sign to the second displacement. Note that whether we
define to the right or to the left as the negative direction actually isn't terribly important in this case, as we are asked for a magnitude. This
means that we will take the absolute value of whatever the displacements sum to anyway. However, as the magnitude is always positive,
taking left as the negative direction is convenient since the displacement to the left is smaller; this gives us a positive result without needing
to think about swapping the signs. The time, meanwhile, is always going to be positive so the two times will be added together. Putting this
all together, the equation we find is:
Part (b)
What is its average speed in m/s?
Here, we are asked for the average speed. Unlike velocity, speed does not care about direction. Therefore, we only need to take the total
distance traveled and divide it by the total time it took to find the average speed.
Problem 3 - 3.1.39 :
A professional baseball pitcher throws a baseball at a speed of towards home plate, which is away.
Part (a)
At that speed, how long does it take, in seconds, for the ball to reach home plate?
Convert the speed to meters per second.
Relating the distance to the velocity and the time,
or
v =
(23.5 km)
1000 m
1 km
[(2) (60 s) + 15 s]
v = 174.1 m/s
= 343 m/s
v
sound
= 0.5075
v
v
sound
=
v
avg
−
d
1
d
2
+
t
1
t
2
=
15 m−8.1 m
4.01 s+2.01 s
= 1.146 m/s
v
avg
=
v
avg
+
d
1
d
2
+
t
1
t
2
=
15 m−8.1 m
4.01 s+2.01 s
= 3.837 m/s
v
avg
130
km/h
18.4 m
v =
=
130
×
×
km
h
1000 m
1 km
1 h
3600 s
36.11 m/s
d = vt
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Problem 3 - 3.1.40 :
An airplane leaves Chicago and makes the 3000-km trip to Los Angeles in 4.5
hours. A second plane leaves Chicago
0.51
hours later and arrives in Los Angeles at the same time. Express your answers in units of km/h.
Part (a)
What is the speed of the first plane?
Speed is equal to distance divided by time, so
Calculating,
Part (b)
What is the speed of the second plane?
The time of travel for the second plane is 0.51 h less than that for the first plane, so
Calculating,
Problem 4 - c3.3.5 :
A rock is thrown straight upward. Neglect air resistance.
Part (a)
What is the direction of its acceleration as it is rising?
The rock's acceleration is due to Earth's gravitational force, which is always pulling the rock downward, causing a constant downward
acceleration. The rock's downward acceleration slows the rock down while it is ascending, reverses the rock's velocity at the trajectory's
highest point, and speeds up the rock during its descent. But the acceleration due to gravity is always downward.
The correct choice is, therefore, ...
Downward
Part (b)
What is the direction of its acceleration at the moment it reaches its highest point?
The rock's acceleration is due to Earth's gravitational force, which is always pulling the rock downward, causing a constant downward
acceleration. The rock's downward acceleration slows the rock down while it is ascending, reverses the rock's velocity at the trajectory's
highest point, and speeds up the rock during its descent. But the acceleration due to gravity is always downward.
The correct choice is, therefore, ...
Downward
Part (c)
What is the direction of its acceleration as it is falling?
The rock's acceleration is due to Earth's gravitational force, which is always pulling the rock downward, causing a constant downward
acceleration. The rock's downward acceleration slows the rock down while it is ascending, reverses the rock's velocity at the trajectory's
highest point, and speeds up the rock during its descent. But the acceleration due to gravity is always downward.
t =
=
d
t
18.4 m
36.11 m/s
t = 0.5095 s
speed =
3000 km
4.5 hr
speed = 666.7 km/h
speed =
3000 km
4.5 hr − 0.51 hr
speed = 751.9 km/h
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The correct choice is, therefore, ...
Downward
Problem 4 - c3.3.6 :
A rock is thrown straight upward, then falls back down. Consider the motion of the rock from the time just after it is
thrown, to the time just before it hits the ground. Neglect air resistance.
Part (a)
Which of the following quantities is zero at least one point in the rock’s flight?
Let's consider whether the acceleration and velocity are ever zero. For the acceleration, the rock is being accelerated downward by gravity.
Gravity isn't ever going to turn off, so the gravitational acceleration will never be zero.
The velocity, meanwhile, starts out going upward and ends going downward. There must be one moment where the velocity "flips" from
pointing upward to downward, and at that exact moment there will be no velocity upward or downward. This means that the velocity is zero
for a moment and the correct answer is:
Velocity
Part (b)
Which of the following quantities changes direction during the rock’s flight?
Let's consider whether the acceleration and velocity ever change direction. The velocity is quite simple; since the rock goes up and then
back down, the direction of the velocity starts out upwards and ends downwards, meaning that it changed direction.
The acceleration, meanwhile, is caused by gravity pulling the rock down. Whether it is slowing down the rock's velocity upward or
speeding up its velocity downward, the gravitational acceleration itself is still pointing down. So the acceleration never changes direction.
This tells us that the correct choice is:
Velocity
Part (c)
Which of the following quantities is constant during the rock’s flight?
Let's begin by considering whether or not the velocity is constant. If the rock moved at a constant velocity the entire time, it would keep
going upwards at the same speed forever and would never hit the ground. Since, however, the rock does reverse direction and hit the
ground, we know that the velocity is not constant.
The acceleration, meanwhile, is caused by the Earth's gravity. The gravitational pull on the rock isn't going to change during its flight with
the rock being pulled downward toward the Earth with the same acceleration the entire motion. Therefore, the acceleration is constant and
the correct answer is:
Acceleration
Problem 5 - c3.4.14 :
A graph of acceleration versus
time is shown.
Part (a)
Which of the following graphs best represents a velocity curve that is consistent with the acceleration curve in the above
problem statement? The horizontal axes are scaled identically.
• Recall that acceleration represents the slope of the velocity curve.
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• Note that the first portion of the acceleration graph is positive indicating that the same portion of the velocity curve should have a positive
slope.
• Note that the second portion of the acceleration graph is negative indicating that the same portion of the velocity curve should have a
negative slope.
• The area between the curve and above the horizontal axis in the first section is equal to the area between the curve and below the
horizontal axis in the second section, so the increase in velocity should be followed by a decrease in velocity of equal magnitude.
The correct choice is
Problem 5 - c3.4.15 :
A graph of acceleration versus
time is shown.
Part (a)
Which of the following graphs best represents a velocity curve that is consistent with the acceleration curve in the above
problem statement? The horizontal axes are scaled identically.
• Recall that acceleration represents the slope of the velocity curve.
• Note that the first portion of the acceleration graph is zero indicating that the slope of the same portion of the velocity curve should have a
zero slope. In other words, that portion of the velocity curve should be a constant value. We don't know what that constant value is unless
we are given the initial velocity.
• Note that the second portion of the acceleration graph is negative indicating that the same portion of the velocity curve should have a
negative slope.
The correct choice is
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Problem 5 - c3.4.16 :
A graph of acceleration versus
time is shown.
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Part (a)
Which of the following graphs best represents a velocity curve that is consistent with the acceleration curve in the above
problem statement? The horizontal axes are scaled identically.
• Recall that acceleration represents the slope of the velocity curve.
• Note that the first portion of the acceleration graph is negative indicating that the same portion of the velocity curve should have a
negative slope.
• Note that the second portion of the acceleration graph is zero indicating that the slope of the same portion of the velocity curve should
have a zero slope. In other words, that portion of the velocity curve should be a constant value.
• We don't know the initial value of the velocity unless it is specified. This graph is drawn with an initially non-zero velocity that has no
impact on the acceleration curve.
The correct choice is
Problem 5 - c3.4.17 :
A graph of velocity versus
time is shown.
Part (a)
Which of the following graphs best represents an acceleration curve that is consistent with the above velocity curve? The
horizontal axes are scaled identically.
• Recall that acceleration represents the slope of the velocity curve.
• Note that the first portion of the velocity graph has a constant positive slope indicating that the same portion of the acceleration curve
should have a constant positive value.
• Note that the second portion of the velocity graph has a constant negative slope indicating that the same portion of the acceleration curve
should have a constant negative value.
• Because the magnitudes of the velocity increase and the velocity decrease are equal, the area between the first portion of the acceleration
curve and the horizontal axis should equal the corresponding area for the second portion of the acceleration curve. The area which is below
the curve indicates a negative velocity change.
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• The velocity curve indicates an initially non-zero velocity which has no impact on the acceleration curve.
The correct choice is
Problem 5 - c3.4.18 :
A graph of velocity versus
time is shown.
Part (a)
Which of the following graphs best represents an acceleration curve that is consistent with the above velocity curve? The
horizontal axes are scaled identically.
• Recall that acceleration represents the slope of the velocity curve.
• Note that the first portion of the velocity graph has a constant positive slope indicating that the same portion of the acceleration curve
should have a constant positive value.
• Note that the second portion of the velocity graph is constant indicating that the same portion of the acceleration curve should be zero.
• The velocity curve indicates an initially non-zero velocity which has no impact on the acceleration curve.
The correct choice is
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Problem 5 - c3.4.19 :
A graph of velocity versus
time is shown.
Part (a)
Which of the following graphs best represents an acceleration curve that is consistent with the above velocity curve? The
horizontal axes are scaled identically.
• Recall that acceleration represents the slope of the velocity curve.
• Note that the first portion of the velocity graph is constant indicating that the same portion of the acceleration curve should be zero.
• Note that the second portion of the velocity graph has a constant positive slope indicating that the same portion of the acceleration curve
should have a constant positive value.
• The velocity curve indicates an initially non-zero velocity which has no impact on the acceleration curve.
The correct choice is
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Problem 6 - 3.5.6 :
A runner is initially at rest at the starting line of a race. When he hears the starting
gun, he accelerates at a constant rate of , which he maintains until he
crosses the finish line at time . It then takes him an additional to come to a
complete stop at time . Use the given coordinate system where is positive to the
right. Refer to the figure.
Part (a)
Enter an expression for the time, , that it takes for the runner to cross the finish line in terms of and .
Because the runner is accelerating at a constant rate, a kinematic equation can be used here. The kinematic variables involved in the
problem are as follows:
The equation that involves all of these variables is
.
We can eliminate the and the terms since both of these quantities are equal to 0. Solving for :
Part (b)
Enter an expression for the runner’s speed, , when he crosses the finish line in terms of and only.
A kinematic equation can be used. The quantities involved in the problem are as follows:
The equation that involves all of these variables is
.
We can eliminate the term since . Solving for :
100 m
=
0.45
m/
a
i
s
2
t = t
1
5.5
s
t = t
2
x
t
1
d
a
i
x
a
v
0
t
=
=
=
=
d
a
i
0
t
1
x =
+
t +
a
.
x
0
v
0
1
2
t
2
x
0
v
0
t
x
t
t
1
=
=
=
a
1
2
t
2
2x
a
2d
a
i
=
t
1
2d
a
i
v
1
a
i
t
1
a
v
0
v
t
=
=
=
=
a
i
0
v
1
t
1
v =
+ at .
v
0
v
0
= 0
v
0
t
v
v
1
=
=
at
a
i
t
1
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Part (c)
Calculate the runner’s constant acceleration, in meters per second squared, after he crosses the finish line until he comes to
rest.
Because of the constant acceleration, a kinematic equation can be used. For this part of the problem, the final velocity, typically represented
as in kinematics, corresponds to , which is equal to 0. The initial velocity, which we typically write as in kinematics, has the same
value as from when the runner crossed the finish line. The variables involved in this part of the problem are as follows:
In this case, we do not know the distance it takes for the runner to come to a stop, so we use the kinematic equation that does not include .
We rearrange and solve for .
It can be determined that and . These can be combined to determine an expression for in terms of variables in the
problem.
Plugging in:
Problem 6 - 3.5.11 :
A motorist in England is on a road that has a posted speed limit of and is traveling in excess of the
speed limit by . A car pulls out of a parking place into the street in front of the motorist
and stops there. The motorist immediately slams on the brakes and begins decelerating at a rate of .
Part (a)
By what conversion factor do you need to multiply a speed expressed in kilometers per hour in order to obtain the value of
that speed expressed in meters per second?
=
v
1
a
i
t
1
v
v
2
v
0
v
1
a
v
v
0
t
=
=
=
=
a
f
= 0
v
2
=
v
1
a
i
t
1
−
= 5.5 s
t
2
t
1
x
a
f
v
a
a
f
=
=
=
+ at
v
0
−
v
v
0
t
−v
1
−
t
2
t
1
=
v
1
a
i
t
1
=
t
1
2d
a
i
v
1
v
1
=
=
=
a
i
t
1
a
i
2d
a
i
2da
i
√
a
f
=
=
=
=
−v
1
−
t
2
t
1
−
2da
i
√
−
t
2
t
1
−
2(100 m)(0.45 m/
)
s
2
√
5.5 s
−1.725 m/s
2
= −1.725 m/
a
f
s
2
=
50.2
km/hr
v
m
=
10.3
km/hr
v
c
d =
10.4
m
a =
3.04
m/s
2
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Let's begin by using dimensional analysis to convert hours to seconds.
As for kilometers to meters, we know from our metric units that there are 1000 meters in a kilometer. From this, we can set up an equation
to get our conversion factor.
Therefore, our conversion factor is
\[x = 0.2778 \frac{\text{m/s}}{\text{km/h}}
\]
Part (b)
Select an expression for the minimum distance, , the motorist would need to come to a complete stop.
To begin, let's look over our kinematic equations. We know that the initial velocity is the speed limit plus the amount the driver is speeding
by. We also know the acceleration. We want to find the distance travelled. Finally, we know that the final velocity is zero since we want to
find out how long until the car stops. We don't know or care about time right now. Given our known values and what we want to find, we
should use the following kinematic equation.
Now, we just need to plug in our known values to solve. The only thing be careful of is that since the acceleration is opposing the direction
of motion to decelerate the car, our acceleration will be negative in this case.
Part (c)
In terms of the defined quantities, enter an expression for the time it would take the motorist to come to a stop after applying
the brakes.
To begin, we need to select the correct kinematic equation based on our known and unknown variables. We know that the initial velocity is
given by the speed limit plus the amount the car is speeding by. We know the acceleration. We know that the final velocity is zero since we
want to see how long until the car stops. We don't know the time, but we want to find out. Finally, we don't know or care about the
distance travelled. Using this information, we can pick the best kinematic equation.
Now we can use our known values to solve this equation for time. The only thing to be careful of is that deceleration is the same as
backwards acceleration. Thus, we will have a negative acceleration.
1 h =
⋅
= 3600 s
60 min
1 h
60 s
1 min
1 km/h =
m/s
1000
3600
1 km/h = 0.2778 m/s
1 = 0.2778
m/s
km/h
d
c
=
+ 2ad
v
2
f
v
2
i
=
+ 2 (−
)
0
2
(
+
)
v
m
v
c
2
a
b
d
c
0 =
− 2 (
)
(
+
)
v
m
v
c
2
a
b
d
c
2
=
a
b
d
c
(
+
)
v
m
v
c
2
=
d
c
(
+
)
v
m
v
c
2
2a
b
=
+ aΔt
v
f
v
i
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Part (d)
How fast, in meters per second, is the motorist traveling when he hits the car in front of him?
It will be useful to convert the initial speed to meters per second.
We may then solve for the speed upon impact by using the initial distance between the vehicles. Note that the acceleration is negative.
Problem 6 - 3.5.3 (alt) :
A car accelerates in the +
x
direction from rest with a constant acceleration of a
1
= 1.5
m/s
2
for t
1
= 20 s. At that point the driver notices a tree limb that has fallen on the road
and brakes hard for t
2
= 5 s until it comes to a stop.
Part (a)
Write an expression for the car's speed just before the driver begins braking, v
1
.
Looking at kinematic equations, we can see that with constant acceleration the final velocity can be calculated by adding the initial velocity
to the acceleration multiplied by the period of time we are looking at. Since the car starts from rest, the initial velocity is zero and we can
drop that term. This gives us the following equation:
Part (b)
If the limb is on the road at a distance of 550 meters from where the car began its initial acceleration, will the car hit the limb?
0 = (
+
) + (−
) Δt
v
m
v
c
a
b
0 = (
+
) −
Δt
v
m
v
c
a
b
Δt = (
+
)
a
b
v
m
v
c
Δt =
(
+
)
v
m
v
c
a
b
v
i
=
=
=
=
=
+
v
m
v
c
(50.2 km/h) + (10.3 km/h)
60.50 km/h
60.50 km/h × 0.2778
m/s
km/h
16.81 m/s
v
2
f
v
f
=
=
=
+ 2
d
v
2
i
a
b
+ 2
d
v
2
i
a
b
(16.81 m/s
+ 2(−3.04 m/
)(10.4 m)
)
2
s
2
= 14.81 m/s
v
f
=
v
1
a
1
t
1
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To determine if the car hits the branch, we will need to find how far the car traveled before it stopped. To calculate this distance we will
need to use the kinematic equation and apply it twice; once to the car while it is accelerating, and once to the car while it is
stopping. For acceleration, we get the following equation:
For deceleration, we get the following equation:
To find the total distance traveled, we can sum these two equations. However, we have two problems with the deceleration equation in that
we don't know either the final velocity or the final acceleration. Thankfully, we found a formula for the final velocity in part (a):
To find the acceleration, we can use the same kinematic equation we employed to find the final velocity in part (a) and rearrange it to solve
for the acceleration. Two key differences are that this time, there is an initial velocity (which is equal to the final velocity from when the car
was accelerating) and that the final velocity is zero. This gives us the following formula:
Now that we have formulas for both the deceleration and the final velocity, let's plug them into our equation for the distance traveled while
the car is decelerating:
Now that we have equations for both the distance traveled during the car's acceleration and its deceleration, we can add them together,
simplify, and then plug in values to find the total distance the car travels.
Since this distance is less than 550 meters, the car will stop before it hits the limb. The answer is therefore:
No
Part (c)
How far, in meters, from the original location of the limb will the car be when it stops?
In part (b) of this problem, we found that the car travels 375.0 meters before stopping. To find how far the car is from the limb when it
stops, we need only subtract this from the distance the limb was from the car when it started accelerating.
Problem 7 - 3.5.62 :
Starting from rest, a cyclist travels in a straight line from point A to point B in 10.00 min. During the first 2.00 min
of her trip, she maintains a uniform forward acceleration of 0.061
m/s
2
. She then travels at constant velocity for the
next 5.00 min. Next, she slows with constant acceleration, so that she comes to a rest at point B 3.00 min later
Part (a)
What is the magnitude of her acceleration during the last 3.00 min in m/s
2
?
Let the positive direction be from A toward B. We'll start by finding the position and velocity after the first (
). From
and with and ,
d =
t +
a
v
0
1
2
t
2
=
d
1
1
2
a
1
t
2
1
=
+
d
2
v
1
t
2
1
2
a
2
t
2
2
=
v
1
a
1
t
1
0 =
+
v
1
a
2
t
2
−
=
v
1
a
2
t
2
=
−v
1
t
2
a
2
=
−a
1
t
1
t
2
a
2
=
d
2
+
v
1
t
2
1
2
a
2
t
2
2
= (
)
+
a
1
t
1
t
2
1
2
−a
1
t
1
t
2
t
2
2
=
−
a
1
t
1
t
2
1
2
a
1
t
1
t
2
=
1
2
a
1
t
1
t
2
=
d
tot
+
d
1
d
2
=
+
1
2
a
1
t
2
1
1
2
a
1
t
1
t
2
=
(
+
)
1
2
a
1
t
1
t
1
t
2
=
1.5
(20 s) (20 s + 5 s)
1
2
m/s
2
=
375.0 m
d = 550 m − 375.0 m
d = 175.0 m
2.00 min 120 s
v =
+ at
v
0
x =
+
t +
a
x
0
v
0
1
2
t
2
= 0
x
0
= 0
v
0
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Applying the same equations to the middle (
), with and , and ,
For the last (
) the velocity becomes zero, so using with , , we have
Calculating,
Part (b)
What is the distance from A to B in meters?
From with ,
Calculating,
Problem 7 - 3.5.65 :
A police car waits in hiding slightly off the highway. A speeding car is spotted by the police car traveling at speed s
=
25
m/s. At the instant the speeding car passes the police car, the police car accelerates forward from rest at a constant
rate of a
= 2.01
m/s
2
to catch the speeding car. Assume the speeding car maintains its speed.
Part (a)
Write an expression for the time it takes for the police car to catch the speeding car. Use the variables from the problem
statement for your expression.
In order to solve this problem, it's necessary to realize that because the two cars are involved in a chase, they will both travel the same
distance and for the same amount of time. With that in mind, let's write an equation for the distance the speeding car travels using the
kinematic equation .
Next, let's write an equation for the distance the police car travels using the same kinematic equation.
Since is the same in both equations, we can set the right side of each equation equal to one another. From there, we simply need to
simplify to find the requested equation.
Part (b)
How long, in seconds, does it take for the police car to catch the speeding car?
Since we found the equation we need to solve for the time in part (a), here we simply need to plug values into that equation and solve to get
the answer.
v = at =
0.061
(120 s) = 7.320 m/s
m/s
2
x =
a
=
0.061
= 439.2 m
1
2
t
2
1
2
m/s
2
(120 s)
2
5.00 min 300 s
= 439.2 m
x
0
= 7.320 m/s
v
0
a = 0
v =
= 7.320 m/s
v
0
x =
+
t = 439.2 m + (7.320 m/s) (300 s) = 2635 m
x
0
v
0
3.00 min 180 s
v =
+ at
v
0
v = 0
= 7.320 m/s
v
0
a =
∣
∣
∣
0 − 7.320 m/s
180 s
∣
∣
∣
a = 0.04067 m/s
2
x =
+
t +
a
x
0
v
0
1
2
t
2
= 2635 m
x
0
x = 2635 m +
(0 + 7.320 m/s) (180 s)
1
2
x = 3294 m
d =
+ vt +
a
d
0
1
2
t
2
d =
t
v
s
d =
1
2
a
p
t
2
d
= d =
t
1
2
a
p
t
2
v
s
=
t
1
2
a
p
t
2
v
s
t =
2v
s
a
p
t =
2v
s
a
p
=
2(25 m/s)
2.01 m/s
2
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Problem 8 - 3.6.22 :
A dolphin in an aquatic show jumps straight up out of the water at a velocity of 10.5
m/s.
Part (a)
How high does his body rise above the water in meters?
Under a constant acceleration, a velocity is related to the deceleration, initial velocity, and distance by the expression
where v
is the initial velocity in m/s, a is the constant deceleration in m/s
, and d is the distance in m. The final velocity is zero so
Plugging in numbers and converting units as needed,
Part (b)
How long is the dolphin in the air in seconds? Neglect any effects due to his size or orientation.
The time the dolphin is in the air is twice the time it takes to bring its velocity to zero at its highest point out of the water. In general, a
velocity is related to a constant deceleration by the expression
where v
is the initial velocity in m/s, a is the constant deceleration in m/s
, and t is the time in s. Therefore, at the peak the final velocity
is zero,
and
Plugging in numbers and converting units as needed,
Problem 8 - 3.6.36 :
Two basketball players jump upward simultaneously. The first reaches a height of 0.81
m above the ground, while
the second reaches a height of just 0.31
m.
t = 24.88 s
=
− 2ad
m/s
v
2
v
2
0
0
2
= 2ad
v
2
0
d =
v
2
0
(2a)
d =
=
y
0
(10.5 m/s)
2
2
⋅
9.81 m/s
2
= 5.625 m
y
0
v = (
− at) m/s
v
0
0
2
=
t
0
v
0
a
t = 2
=
t
0
2v
0
a
t = 2
⋅
(10.5 m/s)
9.81 m/s
2
t = 2.143 s
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Part (a)
How many seconds after the second player reaches the ground does the first player reach the ground? Neglect air resistance.
Take upward to be the positive direction, so and let the ground be the origin. At the highest point the velocity is zero, so
with in , we have . Substituting this into with and results in
Solving for time, is the time to reach the high point. Similarly, the time to fall from the high point can be calculated using
with , , and , so that . Solving for time gives as the time to fall from
the high point. Thus, the total time in the air is . Subtracting the shorter time from the longer time gives the difference in
landing times:
Calculating,
Problem 8 - 3.6.38 :
A hot-air balloon rises from ground level, moving straight upward at a constant speed of 5.01
m/s. At 20.1
s after
liftoff, a sandbag is accidentally dropped from the balloon. Neglect air resistance.
Part (a)
How long, in seconds, does it take the sandbag to reach the ground from the moment it falls off the balloon?
The height of the balloon at the moment the sadbag is released can be calculated using distance equals speed times time:
Take upward to be the positive direction, so that the acceleration of the sanbag after release is . If the ground is the origin,
then and in the equation , so
Using the quadratic formula,
Calculating the positive root,
Part (b)
How fast is the sandbag moving, in m/s, just before it hits the ground?
Using , and recognising the speed as the magnitude of the displacement, we have
Calculating,
a =
− 9.80 m/s
2
v = 0
v =
+ at
v
0
=
− at
v
0
x =
+
t +
a
x
0
v
0
1
2
t
2
= 0
x
0
x = h
h = −a
+
a
= −
a
t
2
1
2
t
2
1
2
t
2
t =
−2h/a
√
x =
+
t +
a
x
0
v
0
1
2
t
2
= 0
v
0
= h
x
0
x = 0
0 = h +
a
1
2
t
2
t =
−2h/a
√
t = 2
−2h/a
√
Δt = 2
− 2
−2 (0.81 m)
−9.80 m/s
2
−2 (0.31 m)
−9.80 m/s
2
Δt = 0.3101 s
height = (5.01 m/s) (20.1 s) = 100.7 m
a =
− 9.80 m/s
2
x = 0
= 100.7 m
x
0
x =
+
t +
a
x
0
v
0
1
2
t
2
0 = (100.7 m) + (5.01 m/s) t +
−9.80
1
2
m/s
2
t
2
t =
− (5.01 m/s) ±
− 4
−9.80
(100.7 m)
(5.01 m/s)
2
1
2
m/s
2
2
−9.80
1
2
m/s
2
t = 5.073 s
v =
+ at
v
0
v = 5.01 m/s +
−9.80
(5.073 s)
∣
∣
m/s
2
∣
∣
v = 44.71 m/s
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Problem 8 - 3.6.39 :
An object is dropped from the roof of a building of height h
. Neglect air resistance.
Part (a)
During the last 0.51
s of its fall, the object drops a distance h
/3 before hitting the ground. What is h
in meters?
To begin, let us use the kinematic equation to write a formula for the entire fall. For the sake of simplicity, we will let
down be the positive direction.
Now let's repeat this process to get an equation for the first two-thirds of the fall. We know that the time it takes for the object to fall this far
will be the total time minus the time for the final third of the fall .
Right now, we have two unknowns ( and ) and want to find the height. To get the height by itself, we can take the square root of both the
equations we have found so far and subtract them from one another. After we have the height by itself as the only unknown value, we can
plug in values and solve to find the answer.
Problem 9 - c2.2.6 :
The diagram shows four vectors in the x
-
y
plane.
Part (a)
Select all vectors with an x
component of zero.
Looking at the diagram, we can see that all of the vectors but #2 have some horizontal component in the x
-direction. The correct answer is
therefore:
Vector 2
Part (b)
Select all vectors with a y
component of zero.
x =
+
t +
a
x
0
v
0
1
2
t
2
h =
g
1
2
t
2
t
t
f
h =
g
2
3
1
2
t − t
f
2
t
h
−
= t
−
t −
h
h
2
3
g
1
2
t
f
g
1
2
−
= t
− t
+
h
2
3
h
g
1
2
g
1
2
t
f
g
1
2
1 −
=
h
2
3
t
f
g
1
2
=
h
t
f
g
1
2
1−
2
3
h =
g
t
2
f
1
2
1−
2
3
2
=
9.8
(0.51 s)
2
1
2
m/s
2
1−
2
3
2
h = 37.85 m
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Looking at the diagram, we can see that all of the vectors but #23 have some vertical component in the y
-direction. The correct answer is
therefore:
Vector 3
Part (c)
Select all vectors with a negative x
component.
To the left is defined as the negative x
direction on the diagram and we can see that none of the vectors point even slightly to the left. The
correct answer is therefore:
None of the vectors have a negative x
component
Part (d)
Select all vectors with a negative y
component.
Downward is defined as the negative y
direction on the diagram and we can see that vector 1 is the only one that points downward. The
correct answer is therefore:
Vector 1
Part (e)
Select all vectors with a positive x
component.
To the right is defined as the positive x
direction on the diagram and we can see that only vector 2, which points straight up, does not point
to the right. The correct answer is therefore:
Vectors 1, 3, and 4
Part (f)
Select all vectors with a positive y
component.
Upward is defined as the positive y
direction on the diagram and both vectors 2 and 4 point upward. The correct answer is therefore:
Vectors 2 and 4
Problem 10 - 2.3.21 :
A cyclist rides 5.01
km east, then 8.01
km in a direction 20.01
degrees west of north, then 7.01
km west.
Part (a)
What is the magnitude of the total displacement, in km?
Taking to be east and to be north, the diagram shows the three individual displacements.
The magnitudes of the and components of the second displacement are and . The component of the total displacment
is
The component of the total displacment is
The diagram illustrates the total displacment vector.
x
y
x
y
sin
ϕ
d
2
cos
ϕ
d
2
x
Δ
=
−
sin
ϕ
−
= (5.01 km) − (8.01 km) sin (
) − (7.01 km) = −4.741 km
r
x
d
1
d
2
d
3
20.01
∘
y
Δ
=
cos
ϕ
= (8.01 km) cos (
) = 7.526 km
r
y
d
2
20.01
∘
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The magnitude of the displacement is
Calculating,
Part (b)
What is the direction of the displacement, measured in degrees west of north?
From the right triangle in the diagram, , so
Calculating,
Problem 10 - 2.3.22 :
In a hockey game, player A passes the puck to player B, who is standing on the blue line, as
shown in the diagram. The y
axis is perpendicular to the blue line, and the x
axis is parallel to
the blue line, as shown. The puck travels a distance d
1
= 20.1
m on its way to player B,
making an angle θ
= 30.1
degrees with the x
axis. Player B then passes the puck so that it
moves a distance d
2
= 6.1
m on the blue line, in the negative x
direction.
Part (a)
What is the magnitude of the total displacement, in meters?
To calculate the magnitude of the displacement, we will need to sum up the components of the two displacement vectors that the puck
travels along. We can decompose the first vector using trigonometry to get the following equation for the total displacement vector:
Now that we have an equation for the total displacement vector, we can use the formula for magnitude and plug in values to find the correct
answer. When plugging in values, notice that the second displacement is to the left, so the value of will be negative.
Δr =
=
Δ
+ Δ
r
x
2
r
y
2
√
+
(−4.741 km)
2
(7.526 km)
2
Δr = 8.895 km
tan θ =
Δ
/Δ
r
x
r
y
θ = tan
= tan
−1
Δr
x
Δr
y
−1
4.741 km
7.526 km
θ = 32.21
∘
=
d
total
→
+
d
1
→
d
2
→
= (
cosθ,
sinθ) + (
, 0)
d
1
d
1
d
2
= (
cosθ +
,
sinθ)
d
1
d
2
d
1
d
2
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Part (b)
What angle, in degrees, does the total displacement make with the x
axis?
In part (a), we found an equation for the total displacement vector.
To find the angle request angle, we will need to use trigonometry. Tangent is equal to the opposite angle over the adjacent angle, or the y
-
component over the x
-component. With that in mind, we can write the following equation.
By taking the inverse tangent of both sides of this equation and then plugging in values, we can solve for the angle we need. Recall that the
actual value of 's x
-component is negative as the vector points to the left.
Problem 10 - 2.3.25 :
A delivery man starts at the post office, drives 40.0 km north, then 11
km west, then 61
km northeast, and finally 21
km north to stop for lunch. (The direction “northeast” is 45 degrees east of north.)
Part (a)
What is the magnitude of his net displacement vector, in units of km?
Taking north to be the positive direction, and east to be the positive direction, the four displacements are
The net displacment is found by adding these vectors, and the result is
The diagram illustrates the situation
The magnitude of the displacment is
=
d
total
+
(
cosθ +
)
d
1
d
2
2
(
sinθ)
d
1
2
√
=
+ ((20.1 m) sin (30.1°))
((20.1 m) cos (30.1°) − 6.1 m)
2
2
= 15.13 m
d
total
= (
cosθ +
,
sinθ)
d
total
→
d
1
d
2
d
1
tan
=
θ
total
sinθ
d
1
cosθ+
d
1
d
2
d
2
=
θ
total
arctan
sinθ
d
1
cosθ+
d
1
d
2
= arctan
(20.1 m)sin(30.1°)
(20.1 m)cos(30.1°)−6.1 m
= 41.76°
θ
total
y
x
(0 km)
+ (40 km)
i
ˆ
j
ˆ
( − 11 km)
+ (0 km)
i
ˆ
j
ˆ
(61 km)cos(
)
+ (61 km)cos(
)
45
∘
i
ˆ
45
∘
j
ˆ
(0 km)
+ (21 km)
i
ˆ
j
ˆ
Δ
= Δ
+ Δ
r
r
x
i
ˆ
r
y
j
ˆ
= (32.13 km)
+ (104.1 km)
i
ˆ
j
ˆ
Δr =
+
(32.13 km)
2
(104.1 km)
2
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Calculating,
Part (b)
What is the direction of his net displacement? Express your answer an angle measured in degrees east of north.
In the diagram the angle measures the direction east of north, where , so
Calculating,
Problem 10 - 2.3.26 :
An adventurous dog strays from home, runs three blocks east, two blocks north, one block east, one block north, and
two blocks west. Assuming that each block is 81
m.
Part (a)
How far from home is the dog, in units of m?
The net displacement is 2 blocks east and 3 blocks north. Taking north to be the positive direction, and east to be the positive direction,
the net displacement is
The diagram illustrates the situation
The magnitude of the displacment is
Calculating,
Part (b)
In what direction is the dog? Express the direction as an angle measured in degrees north of east.
In the diagram the angle measures the direction north of east, where , so
Calculating,
Problem 11 - 4.2.10 :
An airplane flies horizontally at a speed of 301
km/h and drops a crate that falls to the horizontal ground below.
Neglect air resistance.
Part (a)
If the altitude of the plane was 501
m, then how far, horizontally in meters, did the crate move as it fell to the ground?
Δr = 109.0 km
θ
tan θ =
Δr
x
Δr
y
θ = tan
−1
32.13 km
104.1 km
θ = 17.15
∘
y
x
Δ
= Δ
+ Δ
r
r
x
i
ˆ
r
y
j
ˆ
= 2(81 m)
+ 3(81 km)
i
ˆ
j
ˆ
= (162.0 m)
+ (243.0 km)
i
ˆ
j
ˆ
Δr =
+
(162.0 m)
2
(243.0 m)
2
Δr = 292.0 m
θ
tan θ =
Δr
y
Δr
x
θ = tan
−1
243.0 m
162.0 m
θ = 56.31
∘
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In this problem, we know how fast the crate is moving horizontally when it falls and that it has no horizontal acceleration, but we don't
know how long it takes to fall. Since we have two unknowns (the length of time and horizontal distance traveled) it isn't possible to solve
this problem immediately. Instead, we will need to analyze the vertical fall in order to get an expression for how long the fall takes. Let's
begin using the kinematic equation for the vertical motion of the crate. For the sake of simplicity, we will let downward
be the positive direction here.
Now that we have an equation for time, let's write an equation for the horizontal distance the crate falls and plug this in for time. Then we
can plug in values and solve to find the distance. When we begin solving, it's important to remember to convert the distance from km/h to
m/s in order to get an answer in the correct units.
Part (b)
What was the speed of the crate, in m/s, just before it hit the ground?
While we already know that the final speed of the crate in the horizontal direction is the same as its initial speed, to find the total speed we
will also need to know the final speed in the vertical direction. Recall that we found of the following expression for the total length of time
that the crate falls in part (a):
With this equation we can employ the formula for velocity to find a formula for the final speed of the crate in the y
direction. As
in part (a), let's allow downward to be the positive direction for the sake of simplicity. This gives us the following equation:
Now that we know the final velocities in both the x
and y
directions, we can use the formula for magnitude to find the final speed. As in part
(a), we need to be careful when solving this to convert the given horizontal velocity from km/h to m/s in order to get an answer in the
correct units.
Problem 11 - 4.2.11 :
x =
+ vt +
a
x
0
1
2
t
2
h =
g
1
2
t
2
=
2h
g
t
2
= t
2h
g
x = vt
= v
2h
g
= (301 km/h)
1000 m
1 km
1 h
3600 s
2(501 m)
9.8 m/s
2
x = 845.4 m
t =
2h
g
v =
+ at
v
0
=
v
y
g
2h
g
=
2hg
√
v =
+
v
2
x
v
2
y
=
+
v
2
x
2hg
√
2
=
+ 2hg
v
2
x
√
=
+ 2 (501 m)
9.8
(301 km/h)
1000 m
1 km
1 h
3600 s
2
m/s
2
v = 129.7 m/s
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A secret agent skis off a slope inclined at θ
= 25
degrees below horizontal at a speed
of v
0
= 12
m/s. He must clear a gorge, and the slope on the other side of the gorge is
h
= 10.1
m below the edge of the upper slope.
Part (a)
What is the maximum width, w
, of the gorge (in meters) so that the agent clears it?
Take upward to be the the positive direction, and horizontal to be the positive direction. In the absence of air resistance, the components
of the acceleration are and , where is the acceleration of gravity. The components of the initial velocity are
Let the origin of the coordinate system be at the launch point. The equation in quadratic form, with , is
From the quadratic formula, noting that ,
The two roots are and .
From with , and using the positive root,
Calculating,
Problem 12 - 4.3.28 :
A projectile is launched at ground level with an initial speed of 35
m/s, at an angle of 25
° above the horizontal. It
strikes a target above the ground 2.1
seconds later.
Part (a)
What is the horizontal distance, in meters, from where the projectile was launched to where it hits the target?
The horizontal distance the projectile travels is the product of the elapsed time and the horizontal component of the intial velocity, which
doesn't change throughout the motion, since there is assumed to be no acceleration in the horizontal direction.
y
x
= 0
a
x
=
− g
a
y
g
=
cos θ = (12 m/s) cos(
) = 10.88 m/s
v
0x
v
0
25
∘
= −
sin θ = (12 m/s) sin(
) = −5.071 m/s
v
0y
v
0
25
∘
y =
+
t +
y
0
v
0y
1
2
a
y
t
2
= 0
y
0
0 = −y +
t +
v
0y
1
2
a
y
t
2
y =
− h =
− 10.1 m
t =
−
±
v
0y
− 4
(−y)
v
2
0y
1
2
a
y
2
1
2
a
y
=
− (−5.071 m/s) ±
− 2
−9.80
(10.1 m)
(−5.071 m/s)
2
m/s
2
−9.80 m/s
2
t = 1.009 s
t =
− 2.044 s
x =
+
t
x
0
v
0x
= 0
x
0
x = (10.88 m/s) (1.009 s)
x = 10.97 m
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Part (b)
What is the vertical distance, in meters, from where the projectile was launched to where it hits the target?
The vertical distance the projectile travels can be found by applying the equations of kinematics, since the constant downward acceleration
due to gravity always acts on the projectile.
Problem 12 - 4.3.29 :
A ball is kicked at ground level with an initial velocity of 15
m/s in the horizontal direction and 10.5
m/s in the
vertical direction.
Part (a)
At what speed does the ball hit the ground in m/s?
Due to the symmetry of the problem, the magnitude of the final vertical component of the initial velociy will be the same as that of the
initial vertical component. The horizontal component does not change during the motion, assuming no acceleration in the horizontal
direction. Therefore, the magnitude of the final velocity is given by the Pythagorean theorem.
Part (b)
For how long does the ball remain in the air in seconds?
Due to the symmetry of the problem, the total time of flight can be found by first finding the time to reach the highest point, then
multiplying that result by 2. Equivalently, this time is one half the total elapsed time, . We can apply the equations of kinematics again to
find this time because at the highest point, the speed of the ball is momentarily zero in the vertical direction.
Solving for the time gives,
x =
cos (θ) t
v
0
= (35 m/s) cos (25°) (2.1 s)
x = 66.61 m
y =
t +
a
v
0y
1
2
t
2
=
sin (θ) t −
g
v
0
1
2
t
2
= (35 m/s) sin (25°) (2.1 s) −
9.81
1
2
m/s
2
(2.1 s)
2
y = 9.431 m
=
v
f
+
v
2
x
v
2
y
=
+
(15 m/s)
2
(10.5 m/s)
2
= 18.31 m/s
v
f
t
=
+
=
− g
v
y
v
0y
a
y
t
2
v
0y
t
2
t =
2v
0y
g
=
2(10.5 m/s)
9.81 m/s
2
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Part (c)
What maximum height is attained by the ball in meters?
The vertical distance from the ground to the highest point can be found by applying the equations of kinematics using the fact that at the
highest point, the speed of the ball is momentarily zero in the vertical direction.
Solving for the vertical distance when the final velocity is zero gives,
Problem 12 - 4.3.28 (alt) :
A projectile is launched at ground level with an initial speed of 150
ft/s, at an angle of 25
° above the horizontal. It
strikes a target above the ground 2.2
seconds later.
Part (a)
What is the horizontal distance, in feet, from where the projectile was launched to where it lands?
The horizontal launch speed of the projectile is , where denotes the given initial speed and is the given launch angle above the
horizontal. The horizontal distance that the projectile travels during the given time is, accordingly,
We substitute the given values,
Part (b)
What is the vertical distance, in feet, from where the projectile was launched to where it lands?
The vertical launch speed of the projectile is , where denotes the given initial speed and is the given launch angle above the
horizontal. The landing height of the projectile, after time , which is the projectile's vertical distance from launch to landing, is
We substitute the given values, including ,
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t = 2.141 s
=
+ 2
y =
− 2gy
v
2
y
v
2
0y
a
y
v
2
0y
y =
v
2
0y
2g
=
(10.5 m/s)
2
2 9.81 m/s
2
y = 5.619 m
vcos(θ)
v
θ
x
t
x = vcos (θ) t .
x = (150 ft/s) cos (25°) (2.2 s) .
x = 299.1 ft
vsin(θ)
v
θ
y
t
y = vsin (θ) t −
g
.
1
2
t
2
g = 32.2 ft/s
2
y = (150 ft/s) sin (25°) (2.2 s) −
32.2
.
1
2
ft/s
2
(2.2 s)
2
y = 61.54 ft
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