Physics: Principles and Problems
Physics: Principles and Problems
9th Edition
Elliott, Haase, Harper, Herzog, Margaret Zorn, Nelson, Schuler, Zitzewitz
ISBN: 9780078458132
Textbook solutions

All Solutions

Page 250: Assessment

Exercise 32
Step 1
1 of 2
Exercise scan
Result
2 of 2
(force),(time)$rightarrow$(impulse)$rightarrow$(momentum)$leftarrow$(mass),(velocity)
Exercise 33
Step 1
1 of 2
Momentum depends on mass and velocity:

$$
p=mv
$$

The answer is $textbf{yes}$, because it has smaller mass its velocity has to be bigger.

Result
2 of 2
yes
Exercise 34
Step 1
1 of 2
a)

They both exert the same magnitude of the impulse on the ball because there is the same change in magnitude of momentum.

b)

Catcher while caching the ball applies the force in shorter time, to have the same impulse the force has to be larger.

Result
2 of 2
a) same

b) catcher

Exercise 35
Solution 1
Solution 2
Step 1
1 of 2
If acceleration is 0, then velocity will be constant. Hence the momentum will be constant

$$
text{color{#c34632}Remember that : Linear momentum = Mass $times$ Velocity}
$$

Notice that this is true only about linear momentum, angular momentum can change even if the net force on the system is 0

Result
2 of 2
$$
text{color{#4257b2}No change in Linear momentum can occur if net force is 0}
$$
Step 1
1 of 1
The momentum of an object is equal to the mass of the object times the object’s velocity, but it is also the product of the average force on an object and the time interval over which it acts. If no net force is exerted on a system, then the product of the force and time is zero, and hence, the net change in momentum is zero. However, the linear momentum of individual components of a system may still have non-zero linear momentum.
Exercise 36
Step 1
1 of 2
When we crash we have change in momentum, but we can have that change with bigger or smaller force, it depends on the time. Bumpers can extend that time and average force on us would be smaller.
Result
2 of 2
To extend time of the crash
Exercise 37
Step 1
1 of 2
a) The skater’s angular momentum can be changed by external torque.

b) The skater can decrease his inertia, and that would result in increasing angular velocity. He can do that by joining his hand with his body.

Result
2 of 2
a) external torque

b) decreasing inertia

Exercise 38
Step 1
1 of 2
An isolated system is system that does not have any interaction with anything outside of the system. There are no external forces on the system.
Result
2 of 2
There are no external forces on the system.
Exercise 39
Step 1
1 of 2
Total momentum has to be conserved, hence if the gas has change in momentum in negative direction that means that the rocket has to have change in momentum in positive direction.
Result
2 of 2
Total momentum is conserved.
Exercise 40
Step 1
1 of 2
If we use equation for conservation of momentum we will get that the eight ball has the same velocity as cue ball before collision.
Result
2 of 2
Same as cue ball before collision.
Exercise 41
Step 1
1 of 2
a) Because gravity acts on the ball as an external force so this system is not closed system.

b) The momentum is conserved when we have in system earth and the ball.

Result
2 of 2
a) because of the external force.

b) Earth and ball.

Exercise 42
Step 1
1 of 2
a) During collision there is external force on the ball that changes its momentum.

b) We have to include basketball and the floor in the system.

Result
2 of 2
a) There is external force.

b) Basketball and the floor

Exercise 43
Step 1
1 of 2
Brakes acts on wheels and that is internal interaction between components of the car but the wheels have interaction with the ground and friction between wheels and ground is that external force that changes momentum.
Result
2 of 2
Friction is external force.
Exercise 44
Step 1
1 of 2
Child have to apply external torque on the circular-motion ride. That means that child has to be beside the ride and make interaction, or if the child is on the ride, child have to make interaction with something external like ground or something similar.
Result
2 of 2
Child have to apply external torque.
Exercise 45
Step 1
1 of 2
When you apply external force on the system over some time you will change its momentum.
Result
2 of 2
When you apply external force on the system over some time you will change its momentum.
Exercise 46
Step 1
1 of 2
Yes, object can obtain a larger impulse from smaller force if that force is acting on it for longer period of time.

$$
impulse=Ft
$$

Result
2 of 2
Yes
Exercise 47
Step 1
1 of 2
You should move your hands in the same direction as the moving ball, because to stop the ball you have to change its momentum and you want to do it in longer period of time so that average force is smaller.

$$
Delta p=Ft
$$

Result
2 of 2
In the same direction as the moving ball.
Exercise 48
Step 1
1 of 2
The only difference can be is that on faster bullet force acts in larger period of time and bullet gains more momentum.
Result
2 of 2
On faster bullet force acts in larger period of time.
Exercise 49
Step 1
1 of 2
A)

After impulse A an object has an change in momentum:

$$
Delta p=Ft=2cdot2=4,,rm kgm/s
$$

during that time an object accelerate.

B)

After impulse A an object has an change in momentum:

$$
Delta p=Ft=-2cdot2=-4,,rm kgm/s
$$

during that time an object deaccelerate.

C)

After impulse A an object has an change in momentum:

$$
Delta p=Ft=-2cdot=-2,,rm kgm/s
$$

during that time an object accelerate but in opposite direction.

Result
2 of 2
A) accelerate

B) deaccelerate

C) accelerate in opposite direction.

Exercise 50
Step 1
1 of 2
When an astronaut point a gas pistol in opposite direction and start using it, pistol will eject gas out and because the momentum has to be conserved astronaut will have change in momentum in direction of the ship.
Result
2 of 2
Momentum in closed system has to be conserved.
Exercise 51
Step 1
1 of 2
In this system we have to include a wall and a tennis ball to have conserved momentum, because change in momentum of a tennis ball is the same in magnitude but opposite direction as a wall.
Result
2 of 2
System is a ball and a wall.
Exercise 52
Step 1
1 of 2
You could turn your engine in direction of velocity and start to eject gas from the engine, because momentum must be conserved the ship would gain the same magnitude of momentum as the gas but in the opposite direction.
Result
2 of 2
You could turn your engine in direction of velocity and start to eject gas.
Exercise 53
Step 1
1 of 2
If we use conservation of momentum and assume that two trucks are identical we would get:

$$
mv=2mv’rightarrow v’=frac{v}{2}
$$

But they are moving more than half the speed of the moving truck and that means that moving truck must have bigger mass.

Result
2 of 2
Moving truck must have bigger mass.
Exercise 54
Step 1
1 of 2
Because of conservation of momentum change in momentum of bullet is the same in magnitude but opposite in direction of a rifle and if you do not have firm grip on a rifle, a rifle could fall out of hands or hit you in the head.
Result
2 of 2
A rifle could fall out of hands.
Exercise 55
Step 1
1 of 2
The rubber bullet have grater change in momentum then aluminum bullet because it bounces off, hence change in momentum of the wood would be grater if its shut with rubber bullet and its speed after collision is faster.
Result
2 of 2
Rubber bullet.
Exercise 56
Step 1
1 of 2
Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=Delta p\
Ft&=mv\
t&=frac{mv}{F}\
&=frac{0.058cdot62}{272}
end{align*}
$$

$$
boxed{t=0.013,,rm s}
$$

Result
2 of 2
$$
t=0.013,,rm s
$$
Exercise 57
Step 1
1 of 2
a)

Change in momentum is equal to:

$$
begin{align*}
Delta p&=mv’-mv\
&=0.145cdot(-58)-0.145cdot42
end{align*}
$$

$$
boxed{Delta p=-14.5,,rm kgm/s}
$$

b)

Impulse is equal to the change in momentum:

$$
begin{align*}
Ft&=Delta p\
F&=frac{Delta p}{t}\
&=frac{-14.5}{4.6cdot10^{-4}}
end{align*}
$$

$$
boxed{F=-31522,,rm N}
$$

Result
2 of 2
a) $Delta p=-14.5,,rm kgm/s$

b) $F=-31522,,rm N$

Exercise 58
Step 1
1 of 4
Given values from the problem are the force $F$ acting upon the bowling ball, the mass $m$ of the bowling ball, and the time $Delta{t}$ duration in which there is force being acted upon the bowling ball.

$$
begin{align*}
F &= 186 ,mathrm{N}\
m &= 7.3 ,mathrm{kg} \
Delta{t} &= 0.40 ,mathrm{s}
end{align*}
$$

Step 2
2 of 4
$textbf{Change in Momentum.}$

Given the formula such that $Delta{p}$ is the change in momentum, $F$ is the force acting upon the object, and time $t$ is the duration in which the force is acting upon the same object.

$$
begin{equation}
Delta{p} = FDelta{t}
end{equation}
$$

We can solve for the momentum by plugging in the given values.

$$
begin{align*}
Delta{p} &= FDelta{t}\
&= (186,mathrm{N})(0.40,mathrm{s})\
&= 74 N cdot s\
&= boxed{74 ,mathrm{kg}cdot mathrm{frac{m}{s}}}
end{align*}
$$

Step 3
3 of 4
$$
textbf{Change in Velocity.}
$$

Given the formula where $Delta{v}$ is the change in velocity, $Delta{p}$ is the change in momentum, and $m$ is the mass.

$$
begin{equation}
Delta{v} = frac{Delta{p}}{m}
end{equation}
$$

We can solve for the momentum by using $Delta{p}$ acquired from the previous solution and the mass($m$) in the given values.

$$
begin{align*}
Delta{v} &= frac{Delta{p}}{m}\
&= frac{74 ,mathrm{kg}cdot mathrm{frac{m}{s}}}{7.3,mathrm{kg}}\
&= boxed{10 ,mathrm{frac{m}{s}}}
end{align*}
$$

Result
4 of 4
$Delta{p} = 74 ,mathrm{kg}cdot mathrm{frac{m}{s}}$ and $Delta{v} = 10 ,mathrm{frac{m}{s}}$
Exercise 59
Step 1
1 of 2
Given: $m=5500,,rm kg$, $v_1=4.2,,rm m/s$, $v_2=7.8,,rm m/s$, $t=15,,rm s$

a)

We can calculate change in momentum:

$$
Delta p=mv_2-mv_1=5500cdot7.8-5500cdot4.2
$$

$$
boxed{Delta p=19800,,rm kgm/s}
$$

b)

Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=Delta p\
F&=frac{Delta p}{t}\
&=frac{19800}{15}
end{align*}
$$

$$
boxed{F=1320,,rm N}
$$

Result
2 of 2
a) $Delta p=19800,,rm kgm/s$

b) $F=1320,,rm N$

Exercise 60
Step 1
1 of 2
Given: $m=6,,rm g$, $v=350,,rm m/s$, $t=1.8,,rm ms$

Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=mv\
F&=frac{mv}{t}\
&=frac{6cdot10^{-3}cdot350}{1.8cdot10^{-3}}
end{align*}
$$

$$
boxed{F=1167,,rm N}
$$

Result
2 of 2
$$
F=1167,,rm N
$$
Exercise 61
Step 1
1 of 2
Given: $m=0.24,,rm kg$, $v_1=3.8,,rm m/s$, $v_2=-2.4,,rm m/s$, $t=0.025,,rm s$

Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=mv_2-mv_1\
F&=frac{mv_2-mv_1}{t}\
&=frac{0.24cdot(-2.4)-0.24cdot3.8}{0.025}
end{align*}
$$

$$
boxed{F=59.5,,rm N}
$$

Result
2 of 2
$$
F=59.5,,rm N
$$
Exercise 62
Step 1
1 of 2
The impulse given to the puck is:

$$
I = Delta p = F Delta t = (30.0) (0.16) = 4.8 Kg.m/s
$$

Result
2 of 2
$$
4.8 Kg.m/s
$$
Exercise 63
Step 1
1 of 2
Given: $m_1=35.6,,rm kg$, $m=1.3,,rm kg$, $v=9.5,,rm m/s$

Combined momentum is equal to:

$$
begin{align*}
p&=(m_1+m_2)v\
&=(35.6+1.3)cdot9.5
end{align*}
$$

$$
boxed{p=350.6,,rm kgm/s}
$$

Result
2 of 2
$$
p=350.6,,rm kgm/s
$$
Exercise 64
Step 1
1 of 2
The impulse given to the puck increases its momentum:

$p = F t = (30.0) (0.16) = 4.8 Kg.m/s$

Its speed is:

$$
v = dfrac{p}{m} = dfrac{4.8}{0.115} = 42 m/s
$$

Result
2 of 2
$$
42 m/s
$$
Exercise 65
Step 1
1 of 2
Given: $m=25,,rm kg$, $v_1=12,,rm m/s$, $v_a=8,,rm m/s$, $v_b=-8,,rm m/s$

a)

Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=mv_a-mv_1\
&=25cdot8-25cdot12\
end{align*}
$$

$$
boxed{Ft=-100,,rm kgm/s}
$$

b)

Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=mv_a-mv_1\
&=25cdot(-8)-25cdot12\
end{align*}
$$

$$
boxed{Ft=-500,,rm kgm/s}
$$

Result
2 of 2
a) $Ft=-100,,rm kgm/s$

b) $Ft=-500,,rm kgm/s$

Exercise 66
Step 1
1 of 2
Given: $m=0.15,,rm kg$, $v_1=12,,rm m/s$

Area under the graph is change in momentum:

$$
begin{align*}
Delta p&=2cdotleft(frac{2cdot1}{2}right)\
Delta p&=2,,rm kgm/s
end{align*}
$$

now we can calculate speed:

$$
mv_1+Delta p=mvrightarrow v=frac{mv_1+Delta p}{m}=frac{0.15cdot12+2}{0.15}
$$

$$
boxed{v=25,,rm m/s}
$$

Result
2 of 2
$$
v=25,,rm m/s
$$
Exercise 67
Step 1
1 of 2
Given: $m=0.145,,rm kg$, $v=35,,rm m/s$

a)

Change in momentum is equal to:

$$
Delta p=mv=0.145cdot35
$$

$$
boxed{Delta p=5.075,,rm kgm/s}
$$

b)

Impulse is equal o change in momentum:

$$
begin{align*}
Ft&=Delta p\
F&=frac{Delta p}{t}\
&=frac{5.075}{0.05}
end{align*}
$$

$$
boxed{F=101.5,,rm N}
$$

b)

Impulse is equal o change in momentum:

$$
begin{align*}
Ft&=Delta p\
F&=frac{Delta p}{t}\
&=frac{5.075}{5}
end{align*}
$$

$$
boxed{F=10.15,,rm N}
$$

Result
2 of 2
a) $Delta p=5.075,,rm kgm/s$

b) $F=101.5,,rm N$

c) $F=10.15,,rm N$

Exercise 68
Step 1
1 of 2
Given: $m=0.115,,rm kg$, $v_1=37,,rm m/s$, $v_2=-25,,rm m/s$

a)

Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=mv_2-mv_1\
&=0.115cdot(-25)-0.115cdot37
end{align*}
$$

$$
boxed{Ft=-7.13,,rm kgm/s}
$$

b)

Average force is equal to:

$$
F=frac{Ft}{t}=frac{-7.13}{5cdot10^{-4}}
$$

$$
boxed{F=-14260,,rm N}
$$

Result
2 of 2
a) $Ft=-7.13,,rm kgm/s$

b) $F=-14260,,rm N$

Exercise 69
Step 1
1 of 2
a)

To calculate impulse we can use difference in momentum:

$$
begin{align*}
Ft&=p_2-p_1\
&=mv_2-mv_1\
&=4.7cdot10^{-26}cdot(-550)-4.7cdot10^{-26}cdot550
end{align*}
$$

$$
boxed{Ft=-5.17cdot10^{-23},,rm kgm/s}
$$

We put minus sign on $v_2$ because it is in opposite direction.

b)

We can calculate average force by using the definition of impulse, for time duration we will put one second and for number of collisions we will put the number of collisions in one second:

$$
begin{align*}
F&=nfrac{Ft}{t}\
&=1.5cdot10^{23}frac{-5.17cdot10^{-23}}{1}
end{align*}
$$

$$
boxed{F=-7.76,,rm N}
$$

Result
2 of 2
a) $Ft=-5.17cdot10^{-23},,rm kgm/s$

b) $F=F=-7.76,,rm N$

Exercise 70
Step 1
1 of 2
To calculate time that should it be fired we can use that impulse is equal to change in momentum:

$$
begin{align*}
Ft&=mv\
t&=frac{mv}{F}\
&=frac{72000cdot63cdot10^{-2}}{35}
end{align*}
$$

$$
boxed{t=1296,,rm s}
$$

Result
2 of 2
$$
t=1296,,rm s
$$
Exercise 71
Step 1
1 of 3
To calculate vertical velocity of a bale of hay we can use conservation of energy:

$$
begin{align*}
mgh&=frac{mv_v^2}{2}\
v_v&=sqrt{2gh}\
v_v&=sqrt{2cdot9.81cdot60}\
v_v&=34.3,,rm m/s
end{align*}
$$

We can get mass of hey from weight:

$$
begin{align*}
F_g&=mg\
m&=frac{F_g}{g}\
m&=frac{175}{9.81}\
m&=17.85,,rm kg
end{align*}
$$

Now we can calculate magnitude of the momentum in vertical direction:

$$
begin{align*}
p_v&=mv_v\
p_v&=17.85cdot1177.2\
p_v&=612.4,,rm kgm/s
end{align*}
$$

Horizontal velocity is the same as planes:

$$
v_h=36,,rm m/s
$$

And magnitude of momentum in horizontal direction is:

$$
begin{align*}
p_h&=mv_v\
p_h&=17.85cdot36\
p_h&=642.2,,rm kgm/s
end{align*}
$$

Now we can calculate magnitude of total momentum:

$$
begin{align*}
p&=sqrt{p_v^2+p_h^2}\
p&=sqrt{612.4^2+642.2^2}
end{align*}
$$

$$
boxed{p=887.4,,rm kgm/s}
$$

Step 2
2 of 3
We can calculate direction with equation:

$$
begin{align*}
tanphi=frac{p_v}{p_h}\
tanphi=frac{612.4}{642.2}
end{align*}
$$

$$
boxed{phi=44rm^o,,, towards,, the,, center,, of,, the,, earth}
$$

Result
3 of 3
$$
p=887.4,,rm kgm/s
$$

$$
phi=44rm^o
$$

Exercise 72
Step 1
1 of 3
a)

Impulse is equal to change in momentum:

$$
begin{align*}
Ft&=mv\
Ft&=20cdot10
end{align*}
$$

$$
boxed{Ft=200,,rm kgm/s}
$$

b)

Now when we have impulse we can get average force because impulse is equal to force times time:

$$
begin{align*}
F=frac{Ft}{t}\
F=frac{200}{0.05}
end{align*}
$$

$$
boxed{F=4000,,rm N}
$$

Step 2
2 of 3
c)

We can calculate mass of an object whose weight equals the force with equation:

$$
begin{align*}
F_g&=mg\
m&=frac{F_g}{g}\
m&=frac{4000}{9.81}
end{align*}
$$

$$
boxed{m=408,,rm kg}
$$

d)

World record in lifting weight is 501 kg in deadlift, in that movement human uses almost every muscle, we can conclude that using just arm human $textbf{can not lift that weight}$.

e)

Because restraining seat is build to $textbf{prolongs the time}$ in which force acts on the child, hence the average force is smaller.

Result
3 of 3
a) $Ft=200,,rm kgm/s$

b) $F=4000,,rm N$

c) $m=408,,rm kg$

d) No

e) prolongs the time

Exercise 75
Step 1
1 of 4
To solve this you can use equation for conservation of momentum, because momentum before release and after has to be the same.
Step 2
2 of 4
$$
begin{align*}
m_1v_1+m_2v_2=m_1v_1’+m_2v_2’\
end{align*}
$$
Step 3
3 of 4
In this case velocity before release is zero for both carts, after the release they have velocity in opposite directions so we have to put minus sign in front of one of them.

$$
begin{align*}
5cdot0+2cdot0&=5cdot0.12-2v_2’\
v_2’&=frac{5cdot0.12}{2}
end{align*}
$$

$$
boxed{v_2’=0.3,,rm m/s}
$$

Result
4 of 4
$$
v_2’=0.3,,rm m/s
$$
Exercise 76
Step 1
1 of 4
To solve this you can use equation for conservation of momentum, because momentum before launch and after has to be the same.
Step 2
2 of 4
$$
begin{align*}
m_1v_1+m_2v_2=m_1v_1’+m_2v_2’\
end{align*}
$$
Step 3
3 of 4
In this case velocity before launch is the same for both projectile and launcher.

$$
begin{align*}
4.65cdot2+50cdot10^{-3}cdot2&=4.65v_1’+50cdot10^{-3}cdot647\
v_1’&=frac{4.65cdot2+50cdot10^{-3}cdot2-50cdot10^{-3}cdot647}{4.65}
end{align*}
$$

$$
boxed{v_1’=-4.9,,rm m/s}
$$

Result
4 of 4
$$
v_1’=-4.9,,rm m/s
$$
Exercise 77
Step 1
1 of 4
To solve this you can use equation for conservation of momentum, because momentum before collision and after has to be the same.
Step 2
2 of 4
$$
begin{align*}
m_1v_1+m_2v_2=m_1v_1’+m_2v_2’\
end{align*}
$$
Step 3
3 of 4
$$
begin{align*}
8.5cdot 0+12cdot10^{-3}cdot150&=8.5v_1′-12cdot10^{-3}cdot10^{2}\
v_2’&=frac{12cdot10^{-3}cdot150+12cdot10^{-3}cdot10^{2}}{8.5}
end{align*}
$$

$$
boxed{v_1’=0.35,,rm m/s}
$$

Result
4 of 4
$$
v_1’=0.35,,rm m/s
$$
Exercise 78
Step 1
1 of 4
To solve this you can use equation for conservation of momentum, because momentum before Kofi jumps off and after has to be the same.
Step 2
2 of 4
$$
begin{align*}
m_1v_1+m_2v_2=m_1v_1’+m_2v_2’\
end{align*}
$$
Step 3
3 of 4
In this case velocity before is the same for Kofi and skateboard, after Kofi jumps skateboard has velocity zero.

$$
begin{align*}
42cdot1.2+2cdot1.2&=42v_1′-2cdot0\
v_1’&=frac{42cdot1.2+2cdot1.2}{42}
end{align*}
$$

$$
boxed{v_1’=1.26,,rm m/s}
$$

The sign of velocity that we got is plus, that means that he jumped in the same direction as he was moving before.

Result
4 of 4
$$
v_1’=1.26,,rm m/s
$$
Exercise 79
Step 1
1 of 8
To solve this you can use equation for conservation of momentum in each direction, because momentum before collision and after has to be the same.
Step 2
2 of 8
1.

$$
begin{align*}
m_1v_{x1}+m_2v_{x2}=m_1v_{x1}’+m_2v_{x2}’\
end{align*}
$$

2.

$$
begin{align*}
m_1v_{y1}+m_2v_{y2}=m_1v_{y1}’+m_2v_{y2}’\
end{align*}
$$

Step 3
3 of 8
Because the angle between $x$ and $y$ component is $45,rm ^o$, they have the same magnitude.

1.

$$
begin{align*}
m_1v_{x1}+m_2cdot0&=m_1v_{x1}’+m_2v_{x2}’\
end{align*}
$$

2.

$$
begin{align*}
m_1v_{y1}’&=m_2v_{y2}’\
m_1v_{x1}’&=m_2v_{x2}’\
end{align*}
$$

Step 4
4 of 8
Now when we put equation 2. in equation 1. we get:

$$
begin{align*}
m_1v_{x1}&=m_2v_{x2}’+m_2v_{x2}’\
v_{x2}’&=frac{m_1v_{x1}}{2m_2}\
v_{x2}’&=frac{0.16cdot4}{2cdot0.16}\
v_{x2}’&=2,,rm m/s
end{align*}
$$

Step 5
5 of 8
Now we calculate for other ball:

$$
begin{align*}
m_1v_{x1}&=m_1v_{x1}’+m_1v_{x1}’\
v_{x1}’&=frac{m_1v_{x1}}{2m_1}\
v_{x1}’&=frac{0.16cdot4}{2cdot0.16}\
v_{x1}’&=2,,rm m/s
end{align*}
$$

Step 6
6 of 8
We know that the angle is 45$rm ^o$ so we can use sinus of that angle to get total velocity.
Step 7
7 of 8
$$
begin{align*}
sin{45mathrm{^o}}&=frac{v_{x1}’}{v_1′}\
v_1’&=frac{v_{x1}’}{sin{45mathrm{^o}}}
end{align*}
$$

$$
boxed{v_1’=2.8,,rm m/s}
$$

$$
begin{align*}
sin{45mathrm{^o}}&=frac{v_{x2}’}{v_2′}\
v_2’&=frac{v_{x2}’}{sin{45mathrm{^o}}}
end{align*}
$$

$$
boxed{v_2’=2.8,,rm m/s}
$$

Result
8 of 8
$$
v_1’=2.8,,rm m/s
$$

$$
v_2’=2.8,,rm m/s
$$

Exercise 80
Step 1
1 of 4
To solve this you can use equation for conservation of momentum, because momentum before collision and after has to be the same.
Step 2
2 of 4
$$
begin{align*}
m_1v_1+m_2v_2=m_1v_1’+m_2v_2’\
end{align*}
$$
Step 3
3 of 4
In this case velocity before collision velocity of 825 kg compact car is zero, after the release both cars have the same velocity.

$$
begin{align*}
2575v_1+825cdot0&=2575cdot8.5+825cdot8.5\
v_1&=frac{2575cdot8.5+825cdot8.5}{2575}
end{align*}
$$

$$
boxed{v_1=11.2,,rm m/s}
$$

Result
4 of 4
$$
v_1=11.2,,rm m/s
$$
Exercise 82
Step 1
1 of 4
To solve this you can use equation for conservation of momentum, because momentum before release and after has to be the same.
Step 2
2 of 4
$$
begin{align*}
m_1v_1+m_2v_2=m_1v_1’+m_2v_2’\
end{align*}
$$
Step 3
3 of 4
$$
begin{align*}
0.2cdot0.3+0.1cdot0.1&=0.2v_1’+0.1cdot0.26\
v_2’&=frac{0.2cdot0.3+0.1cdot0.1-0.1cdot0.26}{0.2}
end{align*}
$$

$$
boxed{v_1’=0.22,,rm m/s}
$$

Result
4 of 4
$$
v_1’=0.22,,rm m/s
$$
Exercise 83
Step 1
1 of 6
We have to calculate change in the object’s momentum and velocity and it is given that constant force on the object is 6 N for 10 s an its mass is 3 kg.
Step 2
2 of 6
Change in momentum is equal to impulse generated by constant force.

$$
begin{align*}
Ft&=Delta p\
end{align*}
$$

Step 3
3 of 6
Now we put numbers in and we get that change in momentum is:

$$
begin{align*}
Delta p=6cdot10\
end{align*}
$$

$$
boxed{Delta p=60,,rm kgm/s}
$$

Step 4
4 of 6
Momentum is defined as mass times velocity, so we can get change in velocity from that.

$$
begin{align*}
Delta p&=p_2-p_1\
Delta p&=mv_2-mv_1\
Delta p&=m(v_2-v_1)\
Delta p&=mDelta v\
Delta v&=frac{Delta p}{m}
end{align*}
$$

Step 5
5 of 6
Now we put numbers and change in velocity is:

$$
begin{align*}
Delta v=frac{60}{3}
end{align*}
$$

$$
boxed{Delta v=20,,rm m/s}
$$

Result
6 of 6
$$
Delta p=60,,rm kgm/s
$$

$$
Delta v=20,,rm m/s
$$

Exercise 84
Step 1
1 of 6
In part $textbf{a}$ we have to calculate change in momentum of the car and in part $textbf{b}$ we have to calculate magnitude of the force. It is given that mass of the car is 625 kg and that velocity is changed from 10 m/s to 44 m/s in 68 s by external, constant force.
Step 2
2 of 6
a)

Momentum is defined as mass times velocity, so we can get change in momentum if we know the change in velocity.

$$
begin{align*}
Delta p&=p_2-p_1\
Delta p&=mv_2-mv_1\
Delta p&=m(v_2-v_1)\
end{align*}
$$

Step 3
3 of 6
Now we can put numbers an we can get change in momentum:

$$
Delta p=625cdot(44-10)
$$

$$
boxed{Delta p=21250,,rm kgm/s}
$$

Step 4
4 of 6
b)

Change in momentum is equal to impulse generated by constant force.

$$
begin{align*}
Ft&=Delta p\
F&=frac{Delta p}{t}
end{align*}
$$

Step 5
5 of 6
Now we can put numbers and get average force on the car.

$$
begin{align*}
F=frac{21250}{68}\
end{align*}
$$

$$
boxed{F=312.5,,rm N}
$$

Result
6 of 6
a) $Delta p=21250,,rm kgm/s$

b) $F=312.5,,rm N$

Exercise 85
Step 1
1 of 7
In par $textbf{a}$ we have to calculate change in momentum of the dragster, in part $textbf{b}$ we have to calculate average force on the dragster and in part $textbf{c}$ we have to name what exerts that force.
Step 2
2 of 7
a)

Momentum is defined as mass times velocity.

$$
begin{align*}
Delta p&=p_2-p_1\
Delta p&=mv_2-mv_1\
Delta p&=m(v_2-v_1)\
end{align*}
$$

Step 3
3 of 7
Now we can put numbers and we can get change in momenum:

$$
Delta p=845cdot(27.78-0)
$$

$$
boxed{Delta p=23474,,rm kgm/s}
$$

Step 4
4 of 7
b)

Change in momentum is equal to impulse generated by force.

$$
begin{align*}
Ft&=Delta p\
F&=frac{Delta p}{t}
end{align*}
$$

Step 5
5 of 7
Now we can put numbers and we can get average force:

$$
F=frac{23474}{0.9}
$$

$$
boxed{F=26082,,rm N}
$$

Step 6
6 of 7
c)

That force is exerted by the race track. Because that force is friction between dragster and race track.

Result
7 of 7
a) $Delta p=23474,,rm kgm/s$

b) $F=26082,,rm N$

c) race track

Exercise 86
Step 1
1 of 4
A hockey puck strikes a jacket and they slide off together. It is given that hockey puck has mass of 0.115 kg and it has speed of 35 m/s before collision and jacket has mass of 0.365 kg. We have to calculate their velocity after collision. We assume that there is no friction.
Step 2
2 of 4
To solve this you can use equation for conservation of momentum, because momentum before collision and after has to be the same.

$$
begin{align*}
m_1v_1+m_2v_2=m_1v_1’+m_2v_2’\
end{align*}
$$

Step 3
3 of 4
When we put numbers we get that their velocity is:

$$
begin{align*}
0.115cdot35+0.365cdot0&=0.115v’+0.365v’\
v’&=frac{0.115cdot35}{0.115+0.365}
end{align*}
$$

$$
boxed{v’=8.39,,rm m/s}
$$

Result
4 of 4
$$
v’=8.39,,rm m/s
$$
Exercise 88
Step 1
1 of 7
In this problem gymnast is performing a routine in which she does giant swings on the bar holding her body straight, then she lets go of the bar and grabs her knees with her hands, in the final act she straightens up and lands. In part $textbf{a}$ we have to answer around which axis she spin, in part $textbf{b}$ we have to rank, from greatest to least, her momentum of inertia for three positions and in part $textbf{c}$ we have to rank, from greatest to least, here angular velocity for three positions.
Step 2
2 of 7
a)

Gymnast spins around axis that goes through its center of mass and it is parallel to the bar, because in free rotation body tends to speed around center of mass and in this case when gymnast lets go of the bar she had angular velocity that was pointing in the same direction as the bar and because there is no external torque when she is in the air the direction of the angular velocity is the same.

Step 3
3 of 7
b)

Moment of inertia can be calculated with equation:

$$
I=sum_i^nm_ir_i^2
$$

we can see from this equation that moment of inertia is larger the farther mass is from the center of rotation.

Step 4
4 of 7
Rank in order, from greatest to least, her moments of inertia for the three positions:

$$
boxed{rm first>third>second}
$$

Step 5
5 of 7
c)

To solve this we have to use conservation of angular momentum, and we know that angular momentum is given by equation:

$$
L=Iomega
$$

We can see form equation that if the angular momentum is conserved, larger the moment of inertia smaller the angular velocity.

Step 6
6 of 7
Rank in order, from greatest to least, her velocity for the three positions:

$$
boxed{rm second>third>first}
$$

Result
7 of 7
a) center of mass

b) $rm first>third>second$

c) $rm second>third>first$

Exercise 89
Step 1
1 of 9
A male dancer leaps in the air. In part $textbf{a}$ we have to calculate with what momentum does he reach the ground, in part $textbf{b}$ what impulse is needed to stop the dancer, in part $textbf{c}$ we have to find the average force in the dancers body knowing that the stopping time is 0.05 s and in part $textbf{d}$ compare the stopping time with his weight. It is also given that his mass is 60 kg and he leaps 0.32 m high.
Step 2
2 of 9
a)

To calculate momentum we have to get velocity in that moment, we can do that with equation for conservation of energy:

$$
mgh=frac{mv^2}{2}rightarrow v=sqrt{2gh}
$$

Now when we can get momentum with equation:

$$
p=mv
$$

Step 3
3 of 9
When we put the numbers in equation for velocity we get:

$$
v=sqrt{2cdot9.81cdot0.32}=2.5,,rm m/s
$$

Now we can get calculate momentum:

$$
p=60cdot2.5
$$

$$
boxed{p=150,,rm kgm/s}
$$

Step 4
4 of 9
b)

Impulse is equal to change in momentum, in this case we have that starting momentum is that momentum form part $textbf{a}$ and at the end is zero:

$$
Ft=Delta p
$$

$$
boxed{Ft=150,,rm kgm/s}
$$

Step 5
5 of 9
c)

Impulse is equal to force time time, we know from part $textbf{b}$ impulse and the time is given:

$$
F=frac{Ft}{t}
$$

Step 6
6 of 9
When we put the numbers we get that average force is:

$$
F=frac{150}{0.05}
$$

$$
boxed{F=3006,,rm N}
$$

Step 7
7 of 9
d)

Weight of the dancer can be calculated with equation:

$$
F_g=mg
$$

We can compare the stopping force with his weight by dividing them:

$$
x=frac{F}{F_g}
$$

Step 8
8 of 9
When we put number we get that weight is:

$$
F_g=60cdot9.81=589,,rm N
$$

and finally we get:

$$
x=frac{3006}{589}
$$

$$
boxed{x=5.1}
$$

The stopping force on the body is 5.1 times bigger then weight.

Result
9 of 9
a) $p=150,,rm kgm/s$

b) $Ft=150,,rm kgm/s$

c) $F=3006,,rm N$

d) $x=5.1$

Exercise 91
Step 1
1 of 3
In this problem a student is siting on a stool that can rotate without friction and she is holding a wheel with its axis vertical. Students starts to rotate the wheel with her hands. We have to answer if the student and stool would turn.
Step 2
2 of 3
To answer this question we can use conservation of angular momentum. In the starting position when student does not rotate total angular momentum is zero. When student starts to rotate the wheel, wheel gets some angular momentum and if total angular momentum has to be conserved $textbf{student and stool must rotate in the opposite direction}$ then the wheel.
Result
3 of 3
Yes, in opposite direction.
Exercise 95
Step 1
1 of 4
Ball is swung vertically in uniform circular motion. We have to calculate tension in the cord at the top of the ball’s motion. Also it is given that mass is 0.72 kg, length of a string is 0.6 m and speed is 3.3 m/s.
Step 2
2 of 4
We can calculate centripetal force with equation:

$$
F_{cp}=frac{mv^2}{r}
$$

And centripetal force in this case on the top of the ball’s motion is equal to tension plus weight:

$$
T+mg=frac{mv^2}{r}rightarrow T=frac{mv^2}{r}-mg
$$

Step 3
3 of 4
When we put the numbers in we get that tension is:

$$
T=frac{0.72cdot3.3^2}{0.6}-0.72cdot9.81
$$

$$
boxed{T=6,,rm N}
$$

Result
4 of 4
$$
T=6,,rm N
$$
Exercise 96
Step 1
1 of 4
We have to calculate the radius of the circular orbit satellite must have to have period of one day. We got hint that we could use Kepler’s third law and that the Moon is $3.9cdot10^8,,rm m$ from earth and its period is 27.33 days.
Step 2
2 of 4
the third Kepler’s law says that the square of a planet’s orbital period is proportional to the cube of the length of the semi-major axis of its orbit. Because the path of the Moon and the satellite is practically circular, the semi-major axis is equal to radius. Equation for that looks like:

$$
frac{T^2}{T_M^2}=frac{r^3}{r_M^3}rightarrow r=r_Mleft(frac{T^2}{T_M^2}right)^{frac{1}{3}}
$$

Step 3
3 of 4
When we put numbers we get:

$$
r=3.9cdot10^8cdotleft(frac{1^2}{27.33^2}right)^{frac{1}{3}}
$$

$$
boxed{r=4.3cdot10^{7},,rm m}
$$

Result
4 of 4
$$
r=4.3cdot10^{7},,rm m
$$
Exercise 97
Step 1
1 of 4
A machine pulls a rope that is wrapped around a drum. We have to calculated $alpha$, $omega$ and $I$. It is also given that diameter of the drum is 0.6 m, this means that radius is 0.3 m. Constant force is applied by the machine of 40 N in total of 2 s. And in that time rope unwound 5 m.
Step 2
2 of 4
To calculate $alpha$ we have to get linear acceleration and we can do that with equation:

$$
x=frac{1}{2}at^2rightarrow a=frac{2x}{t^2}
$$

Now when we have linear acceleration we can get angular acceleration:

$$
alpha=frac{a}{r}
$$

To calculate angular velocity we have to get linear velocity first, we can di that with equation:

$$
v=at
$$

Now it is easy to get angular velocity:

$$
omega=frac{v}{r}
$$

And finally to calculate moment of inertia we have to find torque first:

$$
tau=Fr
$$

now we can get moment of inertia:

$$
tau=Ialpharightarrow I=frac{tau}{alpha}
$$

Step 3
3 of 4
Lets calculate linear acceleration:

$$
a=frac{2cdot5}{2^2}=2.5,,rm m/s^2
$$

Angular acceleration is:

$$
alpha=frac{2.5}{0.3}
$$

$$
boxed{alpha=8.33,,rm rad/s^2}
$$

Now lets calculate linear velocity:

$$
v=2.5cdot2=5,,rm m/s
$$

Angular velocity is:

$$
omega=frac{5}{0.3}
$$

$$
boxed{omega=16.67,,rm rad/s}
$$

Lets calculate torque:

$$
tau=40cdot0.3=12,,rm N
$$

Moment of inertia is:

$$
I=frac{12}{8.33}
$$

$$
boxed{I=1.44,,rm kgm^2}
$$

Result
4 of 4
$$
alpha=8.33,,rm rad/s^2
$$

$$
omega=16.67,,rm rad/s
$$

$$
I=1.44,,rm kgm^2
$$

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