Solving Impulse and Momentum Problems, Lecture notes of Physics

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Textbook: Physics for Scientists and Engineers 3rd Edition by Randall Knight
STEM Success Center
Physic 201
Worksheet
Phys 201: Chapter 9 Impulse and Momentum
Before we begin the problems, it helps to list your knownโ€™s and unknowns/what we are solving for. This
helps with organization by identifying the what the problem is asking for. Also, red represents the
solution.
Section 9.2: Solving Impulse and Momentum Problems
12) A 250 g ball collides with a wall. The figure below shows the ballโ€™s velocity and the force exerted on
the ball by the wall. What is ๐‘ฃ๐‘“๐‘ฅ, the ballโ€™s rebound velocity?
Known:
๐‘š๐‘=250๐‘˜๐‘”=0.25๐‘˜๐‘”
๐‘ฃ๐’Š๐’™ =โˆ’10๐‘š
๐‘ 
๐น๐‘ฅ=500๐‘ ๐‘“๐‘œ๐‘Ÿ ๐‘ก=8๐‘š๐‘ 
Find:
๐‘ฃ๐‘“๐‘ฅ =?
Given that a force is being applied to an object during a time interval, then find the impulse ( ๐‘ฑ๐’™).
๐ฝ๐‘ฅ=โˆซ ใ€–๐น๐‘ฅ๐‘‘๐‘ก=500โˆซ๐‘‘๐‘ก
8๐‘š๐‘ 
0๐‘  =500[๐‘ก๐‘“โˆ’ใ€—๐‘ก๐‘–]
๐‘ก๐‘“
๐‘ก๐‘–=500 [0.008๐‘š๐‘ โˆ’0๐‘ ]=4๐‘โˆ™๐‘ 
Now, use the impulse-momentum theorem (โˆ†๐‘ƒ๐‘ฅ=๐ฝ๐‘ฅ) to solve for the final velocity.
โˆ†๐‘ƒ๐‘ฅ=๐ฝ๐‘ฅ
๐‘ƒ๐‘“๐‘ฅ โˆ’๐‘ƒ๐‘–๐‘ฅ =๐ฝ๐‘ฅ
๐‘š๐‘๐‘ฃ๐‘“๐‘ฅโˆ’๐‘š๐‘๐‘ฃ๐‘–๐‘ฅ =๐ฝ๐‘ฅ
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Textbook: Physics for Scientists and Engineers 3 Edition by Randall Knight

STEM Success Center

Physic 201

Phys 201: Chapter 9 Impulse and Momentum

Before we begin the problems, it helps to list your knownโ€™s and unknowns/what we are solving for. This

helps with organization by identifying the what the problem is asking for. Also, red represents the

solution.

Section 9.2: Solving Impulse and Momentum Problems

12) A 250 g ball collides with a wall. The figure below shows the ballโ€™s velocity and the force exerted on

the ball by the wall. What is ๐‘ฃ

๐‘“๐‘ฅ

, the ballโ€™s rebound velocity?

Known:

๐‘

๐’Š๐’™

๐‘ฅ

Find:

๐‘“๐‘ฅ

Given that a force is being applied to an object during a time interval, then find the impulse ( ๐‘ฑ ๐’™

๐‘ฅ

๐‘ฅ

8 ๐‘š๐‘ 

0 ๐‘ 

[

๐‘“

๐‘–

]

๐‘ก

๐‘“

๐‘ก

๐‘–

= 500 [ 0. 008 ๐‘š๐‘  โˆ’ 0 ๐‘ ] = 4 ๐‘ โˆ™ ๐‘ 

Now, use the impulse-momentum theorem (โˆ†๐‘ƒ ๐‘ฅ

๐‘ฅ

) to solve for the final velocity.

๐‘ฅ

๐‘ฅ

๐‘“๐‘ฅ

๐‘–๐‘ฅ

๐‘ฅ

๐‘

๐‘“๐‘ฅ

๐‘

๐‘–๐‘ฅ

๐‘ฅ

Textbook: Physics for Scientists and Engineers 3 Edition by Randall Knight

STEM Success Center

Physic 201

๐‘

๐‘“๐‘ฅ

๐‘ฅ

๐‘

๐‘–๐‘ฅ

๐‘“๐‘ฅ

๐‘ฅ

๐‘

๐‘–๐‘ฅ

๐‘“๐‘ฅ

Section 9.3: Conservation of Momentum

16) A 10-m-long glider with a mass of 680 kg (including the passengers) is gliding horizontally through the

air at 30 m/s when a 60 kg skydiver drops out by releasing his grip on the glider. What is the gliderโ€™s

velocity just after the skydiver lets go?

Known:

๐‘†

= 60 ๐‘˜๐‘” (mass of skydiver)

๐บ+๐‘†

= 680 ๐‘˜๐‘” (mass of glider plus the mass of skydiver)

๐บ

๐บ+๐‘†

๐‘†

= 680 ๐‘˜๐‘” โˆ’ 60 ๐‘˜๐‘” = 620 ๐‘˜๐‘” (mass of glider)

๐บ

๐‘–

๐‘†

Note: turns out as the skydiver releases, the skydiverโ€™s final velocity will be the same as gliderโ€™s initial

velocity thus,

๐‘†

๐‘“

๐บ

๐‘–

Find:

๐บ ๐‘“

Using the Law of Conservation of Momentum equation (๐‘ท

๐’‡

๐’Š

๐บ

๐บ

๐‘“

๐‘†

๐‘†

๐‘“

๐บ+๐‘†

๐บ

๐‘–

Substitute ๐‘ฃ

๐บ

๐‘–

for ๐‘ฃ

๐‘†

๐‘–

given that ๐‘ฃ

๐‘†

๐‘–

๐บ

๐‘–

, then solve for the gliders final velocity

๐บ

๐บ

๐‘“

๐‘†

๐บ

๐‘–

๐บ+๐‘†

๐บ

๐‘–

Textbook: Physics for Scientists and Engineers 3 Edition by Randall Knight

STEM Success Center

Physic 201

To check your answer, see if the momentum of the clay is same as the momentum of the car.

Section 9.6: Momentum in Two Dimensions

25) A 20 g ball of clay traveling east at 3.0 m/s collides with a 30 g ball of clay traveling north at 2.0 m/s.

What are the speed and the direction of the resulting 50 g ball of clay?

Known:

1

๐‘–๐‘ฅ

1

2

๐‘–๐‘ฆ

2

Find:

๐‘“

Use the Law of Conservation of Momentum (๐‘ท ๐’‡

๐’Š

) to solve for the clayโ€™s velocity

๐‘“

๐‘–

Textbook: Physics for Scientists and Engineers 3 Edition by Randall Knight

STEM Success Center

Physic 201

X-direction: ๐‘š

1

๐‘–๐‘ฅ

1

2

๐‘–๐‘ฅ

2

1

2

๐‘“๐‘ฅ

Rewrite ๐‘ฃ

๐‘“๐‘ฅ

in terms of ๐‘ฃ

๐‘“

using trigonometry.

cos(๐œƒ) =

๐‘“๐‘ฅ

๐‘“

๐‘“๐‘ฅ

๐‘“

cos(๐œƒ)

1

๐‘–๐‘ฅ

1

2

๐‘–๐‘ฅ

2

1

2

๐‘“

cos(๐œƒ)

๐‘“

cos(๐œƒ) =

1

๐‘–๐‘ฅ

1

2

๐‘–๐‘ฅ

2

1

2

๐‘“

cos(๐œƒ) = 1. 2

Y-direction: ๐‘š

1

๐‘–๐‘ฆ

1

2

๐‘–๐‘ฆ

2

1

2

๐‘“๐‘ฆ

Rewrite ๐‘ฃ

๐‘“๐‘ฆ

in terms of ๐‘ฃ

๐‘“

using trigonometry.

sin

๐‘“๐‘ฆ

๐‘“

๐‘“๐‘ฆ

๐‘“

sin

1

๐‘–๐‘ฆ

1

2

๐‘–๐‘ฆ

2

1

2

๐‘“

sin(๐œƒ)

๐‘“

sin(๐œƒ) =

1

๐‘–๐‘ฆ

1

2

๐‘–๐‘ฆ

2

1

2

๐‘“

sin(๐œƒ) = 1. 2

Use the Pythagorean theorem ( ๐’„

๐Ÿ

๐Ÿ

๐Ÿ

) to find ๐‘ฃ

๐‘“

, thus

๐‘“

2

๐‘“๐‘ฅ

2

๐‘“๐‘ฆ

2

Substitute ๐‘ฃ

๐‘“๐‘ฅ

and ๐‘ฃ

๐‘“๐‘ฆ

(which was found above):

๐‘“

๐‘“๐‘ฆ

๐‘“๐‘ฅ