forces & newton’s laws of motion chapter 4 (angles)

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Forces & Newton’s Laws of Motion Chapter 4 (angles)

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Page 1: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Forces & Newton’s Laws of Motion

Chapter 4(angles)

Page 2: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Sign Problems

Equilibrium-the state where all forces are balanced and acceleration is zero.

Includes both stationary and constant velocity cases.

Page 3: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #15 If the sign has a mass of

15kg, what is the tension in the string? What is the force the beam exerts on the sign?

Assume equilibrium. One component at a time.

Page 4: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Set up equilibrium case

0

0

vertical

horizontal

F

F

cos

sin

Tx

Ty

FF

FF

Fy

Fx

FT

23

Fg

Fbeam

Page 5: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Equilibrium case for vertical

0sin mgFT

0 gy FF

Nmg

FT 2.376sin

0verticalF

Page 6: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Equilibrium case for horizontal

0horizontalF

0 Beamx FF

0cos BeamT FF

BeamT FF cos

N3.34623cos2.376

Page 7: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #16 Find the tension in

each rope.

T1T2

Page 8: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Break up Components

111 sinFFy

222 sinFFy

111 cosFFx

222 cosFFx

F1 F2

Fx1 Fx2

Fy1 Fy2

Fg

Page 9: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Horizontal Pieces

Since the sign isn’t accelerating horizontally, we can use: 021 xx FF

0coscos 2211 FF

2211 coscos FF

0 xF

Fx1 Fx2

Fy1 Fy2

Fg

Page 10: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Vertical Pieces

Since the sign isn’t accelerating vertically, we can use: 021 gyy FFF

0sinsin 2211 mgFF

0 F

Fx1 Fx2

Fy1 Fy2

Fg

Page 11: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Putting the two together

0sinsincos

cos221

1

22

mgF

F

0sinsin 2211 mgFF 2211 coscos FF

1

221 cos

cos

F

F

Page 12: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Putting the two together cont.

mgFF

221

1

22 sinsincos

cos

mgF

21

1

22 sinsin

cos

cos

211

2

2

sinsincoscos

mgF

Page 13: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Putting the two together cont.

NF 383

62sin34sin34cos62cos

8.9472

NF

F 6.214cos

cos

1

221

Page 14: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #17

What is the tension in the cables that support the sign?

Physics is

Phun!!

m = 1500 kg

40°

Page 15: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #18 – Angles with accelerationA sled of mass 30 kg is pulled with a force of 50 N at a 25 degree angle. IF the coefficient of friction between the runners and the snow is 0.1, what is the acceleration of the sled?

Page 16: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #19

A 50 kg boy is pushed on a 20 kg scooter with a force shown below at 20 degrees below the horizontal. What is the coefficient of friction that would keep the scooter from accelerating? FA=200 N

Page 17: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #20

A 50 kg girl is pushed on a 20 kg scooter with a force shown below at 20-degrees below the horizontal. What is the coefficient of friction that would keep the scooter accelerating at 1.5 m/sec2?

FA=200 N

Page 18: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #21 – Ramp Problem

A crate slides down a 37 degree incline. What is the acceleration of the crate?

Page 19: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #22

A crate slides down a 35 degree incline. What is the acceleration of the crate if the coefficient of friction between the crate and the incline is 0.2?

Page 20: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #23

A skier is accelerating down a mountain that has a 30-degree incline at 4.0 m/sec2.

A) What is the coefficient of friction?

B) How long does it take him to get to the bottom of the 0.5 km long mountain?

C) How fast is he going by the time he reaches the bottom of the mountain assuming that he goes straight down without turns?

Page 21: Forces & Newton’s Laws of Motion Chapter 4 (angles)

Example #24

A crate is sliding down an incline at constant speed. If the coefficient of friction is 0.45, at what angle is the incline?

Page 22: Forces & Newton’s Laws of Motion Chapter 4 (angles)

What must be for the second incline?