Newton’s first law. Newton’s second law. Particular forces:

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I. I. Newton’s first law. Newton’s first law. II. II. Newton’s second law. Newton’s second law. III. III. Particular forces: Particular forces: - Gravitational - Gravitational - - Weight Weight - - Normal Normal - Tension - Tension IV. Newton’s third law. IV. Newton’s third law. Chapter 5 – Force and Chapter 5 – Force and Motion I Motion I

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Chapter 5 – Force and Motion I. Newton’s first law. Newton’s second law. Particular forces: - Gravitational - Weight - Normal - Tension IV. Newton’s third law. - PowerPoint PPT Presentation

Transcript of Newton’s first law. Newton’s second law. Particular forces:

Page 1: Newton’s first law. Newton’s second law. Particular forces:

I.I. Newton’s first law.Newton’s first law.

II.II. Newton’s second law.Newton’s second law.

III.III. Particular forces:Particular forces: - Gravitational- Gravitational

- Weight- Weight - Normal- Normal

- Tension- Tension

IV. Newton’s third law.IV. Newton’s third law.

Chapter 5 – Force and Motion IChapter 5 – Force and Motion I

Page 2: Newton’s first law. Newton’s second law. Particular forces:

In the figure below, mIn the figure below, mblockblock=8.5kg and =8.5kg and θθ=30º. Find (a) Tension in =30º. Find (a) Tension in

the cord. (b) Normal force acting on the block. (c) If the cord is cut, the cord. (b) Normal force acting on the block. (c) If the cord is cut, find the find the magnitude of the block’s acceleration.magnitude of the block’s acceleration.

TN

Fg

y

x

2/9.45.865.410)( smaaNmaFTc gx

NsmkgmgFaa gx 65.415.0)/8.9)(5.8(30sin0)( 2

NmgFNb gy 14.7230sincos)(

Page 3: Newton’s first law. Newton’s second law. Particular forces:

Chapter 6 – Force and Motion IIChapter 6 – Force and Motion II

I.I. Frictional forces.Frictional forces.

II.II. Drag forces and terminal speed.Drag forces and terminal speed.

III.III. Uniform circular motion.Uniform circular motion.

Page 4: Newton’s first law. Newton’s second law. Particular forces:

I. Frictional forceFrictional force

-Kinetic: Kinetic: (f(fkk)) appears after a large enough external force is appears after a large enough external force is

applied and the body loses its intimate contact with applied and the body loses its intimate contact with the surface, sliding along it.the surface, sliding along it.

No motion

Acceleration

Constant velocity

Counter force that appears when an external force tends to slide a body Counter force that appears when an external force tends to slide a body along a surface. It is along a surface. It is directeddirected parallel parallel to the to the surface surface and and oppositeopposite to the to the sliding motionsliding motion..

FF

(applied(applied force)force)

//Ffs

-Static: Static: (f(fss) compensates the applied force, the body does ) compensates the applied force, the body does

not move.not move.

Page 5: Newton’s first law. Newton’s second law. Particular forces:

max,sk ff Nf ss max,

Nf kk

Friction coefficientsFriction coefficientsslidesbodyfFIf s max,//

After the body starts sliding, fAfter the body starts sliding, fkk decreases decreases.

II. Drag force and terminal speedII. Drag force and terminal speed

-Fluid: anything that can flow. Example: gas, liquid.

-Drag force: DDrag force: D

- Appears when there is a relative velocity between a fluid and - Appears when there is a relative velocity between a fluid and a body.a body.- - OpposesOpposes the relative motion of a body in a fluid. the relative motion of a body in a fluid.

- Points in the direction in which the fluid flows.- Points in the direction in which the fluid flows.

Page 6: Newton’s first law. Newton’s second law. Particular forces:

2

2

1AvCD

AC

Fv gt

2

-Terminal speed: vTerminal speed: vtt

02

10 2 gg FAvCaifmaFD

AssumptionsAssumptions:: * Fluid = air.* Fluid = air. * Body is baseball.* Body is baseball. * Fast relative motion * Fast relative motion turbulent air. turbulent air.

C = drag coefficient (0.4-1).C = drag coefficient (0.4-1).ρρ = air density (mass/volume). = air density (mass/volume). A= effective body’s cross sectional area A= effective body’s cross sectional area area perpendicular to v area perpendicular to v

- Reached when the acceleration of an object that experiences a - Reached when the acceleration of an object that experiences a vertical movement through the air becomes zero vertical movement through the air becomes zero F Fgg=D=D

Page 7: Newton’s first law. Newton’s second law. Particular forces:

III. Uniform circular motionIII. Uniform circular motion

-Centripetal acceleration:Centripetal acceleration:

R

vmF

2

r

va

2

A centripetal force accelerates a body by changing the direction of the A centripetal force accelerates a body by changing the direction of the body’s velocity without changing its speed.body’s velocity without changing its speed.

v, a are constant, but direction changes during motionv, a are constant, but direction changes during motion.

-Centripetal force:Centripetal force:

a, F are directed toward the center of curvaturea, F are directed toward the center of curvatureof the particle’s path.of the particle’s path.

Page 8: Newton’s first law. Newton’s second law. Particular forces:

A puck of mass m slides on a frictionless table while attached to a hanging cylinder of mass M by a cord

through a hole in the table. What speed keeps the cylinder at rest?

Mg

mg T

TN

MgTMFor

m

Mgrv

r

vmMg

r

vmTmFor

22

Page 9: Newton’s first law. Newton’s second law. Particular forces:

Calculate the drag force on a missile 53cm in diameter cruising with a speed of 250m/s at low altitude, where the density of air is 1.2kg/m3. Assume C=0.75

kNsmmmkgAvCD 2.6/250)2/53.0()/2.1(75.05.02

1 2232

The terminal speed of a ski diver is 160 km/h in the spread eagle position and 310 km/h in the nose- dive position. Assuming that the diver’s drag coefficient C does not change from one point to another, find the ratio of the effective cross sectional area A in the slower position to that of the faster position.

Page 10: Newton’s first law. Newton’s second law. Particular forces:

The terminal speed of a ski diver is 160 km/h in the spread eagle position and 310 km/h in the nose-

dive position. Assuming that the diver’s drag coefficient C does not change from one point to

another, find the ratio of the effective cross sectional area A in the slower position to that of the

faster position.

7.32

2

/310

/1602

D

E

E

D

D

g

E

g

gt A

A

A

A

AC

F

AC

F

hkm

hkm

AC

Fv

Page 11: Newton’s first law. Newton’s second law. Particular forces:

Two blocks of weights 3.6N and 7.2N, are connected by a massless string and slide down a 30º inclined plane. The coefficient of kinetic friction between the lighter block and the plane is 0.10; that between the heavier block and the plane is 0.20. Assuming that the lighter block leads, find (a) the magnitude of the acceleration of the blocks and (b) the tension in the string.

A

B

FgA

FgB

NA

NB

T

T

fk,B

fk,A

MovementBlock A Block BNA NB

fkAfkB

TFgxA

FgyA

FgxB

FgyB

T

Light block A leads

Page 12: Newton’s first law. Newton’s second law. Particular forces:

Light block A leadsLight block A leads

NT

sma

2.0

/49.3 2

Page 13: Newton’s first law. Newton’s second law. Particular forces:

Block B weighs 711N. The coefficient of static friction between the block and the table is 0.25; assume that the cord between B and the knot is horizontal. Find the maximum weight of block A for which the system will be stationary.

FgA

N

FgB

T1

f

T3

T1

T2

T3

NfstationarySystem ss max,

NNTfT

gmNBBlock

s

B

75.17771125.00 1max,1

322

2221

30sin

25.20530cos

75.17730cos

TTT

NN

TTTTKnot

y

x

NNTgmTABlock A 62.10225.2055.030sin23

Page 14: Newton’s first law. Newton’s second law. Particular forces:

NNNf

NNNf

kk

ss

8.22)60(38.0

33)60(55.0max,

A block weighing 22N is held against a vertical wall by a horizontal force F of magnitude 60N. The coefficient of static friction between the wall and the block is 0.55 and the coefficient of kinetic friction between them is 0.38. A second force P acting parallel to the wall is applied to the block. For the following magnitudes and

directions of P, determine whether the block moves, the direction of motion, and

the magnitude and direction of the frictional force acting on the block: (a) 34N up, (b) 12N up, (c) 48N up, (d) 62N up, (e) 10N down, (f) 18N down.

F=60N

(a) P=34N, up

mg=22N

N

N=F=60N

P

22Nf

Without P, the block is at rest Without P, the block is at rest

movenotdoesBlockNff

downNffNN

affassumeweIf

mafmgP

s

s

33

122234

0

max,

P

Page 15: Newton’s first law. Newton’s second law. Particular forces:

74. A block weighing 22N is held against a vertical wall by a horizontal force F of magnitude 60N. The coefficient of static friction between the wall and the block is 0.55 and the coefficient of kinetic friction between them is 0.38. A second P acting parallel to the wall is applied to the block. For the following magnitudes and directions of P, determine whether the block moves, the direction of motion, and the magnitude and direction of the frictional force acting on the block: (a) 34N up (b) 12N up, (c) 48N up, (d) 62N up, (e) 10N down, (f) 18N down.

F=60N

(a) P=34N, up

mg=22N

N

N=F=60N

P

(b) P=12N, up

P

22N

f

movingNotNff

upNNNf

mamgfP

s

33

102212

0

max,

(c) P=48N, up

P

22Nf

movingNotNff

downNNNf

mamgfP

s

33

262248

0

max,

(d) P=62N, up P

22Nf

downNffwithmamgfP

wrongAssumptionupmovesBlockNff

upNNNfmgfP

k

s

8.22

(*)33

402262(*)0

max,

Page 16: Newton’s first law. Newton’s second law. Particular forces:

(e) P=10N, down

P

22N

f

movingNotNff

upNNNf

mamgPf

s

33

321222

0

max,

(f) P=18N, down

P22N

f

upNff

movesNff

upNNNf

mamgPf

k

s

8.22

33

402218

0

max,

WA=44N

Page 17: Newton’s first law. Newton’s second law. Particular forces:

P

Blocks A and B have weights of 44N and 22N, respectively. (a) Determine the minimum weight of block C to keep A from sliding if μs between A and the table is 0.2. (b) Block C suddenly is lifted of A. What is the acceleration of block A if μk between A and the table is 0.15?

T

T

WB=22N

WA=44N

f

Wc

N

)1(00 max,

max,

NTfTaABlock

Nff

ss

ss

)2(220 NTmgTBBlock

NNT

Ns

1102.0

22)2()1(

NNNWWWNBABlocks CCA 6644110,

(a)

Page 18: Newton’s first law. Newton’s second law. Particular forces:

P

Blocks A and B have weights of 44N and 22N, respectively. (a) Determine the minimum weight of block C to keep A from sliding if μs between A and the table is 0.2. (b) Block C suddenly is lifted of A. What is the acceleration of block A if μk between A and the table is 0.15?

T

T

WB=22N

WA=44N

f

Wc

N

amgmT

amNT

NgmNdisappearsC

BB

Ak

A

44

(b)

NTaT

smaaT

172.222

/3.25.46.6 2

Page 19: Newton’s first law. Newton’s second law. Particular forces:

The two blocks (with m=16kg and m=88kg) shown in the figure below are not attached. The coefficient of static friction between the blocks is: μs=0.38 but the surface beneath the larger block is frictionless.

What is the minimum value of the horizontal force F required to keep the smaller block from slipping

down the larger block?

Mm

FaamF total

)2(0'0

)1('

mgFmgf

Mm

FmmaFFblockSmall

ss

NM

MmmgFmg

Mm

Fm

ss 488)2()1(

Mg

N

F’

mg

fF’

Movement

FFminmin required to keep m from sliding down? required to keep m from sliding down?

Treat both blocks as a single system sliding across a frictionless floor

Page 20: Newton’s first law. Newton’s second law. Particular forces:

mg

An amusement park ride consists of a car moving in a vertical circle on the end of a rigid boom of negligible mass. The combined weigh of the car and riders is 5kN, and the radius of the circle is 10m.

What are the magnitude and the direction of the force of the boom on the car at the top of the circle if the car’s speed is (a) 5m/s (b) 12m/s?

Rg

vWF

R

vmWF BB

22

1

The force of the boom on the car is capable of pointing any direction

FB

W

y

downFsmvbupNFsmva BB 3.2/12)(7.3/5)(