chapter 7 forces in two dimensions

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Chapter 7 Forces in Two Dimensions A 50 kg sign is supported in a motionless position supported by two ropes that make a 40º angle with the horizontal What is the Tension in each rope?

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Chapter 7 Forces in Two Dimensions. A 50 kg sign is supported in a motionless position supported by two ropes that make a 40 º angle with the horizontal What is the Tension in each rope?. F A. F B. 40 °. 40 °. F g. F B. 50 °. 490 N. 80 °. 50 °. F A. - PowerPoint PPT Presentation

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Page 1: Chapter 7 Forces in Two Dimensions

Chapter 7Forces in Two Dimensions

A 50 kg sign is supported

in a motionless position

supported by two ropes that

make a 40º angle with the

horizontal What is the

Tension in each rope?

Page 2: Chapter 7 Forces in Two Dimensions

Chapter 7Forces in Two Dimensions

Draw a free body diagram FBFA

Fg

40°40°

The force of gravity is F=maor F= (50kg)(9.8 m/s2)=490 N

Since the system is in equilibrium,the sum of the vectors is zero and by the head tail method

= 490 N

490 N50°

50°

FA

FB

80°

50sin80sin

490 AFN FA = FB = 381 N

Page 3: Chapter 7 Forces in Two Dimensions

Chapter 7Forces in Two Dimensions

Motion along inclined planesFy

Fx

Fg

By vector addition and similartriangles Fg

Fy

Fx

Page 4: Chapter 7 Forces in Two Dimensions

Chapter 7Forces in Two Dimensions

A trunk weighing 300 N

is placed on a plane and

starts to slide when inclined

at 30°.Find the parallel and

perpendicular components

of the force and the

coefficient of friction.

Fy

Fx

300 N 30

300 N

Fy

Fx

30

Page 5: Chapter 7 Forces in Two Dimensions

Chapter 7Forces in Two Dimensions

Fx=F sin 30°=300 N *.5

Fx = 150 N

300 N

Fy

Fx

30

Check (150 N)2+(260 N)2 = (300 N)2

Fy=F cos 30°=300 N *.866

Fy = 260 N

Fy

Fx

300 N 30

.577260N

150N

F

F

N

f or µ = tan ø

Page 6: Chapter 7 Forces in Two Dimensions

Chapter 7Forces in Two Dimensions

Suppose the crate is moving down the plane

and the coefficient of kinetic friction between

the surfaces is .10. How fast is the crate going

2 seconds after starting from rest?

Page 7: Chapter 7 Forces in Two Dimensions

Chapter 7Forces in Two Dimensions

y direction

FN= mg cos Ø

x direction

Fnet= Fx-kFN

Fnet= 150 N- .10(260 N) = 124 N

F = ma

a = 4.0 m/s2 vf = vi + at vf = 0 + 4.0 m/s2*2 s = 8 m/s

Fy

Fx

300 N 30

Ff

Fnet = Fx - Ff

Applet

124 = (300N/9.8 m/s2) a

Page 8: Chapter 7 Forces in Two Dimensions
Page 9: Chapter 7 Forces in Two Dimensions

Projectiles Launched Horizontally

Page 10: Chapter 7 Forces in Two Dimensions
Page 11: Chapter 7 Forces in Two Dimensions

A projectile is thrown horizontally at 20 m/sfrom the top of a cliff 490 m high.

a. How long is the object in the air?b. How far from the base of the cliff does it land?c. How fast is it moving the instant it hits the ground?

x0 = 0vx0 = 20 m/sy0 = -490 may = -9.8 m/s2

20 m/s

490 m

a. d = vit + ½ at2

solve for t

t = 29.8m/s

490m)2(

a

2d

t = 10 s

b. d = vt d = (20m/s)(10s) d = 200 m

c. vf = vi+at vf = 0 + (-9.8m/s2)(10s) vf = -98 m/s

Page 12: Chapter 7 Forces in Two Dimensions

A projectile is thrown horizontally at 5 m/sfrom the top of a cliff 19.6 m high.

a. How long is the object in the air?b. How far from the base of the cliff does it land?c. How fast is it moving the instant it hits the ground?

x0 = 0vx0 = 5 m/sy0 = -19.6 may = -9.8 m/s2

a. d = vit + ½ at2

solve for t

t = 29.8m/s

19.6m)2(

a

2d

t = 2 s

b. d = vt d = (5m/s)(2s) d = 10 m

5 m/s

19.6 m

c. vf = vi+at vf = 0 + (-9.8m/s2)(2s) vf = -19.6 m/s

Page 13: Chapter 7 Forces in Two Dimensions

Projectiles Launched at an AngleA ball is thrown with an initial velocityof 5 m/s at an angle of 60º with the horizonat ground level.

a. How long is the ball in the air?b. How high does it go?c. How far does it go?

x0=0y0 = 0v = 5 m/s = 60ºa = -9.8 m/s2

60º

60º

5m/svx = v cos Ø = 5 cos 60º= 2.5 m/svy = v sin Ø = 5 sin 60º = 4.33 m/s

vx

vy

.88s9.8m/s

(4.33m/s)4.33m/s

a

vvt a.

2if

.956m)(.44s)9.8m/s(2

1.44s)(4.33m/s)(at

2

1tvd b. 222

i

2.2mm/s)(.88s) (2.5 vt d c.

Page 14: Chapter 7 Forces in Two Dimensions

Projectiles Launched at an AngleA projectile is thrown with an initial velocityof 98 m/s at an angle of 53º with the horizonat ground level.

a. How long is the ball in the air?b. How high does it go?c. How far does it go?

x0=0y0 = 0v = 98 m/s= 53ºa = -9.8 m/s2

53º

53º

98 m/svx = v cos Ø = 98 cos 53º= 58.98 m/svy = v sin Ø = 98 sin 53º = 78.27 m/s

vx

vy

15.97s9.8m/s

(78.27m/s)78.27m/s

a

vvt a.

2if

m 312)(8s)9.8m/s(2

1s) (8(78.27m/s)at

2

1tvd b. 222

i

941.88ms)m/s)(15.97 (58.98 vt d c.

Page 15: Chapter 7 Forces in Two Dimensions

Projectiles Launched at an AngleA projectile is thrown with an initial velocityof v m/s at an angle of ø with the horizonat ground level.

a. How long is the ball in the air?b. How high does it go?c. How far does it go?

x0=0y0 = 0v = v= a = -9.8 m/s2

ø

ø

vvx = v cos Øvy = v sin Ø

vx

vy

22if

m/s9.8

2vsin

9.8m/s

m/s)(vsinm/sv

a

vvt a.

)sin(

2

22

22

i 9.8m/s-

2vsin-)9.8m/s(

2

1

9.8m/s-

2vsin-m/s)(vsinat

2

1tvd b.

2

2

2 9.8m/s

cossin2v

m/s9.8

sin2vm/s) cos(v vt d c.

Page 16: Chapter 7 Forces in Two Dimensions

Projectile Motion

Page 17: Chapter 7 Forces in Two Dimensions
Page 18: Chapter 7 Forces in Two Dimensions
Page 19: Chapter 7 Forces in Two Dimensions

What goes faster, the inside of a record or the outside?

Animation

Page 20: Chapter 7 Forces in Two Dimensions

Circular Motion

Fc

ac

Page 21: Chapter 7 Forces in Two Dimensions

As a car makes a turn, the force of friction acting upon the turned wheels of the car provide the centripetal forcerequired for circular motion.

Page 22: Chapter 7 Forces in Two Dimensions

As a bucket of water is tied to a string and spun in a circle, the force of tension acting upon the bucket provides the centripetal force required for circular motion.

Page 23: Chapter 7 Forces in Two Dimensions

As the moon orbits the Earth, the force of gravity acting upon the moon provides the centripetal force required for circular motion.

Page 24: Chapter 7 Forces in Two Dimensions

T

R2

t

dv

rr

AB

v

Δv

r

tv

v

Δv

ar

v

t

Δv 2

2

22

cc T

R4πm

R

mvmaF

Page 25: Chapter 7 Forces in Two Dimensions

A 900-kg car moving at 10 m/s takes a turn around a circle with a radius of 25.0 m. Determine the acceleration and the net force acting upon the car.

Known Information:

m = 900 kg v = 10.0 m/sR = 25.0 m

Requested Information:

a = ???? Fnet = ????

To determine the acceleration of the car, use the equation a = (v2)/R.The solution is as follows: a = (v2)/R

a = ((10.0 m/s)2)/(25.0 m)a = (100 m2/s2)/(25.0 m)

a = 4 m/s2

To determine the net force acting upon the car, use the equation F net = m*a. The solution is as follows.Fnet = m*a

Fnet = (900 kg)*(4 m/s2)

Fnet = 3600 N

Page 26: Chapter 7 Forces in Two Dimensions

Joe Brick, the new 95-kg halfback makes a turn on the football field. He sweeps out a path which is a portion of a circlewith a radius of 12-meters. The halfback makes a quarter of a turn around the circle in 2.1 seconds. Determine the speed, acceleration and net force acting on Joe.

Known Information:m = 95.0 kg R = 12.0 mTraveled 1/4-th of the circumference in 2.1 s

Requested Information:v = ???? a = ????Fnet = ????

To determine the speed of the halfback, use the equation v = d/t where the d is one-fourth of the circumference and the time is 2.1 s. The solution is as follows: v = d/t v = (0.25 * 2 π * R)/t v = (0.25 * 2 * 3.14 * 12.0 m)/(2.1 s) v = 8.97 m/s

Page 27: Chapter 7 Forces in Two Dimensions

To determine the acceleration of the halfback, use the equation a = (v2)/R. The solution is as follows:•a = (v2)/R •a = ((8.97 m/s)2)/(12.0 m)

•a = (80.5 m2/s2)/(12.0 m)

•a = 6.71 m/s2

To determine the net force acting upon the halfback, use the equation Fnet = m*a. The solution is as follows.•Fnet = m*a

•Fnet = (95.0 kg)*(6.71 m/s2)

•Fnet = 637 N

Page 28: Chapter 7 Forces in Two Dimensions

Simple Harmonic Motion Definitions

•Period (s) The time required to complete one cycle.•Frequency (hz) The number of cycles per second. •Amplitude (m) The point of maximum displacement from rest.

Page 29: Chapter 7 Forces in Two Dimensions

AB

CD

E

+-

Simple Harmonic Motion

A

B

C

D

E

D

C

B

A

Time (sec)

+

- Dis

tan

ce

(mete

rs)

Page 30: Chapter 7 Forces in Two Dimensions

AB

CD

E

+-Simple Harmonic Motion

Time (sec)

+

- Velo

city

(m

/s)

B

D

ED

C

A

B

C

A

Page 31: Chapter 7 Forces in Two Dimensions

AB

CD

E

+-Simple Harmonic Motion

Time (sec)

+

- Acc

ele

rati

on

(m

/s

2)

A

B

D

ED

C

A

B

C

Page 32: Chapter 7 Forces in Two Dimensions

Simple Harmonic Motion