Chapter 4

65
Chapter 4 Motion With a Changing Velocity

description

Chapter 4. Motion With a Changing Velocity. P2.27: Find the magnitude and direction of the vector with the following components: x = -5.0 cm, y = +8.0 cm F x = +120 N, F y = -60.0 N v x = -13.7 m/s, v y = -8.8 m/s a x = 2.3 m/s 2 , a y = 6.5 cm/s 2. - PowerPoint PPT Presentation

Transcript of Chapter 4

Page 1: Chapter 4

Chapter 4

Motion With a Changing Velocity

Page 2: Chapter 4

P2.27: Find the magnitude and direction of the vector with the following components:

(a) x = -5.0 cm, y = +8.0 cm

(b) Fx = +120 N, Fy = -60.0 N

(c) vx = -13.7 m/s, vy = -8.8 m/s

(d) ax = 2.3 m/s2, ay = 6.5 cm/s2

Page 3: Chapter 4

P2.56: A 3.0 kg block is at rest on a horizontal floor. If you push horizontally on the block with a force of 12.0 N, it just starts to move.

(a) What is the coefficient of static friction?

(b) A 7.0-kg block is stacked on top of the 3.0-kg block. What is the magnitude F of the force acting horizontally on the 3.0-kg block as before, that is required to make the two blocks start to move?

Page 4: Chapter 4

P3.47: A 2010-kg elevator moves with an upward acceleration of 1.50 m/s2. What is the tension that supports the elevator?

P3.48: A 2010-kg elevator moves with a downward acceleration of 1.50 m/s2. What is the tension that supports the elevator?

Page 5: Chapter 4

Kinematic Equations for Const. Acceleration

Fnet = ma.

If Fnet is const, a will also be const.

Uniformly accelerated motion: a = const.

Page 6: Chapter 4

A car moves at a constant acceleration of magnitude 5 m/s2. At time t = 0, the magnitude of its velocity is 8 m/s. What is the magnitude of its velocity at

(i) t = 2s? (ii) t = 4s? (iii) t = 10s?

A car moves at a constant acceleration of magnitude 5.7 m/s2. At time t = 0, the magnitude of its velocity is 18.3 m/s. What is the magnitude of its velocity at

t = 2.2s?

Page 7: Chapter 4

Kinematic Equations for Const. Acceleration

Consider an object on which a net force Fnet acts on it. Thus it moves with an acceleration.As the object moves, its velocity changes.

Fnet

a

Fnet

aTime = 0

Initial position = x0

Initial velocity = v0

Time = t

Final position = x

Final velocity = v

Fnet

Page 8: Chapter 4

Kinematic Equations for Const. Acceleration

• aave = ainst

• Let us use initial time, t1 = 0.

•Final time, t2 = t, hence t = t – 0 = t

• Position: initial, x1 = x0, final, x2 = x

• Velocity, initial v1 = v0, final, v2 = v

Fnet = ma.

If Fnet is const, a will also be const.

Uniformly accelerated motion:

a = const.

Page 9: Chapter 4

Kinematic Equations for Constant Acceleration

v = v0 + atx = x0 +vot + ½ at2

v2 = v02 + 2a(x-x0)

Average velocity vav = (v0 + v)/2

Uniformly accelerated motion: a = constant.

Time: Initial = 0, final = tPositions: Initial = x0, final = x Velocity: Initial = v0, final = v

Page 10: Chapter 4

Example Problem 4.14 A train traveling at a constant speed of

22 m/s, comes to an incline with a constant slope. While going up the incline the train slows down with a constant acceleration of magnitude 1.4 m/s2.

(a)Draw a graph of vx versus t.

(b)What is the speed of the train after 8.0s on the incline?

(c) How far has the train traveled up the incline after 8.0 s?

Page 11: Chapter 4

A car moving south slows down with at a constant acceleration of 3.0 m/s2. At t = 0, its velocity is 26 m/s. What is its velocity at t = 3 s?

A. B. C. D. E.

0% 0% 0%0%0%

A. 35 m/s south

B. 17 m/s south

C. 23 m/s south

D. 29 m/s south

E. 17 m/s north

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Page 12: Chapter 4

A car initially traveling at 18.6 m/s begins to slow down with a uniform acceleration of 3.00 m/s2. How long will it take to come to a stop?

A. B. C. D. E.

0% 0% 0%0%0%

A. 55.8 s

B. 15.6 s

C. 6.20 s

D. 221.6 s

E. None of these

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Page 13: Chapter 4

Free Fall

• Free fall: Only force of gravity acting on an object making it fall.

• Effect of air resistance is assumed negligible.

• Force of gravity acting on an object near the surface of the earth is F = W = mg.

• Acceleration of any object in free fall:

a = g = 9.8 m/s2 down (ay = -9.8 m/s2).

Page 14: Chapter 4

Free Fall

+y

+x

ay = -9.8 m/s2

ax = 0

Page 15: Chapter 4

Free Fall contd…

1. a = g, regardless of mass of object.

Page 16: Chapter 4

2. a = g, regardless of initial velocity

+y

+x

ay = -9.8 m/s2, ax = 0

v0 = 0 v0 = -15 m/s v0 = +15 m/s

Page 17: Chapter 4

3. Free Fall: Motion is symmetric.

+y

+x

ay = -9.8 m/s2, ax = 0

v0 = +5 m/s

At the maximum height:

• vy = 0

• Speed at equal heights will be equal.

• Equal time going up and down.

Page 18: Chapter 4

Example: Problem 4.32

A stone is launched straight up by a slingshot. Its initial speed is 19.6 m/s and the stone is 1.5 m above the ground when launched.

(a) How high above the ground does the stone rise?

(b) How much time elapses before the

stone hits the ground?

Page 19: Chapter 4

APPARENT WEIGHT

A physics student whose mass is 40 kg stands inside an elevator on a scale that reads his weight in Newtons.

Scale Reading = Normal force the scale

exerts on the student.Scale Reading = N

= mg

= 40 x 9.8 N

= 392 N

N

mg

Page 20: Chapter 4

1. Elevator at rest. What will be the scale reading?

Fnet = N – W = may

At rest means ay = 0.

Hence N = W, ie apparent weight = true weight = 40 x 9.8 = 392 N

N

W = mg

Page 21: Chapter 4

2. Elevator accelerating upwards with ay = 2.0 m/s2. What will be the scale reading?

Page 22: Chapter 4

2. Elevator accelerating upwards with ay = 2.0 m/s2. What will be the scale reading?

Fnet = N – W = may

ay = + 2.0 m/s2 (positive because acceleration is upwards) . Hence,

N –W = N – mg = may.

N = mg + may = m(g+ay) = 40(9.8 + 2.0) = 472 N

ie, apparent weight is greater than the true weight.

N

W = mg

a

Page 23: Chapter 4

3. Elevator accelerating downwards with ay = 2.0 m/s2. What will be the scale reading?

Page 24: Chapter 4

3. Elevator accelerating downwards with ay = 2.0 m/s2. What will be the scale reading?

Fnet = N – W = may

ay = - 2.0 m/s2 (negative because acceleration is downwards) .

Hence N –W = N – mg = -may.

N = mg - may = m(g - ay) = 40(9.8 - 2.0) = 312 N

ie, apparent weight is less than the true weight.

N

W = mg

a

Page 25: Chapter 4

A 112.0-kg person stands on a scale inside an elevator moving downward with an acceleration of 1.80 m/s2. What will be the scale reading?

A. B. C. D. E.

12%7%

0%0%

81%A. 1299 N

B. 1,098 N

C. 896 N

D. 112 N

E. 0 N

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Page 26: Chapter 4

A ball is kicked straight up from ground level with initial velocity of 22.6 m/s. How high above the ground will the ball rise?

A. B. C. D. E.

5% 3%8%

73%

13%

A. 9.8 m

B. 3.00 m

C. 1.15 m

D. 26.1 m

E. 19.6 m

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Page 27: Chapter 4

WEIGHTLESSNESS

If the elevator was going down with an acceleration ay = g = -9.8m/s2, then

N = m(g-g) = 0

ie, apparent weight = 0

This is “weightlessness” or “zero gravity”

Apparent weight of an object in free fall is zero while its true weight remains unchanged.

Page 28: Chapter 4

Equilibrium

Newton’s 2nd Law: Fnet = ma

For an object in equilibrium: Fnet = 0

Static (v = 0) 0r dynamic (v = constant) eqlbm.

2-dimensions, separate the x and y components and treat the problem as two 1-dim problems.

Fx = max

Fy = may

For equilibrium, Fx = max = 0 and Fy = may = 0

Page 29: Chapter 4

2-Dimensions

• X and Y are INDEPENDENT!

• Break 2-D problem into two 1-D problems.

y

x

Page 30: Chapter 4

EquilibriumDetermine the tension in the 6 m rope if it sags 0.12 m in the center when a gymnast with weight 250 N is standing on it.

x direction: Fx = max = 0

-TL cos + TR cos = 0

TL = TR

3 m.12 my direction: Fy = may = 0

TL sin + TR sin - W = 0

2 T sinWT = W/(2 sin

y

x

312.0

tan 3.2

TL

TR

WTR

Page 31: Chapter 4

Equilibrium on a Horizontal Plane

Object at rest or moving with const. velocityFx = max = 0 and Fy = may = 0

No motion until F = > fsmax

Fx = F - fs = 0 or F = fs.

Fy = N - W = 0 or N = W

Fx = F - fk = 0 or F = fk

Fy = N - W = 0 or N = W

Ffs

W

N

Ffk

W

NSliding with constant velocityObject at rest

Page 32: Chapter 4

Equilibrium on an inclined PlaneAn object at rest on an inclined planeFx = max = 0 and Fy = may = 0

f sN

W

xy

f s

N

W

xy

Wx

W y

W

W.sin

W.cos

f sN xy

W.cosW.sin

Page 33: Chapter 4

Equilibrium on an inclined PlaneAn object at rest on an inclined planeFx = max = 0 and Fy = may = 0

f sN xy

W.cosW.sin

Fy = may = 0N - Wcos = 0 or N = Wcos

Fx = max = 0

fs - Wsin = 0 or fs = Wsin

If angle is increased, the object will eventually slide

down the plane. Sliding will start beyond angle max

At max: fsmax = W.sinmax. But fsmax = sN = s(Wcosmax)

Therefore, sWcosmax = Wsin max

OR s = (Wsinmax)/ Wcosmax ie, s = tanmax

Page 34: Chapter 4

Equilibrium on an inclined Plane

f sN xy

W.cosW.sin

N = Wcos

fs = Wsin

• If angle is increased, the object will eventually slide down the plane.• Sliding will start beyond angle max • At max: fsmax = W.sinmax.

• But fsmax = sN = s(Wcosmax)• Therefore, sWcosmax = Wsin max

• OR s = (Wsinmax)/ Wcosmax ie, s = tanmax

An object at rest on an inclined plane

Page 35: Chapter 4

f k

x

FN

y

W.sin

W.cos

A mass m being pulled uphill by a force F

If m = 510 kg, s= 0.42, k =

0.33, = 15o:(a)Find minimum force F

needed to start the mass moving up.

(b)If the force in (a) is maintained on the mass, what will its acceleration be?

(c) To move the mass with constant speed, what must the value of F be?

Page 36: Chapter 4

A block is at rest on a flat board. The flat board is gently tilted. At what angle will the block start to slide? Assume the coefficient of static friction (s) between the block and the board is 0.48.

A. B. C. D. E.

2% 0% 2%

95%

0%

A. 0.48o

B. 61.3o

C. 28.7o

D. 25.6o

E. 0.00837o

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Page 37: Chapter 4

Position, Velocity and Acceleration

• Position, Velocity and Acceleration are Vectors!

• x and y directions are INDEPENDENT!

0

0

tt

rrv

f

fav

0

0

tt

vva

f

fav

0

0

tt

xxv

f

fx

0

0

tt

yyv

f

fy

0

0

tt

vva

f

xxfx

0

0

tt

vva

f

yyfy

22yx vvv

22yx aaa

x direction y direction

Page 38: Chapter 4

Velocity in Two Dimensions

5 m/s

3 m/s

A ball is rolling on a horizontal surface at 5 m/s. It then rolls up a ramp at a 25 degree angle. After 0.5 seconds, the ball has slowed to 3 m/s. What is the change in velocity?

y

x

x-direction

vix = 5 m/s

vfx = 3 m/s cos(25)

vx = 3cos(25)–5 =-2.28m/s

y-direction

viy = 0 m/s

vfy = 3 m/s sin(25)

vy = 3sin(25)=+1.27 m/s 22yx vvv m/s 6.2

Page 39: Chapter 4

Acceleration in Two Dimensions

5 m/s

3 m/s

A ball is rolling on a horizontal surface at 5 m/s. It then rolls up a ramp at a 25 degree angle. After 0.5 seconds, the ball has slowed to 3 m/s. What is the average acceleration? [Assume force of gravity is very small].

y

xx-direction y-direction

s 0.5m/s28.2xa

2m/s 21.5

2m/s 56.4 s 0.5.27m/s1xa

2m/s 54.2

22yx aaa

Page 40: Chapter 4

A wagon of mass 50 kg is being pulled by a force F of magnitude 100 N applied through the handle at 30o

from the horizontal. Ignoring friction, find the magnitude of

(a) the horizontal component of F.

(b) the horizontal component of acceleration.

(c) the normal force exerted on the wagon.

Page 41: Chapter 4

Projectile Motion

A projectile – An object moving in 2-dimensions near the surface of the earth with only the force of gravity acting on it.

Eg: golf ball, batted base ball, kicked football, soccer ball, bullet, etc.

• Assume no air resistance.

• Assume g = -9.8 m/s2 constant.

• We are not concerned with the process that started the motion!

Page 42: Chapter 4

Free Fall: 1-dimensional motion.

+y

+x

ay = -9.8 m/s2, ax = 0

v0 = +5 m/s

At the maximum height:

• vy = 0

• Speeds at equal heights will be equal.

• Equal time going up/down.

Page 43: Chapter 4

+y

+x

ay = -9.8 m/s2,

ax = 0

v0 = 5 m/s

PROJECTILE: Free Fall motion in 2-dimensions.

v0x

v0y

Page 44: Chapter 4

PROJECTILE: Free Fall motion in 2-dimensions.

ay = -9.8 m/s2

ax = 0

v0x = v0cos

v0y = v0sin

What will happen to the y-component of the velocity?

What will happen to the x-component of the velocity?

Page 45: Chapter 4

Kinematics in Two Dimensions

• x = x0 + v0xt + ½ axt2

• vx = v0x + axt

• vx2 = v0x

2 + 2ax (x - x0)

• y = y0 + v0yt + ½ ayt2

• vy = v0y + ayt

• vy2 = v0y

2 + 2ay (y – y0)

x and y motions are independent!They share a common time t.

Page 46: Chapter 4

Kinematics for Projectile Motion

ax = 0 ay = -g

• x = x0 + v0t

• vx = v0x

• y = y0 + v0yt - 1/2 gt2

• vy = v0y - gt

• vy2 = v0y

2 - 2g yX

Y

Page 47: Chapter 4

PROJECTILE: Free Fall motion in 2-dimensions.

ay = -9.8 m/s2, ax = 0

Once the projectile is in air, the only force acting on it is gravity. Its trajectory (path of motion) is a parabola.

Fnet = ma = -mg

ay = -9.8 m/s2

ax = 0

Page 48: Chapter 4

PROJECTILE: Free Fall motion in 2-dimensions.

ay = -9.8 m/s2 and ax = 0

v0x = v0cos and v0y = v0sin

Page 49: Chapter 4

Two balls A and B of equal mass m. Ball A is released to fall straight down from a height h. Ball B is thrown horizontally. Which ball lands first?

A B

h

ay = -9.8 m/s2

ax = 0

Vo = 0

v0x = 0

v0y = 0

ay = -9.8 m/s2

ax = 0

Vo 0

v0x = Vo

v0y = 0

Page 50: Chapter 4

A

ay = -9.8 m/s2

ax = 0

vo = 0

v0x = 0

v0y = 0

y0 = 0, y = -h

• y = y0 + v0yt + ½ ayt2

• vy = v0y + ayt• vy

2 = v0y2 + 2ay (y – y0)

To find time t, use

y = y0 + v0yt + ½ ayt2

-h = 0 + (0 . t) + ½ (-g)t2

Gives 2h = gt2 and t = (2h/g)

Page 51: Chapter 4

Bay = -9.8 m/s2

ax = 0

Vo 0

v0x = vo

v0y = 0 • y = y0 + v0yt + ½ ayt2

• vy = v0y + ayt• vy

2 = v0y2 + 2ay (y – y0)

To find time t, use

y = y0 + v0yt + ½ ayt2

-h = 0 + (0 . t) + ½ (-g)t2

Gives 2h = gt2 and t = (2h/g)

Page 52: Chapter 4

A flatbed railroad car is moving along a track at constant velocity. A passenger at the center of the car throws a ball straight up. Neglecting air resistance, where will the ball land?1. Forward of the center of the car

2. At the center of the car

3. Backward of the center of the car

Page 53: Chapter 4

Since no air resistance is present, the ball and the train would be moving with the same horizontal velocity, and when the ball is tossed, it is given an additional velocity component in the vertical direction, but the original horizontal velocity component remains unchanged, and lands in the center of the train.

Page 54: Chapter 4

P 4.22A penny is dropped from the

observation deck of the Empire State building (369 m above the ground). With what velocity does it strike the ground? Ignore air resistance.

Page 55: Chapter 4

P 4.36An arrow is shot into the air at an

angle of 60.0o above the horizontal with a speed of 20.0 m/s.

(a) What are the x- and y-components of the velocity of the arrow 3.0 s after it leaves the bowstring?

(b) What are the x- and y- components of the displacement of the arrow during the 3.0-s interval?

Page 56: Chapter 4

A ball is thrown with a speed of 40.0 m/s at 55o above the horizontal. At the maximum height, its speed will be

A. B. C. D. E.

30%

0%

9%

47%

14%

A. 22.9 m/s

B. -9.8 m/s

C. 0 m/s

D. 32.8 m/s

E. 40.0 m/s

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Page 57: Chapter 4

A ball is thrown with a speed of 40.0 m/s at 35o above the horizontal. How long is it in air?

A. B. C. D. E.

8%

23%

25%25%

20%A. 6.69 s

B. 8.16 s

C. 2.34 s

D. 4.08 s

E. 4.68 s

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Page 58: Chapter 4

A ball is kicked straight up from ground level with initial velocity of 22.6 m/s. How high above the ground will the ball rise?

A. B. C. D. E.

8% 8%10%

69%

5%

A. 9.8 m

B. 3.00 m

C. 1.15 m

D. 26.1 m

E. 19.6 m

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Page 59: Chapter 4

Summary of Concepts

• X and Y directions are Independent!– Position, velocity and acceleration are vectors

• F = m a applies in both x and y direction

• Projective Motion– ax = 0 in horizontal direction

– ay = g in vertical direction

50

Page 60: Chapter 4

1. A car initially traveling at a velocity vo begins to slow down with a uniform deceleration of 1.20 m/s2 and comes to a stop in 26.0 seconds. Determine the value of vo.

A. B. C. D. E.

95%

5%0%0%0%

A. 31.2 m/s

B. 21.7 m/s

C. 27.2 m/s

D. 24.8 m/s

E. None of these

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Page 61: Chapter 4

2. A 102.0-kg person stands on a scale inside an elevator moving downward with anacceleration of 1.300 m/s2. What will be his apparent weight?

A. B. C. D. E.

0%7%

0%2%

91%

A. 999.6 N

B. 132.6 N

C. 867.0 N

D. 1132 N

E. 0 N

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Page 62: Chapter 4

3. A ball is thrown with a speed of 27.0 m/s at 35o above the horizontal. At the maximum height, its speed will be

A. B. C. D. E.

2% 0%

16%

82%

0%

A. 27.0 m/s

B. -9.8 m/s

C. 0 m/s

D. 22.1 m/s

E. 15.5 m/s

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Page 63: Chapter 4

4. A ball is thrown with a speed of 32.0 m/s at 50o above the horizontal. How long is it in air?

A. B. C. D. E.

11% 13%

64%

4%7%

A. 4.20 s

B. 6.53 s

C. 3.27 s

D. 2.50 s

E. 5.00 s

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Page 64: Chapter 4

5. A ball is kicked straight up from ground level with initial velocity of 16.6 m/s. How high above the ground will the ball rise?

A. B. C. D. E.

2%

93%

0%2%2%

A. 28.1 m

B. 14.1 m

C. 1.69 m

D. 0.847 m

E. 1.18 m

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Page 65: Chapter 4

6. A block is at rest on a flat board. The flat board is then gently tilted. If the block starts to slide at a tilt angle of 23.8o, what is the coefficient of static friction (s) between the block and the board?

A. B. C. D. E.

0% 0%

89%

9%2%

A. 0.40

B. 0.91

C. 23.8

D. 87.6

E. 0.44

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