Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

68
Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions

Transcript of Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Page 1: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Newtonian Mechanics

Chapter 3

Kinematics in Two Dimensions

Page 2: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Learning ObjectivesNewtonian Mechanics-Kinematics

I.A.2. Motion in two dimensions, including projectile motion a) Students should be able to add, subtract, and resolve displacement

and velocity vectors, so they can:1) Determine components of a vector along two specified, mutually

perpendicular axes.2) Determine the net displacement of a particle or the location of a

particle relative to another.3) Determine the change in velocity of a particle or the velocity of

one particle relative to another.b) Students should understand the motion of projectiles in a uniform

gravitational field, so they can:1) Write down expressions for the horizontal and vertical

components of velocity and position as functions of time, and sketch or identify graphs of these components.

2) Use these expressions in analyzing the motion of a projectile that is projected with an arbitrary initial velocity.

Page 3: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Table of Contents

3.1 Displacement, Velocity and Acceleration

3.2 Equations of Kinematics in Two Dimensions

3.3 Projectile Motion

3.4 Relative Velocity

Page 4: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Chapter 3Motion in Two Dimensions

Section 1:

Displacement, Velocity, and Acceleration

Page 5: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Motion in Two Dimensions

How do we describe an object moving across a

surface (x & y directions)?

Similar to how we described motion along a line.

Define a reference point, axes of measurement,

and positive directions.

Each Dimension is independent of the other

Think Etch-a-Sketch

Page 6: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Ahhh the memories…

Page 7: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

position initial or

position final r

ntdisplaceme orrr

Displacement

Page 8: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

ttt o

o

rrr

v

Average velocity is the displacement divided by the elapsed time.

Velocity

Page 9: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

The instantaneous velocity indicates how fastthe car moves and the direction of motion at eachinstant of time.

tt

rv

0lim

Velocity

Page 10: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

ttt o

o

vvv

a

DEFINITION OF AVERAGE ACCELERATION

ov

v v

Acceleration

Page 11: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #1A truck drives due south for 1.2 km in 1.5 minutes. Then, the truck turns and drives 1.2 km due west for 1.5 minutes. Which one of the following statements is correct?

a) The average speed for the two segments is the same. The average velocity for the two segments is the same.

b) The average speed for the two segments is not the same. The average velocity for the two segments is the same.

c) The average speed for the two segments is the same. The average velocity for the two segments is not the same.

d) The average speed for the two segments is not the same. The average velocity for the two segments is not the same.

Page 12: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #2A ball is rolling down one hill and up another as shown. Points A and B are at the same height. How do the velocity and acceleration change as the ball rolls from point A to point B?

a) The velocity and acceleration are the same at both points.b) The velocity and the magnitude of the acceleration are the same at both

points, but the direction of the acceleration is opposite at B to the direction it had at A.

c) The acceleration and the magnitude of the velocity are the same at both points, but the direction of the velocity is opposite at B to the direction it had at A.

d) The horizontal component of the velocity is the same at points A and B, but the vertical component of the velocity has the same magnitude, but the opposite sign at B. The acceleration at points A and B is the same.

e) The vertical component of the velocity is the same at points A and B, but the horizontal component of the velocity has the same magnitude, but the opposite sign at B. The acceleration at points A and B has the same magnitude, but opposite direction.

Page 13: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Chapter 3Motion in Two Dimensions

Section 2:

Equations of Kinematics in Two Dimensions

Page 14: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Equations of Kinematics

221 attvxx oo

atvv o

oo xxavv 222

Quick Review

Page 15: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Keys to Solving 2-D Problems

1. Resolve all vectors into components x-component Y-component

2. Work the problem as two one-dimensional problems. Each dimension can obey different

equations of motion.3. Re-combine the results for the two components

at the end of the problem.

Page 16: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

tavv xoxx oxoxx xxavv 222

221

, tatvxx xxoo

x component

Page 17: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

tavv yoyy 2

21 tatvyy yoyo

oyoyy yyavv 222

y component

Page 18: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Actual motion

The x part of the motion occurs exactly as it would if the y

part did not occur at all, and vice versa.

Remember the bullet drop video!

Page 19: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

In the x direction, the spacecraft has an initial velocity component of +22 m/s and an acceleration of +24 m/s2. In the y direction, the analogous quantities are +14 m/s and an acceleration of +12 m/s2. Find (a) x and vx, (b) y and vy, and (c) the final velocity of the spacecraft at time 7.0 s.

Example 1 A Moving Spacecraft

Page 20: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

In the x direction, the spacecraft has an initial velocity component of +22 m/s and an acceleration of +24 m/s2. In the y direction, the analogous quantities are +14 m/s and an acceleration of +12 m/s2. Find (a) x and vx, (b) y and vy, and (c) the final velocity of the spacecraft at time 7.0 s.

x ax vx vox t

? +24.0 m/s2 ? +22 m/s 7.0 s

y ay vy voy t

? +12.0 m/s2 ? +14 m/s 7.0 s

Example 1 A Moving Spacecraft

Page 21: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

x ax vx vox t? +24.0 m/s2 ? +22 m/s 7.0 s

m 740s 0.7sm24s 0.7sm22 2221

221

tatvx xox

sm190s 0.7sm24sm22 2

tavv xoxx

x component

Page 22: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

y ay vy voy t? +12.0 m/s2 ? +14 m/s 7.0 s

m 390s 0.7sm12s 0.7sm14 2221

221

tatvy yoy

sm98s 0.7sm12sm14 2

tavv yoyy

y component

Page 23: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

vsm98yv

sm190xv

sm210sm98sm190 22 v

2719098tan 1

Resultant velocity

Page 24: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #3

An eagle takes off from a tree branch on the side of a mountain and flies due west for 225 m in 19 s. Spying a mouse on the ground to the west, the eagle dives 441 m at an angle of 65 relative to the horizontal direction for 11 s to catch the mouse. Determine the eagle’s average velocity for the thirty second interval.

a) 19 m/s at 44 below the horizontal direction

b) 22 m/s at 65 below the horizontal direction

c) 19 m/s at 65 below the horizontal direction

d) 22 m/s at 44 below the horizontal direction

e) 25 m/s at 27 below the horizontal direction

Page 25: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #4

In two-dimensional motion in the x-y plane, what is the relationship between the x part of the motion to the y part of the motion?

a) The x part of the motion is independent of the y part of the motion.

b) The y part of the motion goes as the square of the x part of the motion.

c) The x part of the motion is linearly dependent on the y part of the motion.

d) The x part of the motion goes as the square of the y part of the motion.

e) If the y part of the motion is in the vertical direction, then x part of the motion is dependent on the y part.

Page 26: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #5

Complete the following statement: In two-dimensional motion in the x-y plane, the x part of the motion and the y part of the motion are independent

a) only if there is no acceleration in either direction.

b) only if there is no acceleration in one of the directions.

c) only if there is an acceleration in both directions.

d) whether or not there is an acceleration in any direction.

e) whenever the acceleration is in the y direction only.

Page 27: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #6

A roller coaster car rolls from rest down a 20o incline with an acceleration of 5.0 m/s2

How far horizontally has the coaster travelled in 10 seconds?

a = 5.0 m/s2

a

ax

ay

Page 28: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #7

A roller coaster car rolls from rest down a 20o incline with an acceleration of 5.0 m/s2

How far vertically has the coaster travelled in 10 seconds?

a = 5.0 m/s2

a

ax

ay

Page 29: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #8

Jackson heads east at 25 km/h for 20 minutes before heading south at 45 km/h for 20 minutes. Hunter heads south at 45 km/h for 10 minutes before heading east at 25 km/h for 30 minutes. Which driver has the greater average velocity, if either?

a) Jackson

b) Hunter

c) They both have the same average velocity.

Page 30: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Chapter 3Motion in Two Dimensions

Section 3:

Projectile Motion

Page 31: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Projectile Motion

Something is fired, thrown, shot, or hurled near the

Earth’s surface

Horizontal velocity is constant

• ax = 0, vo,x = vx

Vertical velocity is accelerated

• ay = g = 9.80665 m/s2 ≈ 10 m/s2 (constant)

Air resistance is ignored

If launch angle is not horizontal or vertical

• must resolve initial velocity into x and y components

Page 32: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

The airplane is moving horizontally with a constant velocity of +115 m/s at an altitude of 1050 m. Determine the time requiredfor the care package to hit the ground.

Example 3 A Falling Care Package

Page 33: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

y ay vy voy t-1050 m -9.80 m/s2 0 m/s ?

Page 34: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

y ay vy voy t-1050 m -9.80 m/s2 0 m/s ?

221 tatvy yoy

221Δ tay y

ya

yt

2

0

Page 35: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Example 4 The Velocity of the Care Package

A plane is moving horizontally with a constant velocity of 115 m/s at an altitude of 1050 m. Ignoring air resistance, determine the velocity of a package just before it hits the ground.

Page 36: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

yavv yyoy Δ22,

2

sm184v

22yx vvv

yavvv yoxo 22,

2,

xox vv ,

msmsmsmv 105081.920115 222

v

vxcos

v

vx1cos

o3.51

y ay v vo,y vo,x t-1050 m -9.80 m/s2 ? 0 m/s 115 m/s 14.6 s

sm

sm

184

115

Page 37: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Conceptual Example 5I Shot a Bullet into the Air…

Suppose you are driving a convertible with the top down. The car is moving to the right at constant velocity. You point a rifle straight up into the air and fire it. In the absence of air resistance, where would the bullet land – (a) behind you

(b) ahead of you

(c) in the barrel of the rifle

Page 38: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

A placekicker kicks a football at and angle of 40.0 degrees andthe initial speed of the ball is 22 m/s. Ignoring air resistance, determine the maximum height that the ball attains.

Example 6 The Height of a Kickoff

Page 39: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

ov

oxv

oyv

sm1440sinsm22sin ooy vv

sm1740cossm22sin oox vv

Page 40: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

y ay vy voy t? -9.80 m/s2 0 14 m/s

Page 41: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

3.3 Projectile Motion

yavv yyoy Δ22,

2

y ay vy voy t? -9.80 m/s2 0 14 m/s

y

oyy

a

vvy

2

22

2

2

sm8.92

sm140

y m10

Page 42: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

What is the time of flight between kickoff and landing?

Example 7 The Time of Flight of a Kickoff

Page 43: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

y ay vy voy t0 -9.80 m/s2 14 m/s ?

221

, tatvy yyo

s 9.2t

tavty yyo 21

,0 s 0t

tav yyo 21

,0

y

yo

a

vt ,2

280.9

142

sm

sm

Page 44: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Calculate the range R of the projectile.

Example 8 The Range of a Kickoff

Page 45: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

x ax vx Vo,x t? 0 17 m/s 2.9 s

221

, tatv xxox

mx 49

ssmx 9.217

0

Page 46: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #9

A diver running 1.8 m/s dives out horizontally from the edge of a vertical cliff and 3.0 s later reaches the water below. How high was the cliff?

h

d

v

Page 47: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #10A diver running 1.8 m/s dives out horizontally from the edge of a vertical cliff and 3.0 s later reaches the water below. How far from its base did the diver hit the water?

h

d

v

Page 48: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #11

When a football in a field goal attempt reaches its maximum height, how does its speed compare to its initial speed?

a) It is zero.

b) It is equal to its initial speed.

c) It is greater than its initial speed.

d) It is less than its initial speed.

Page 49: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #12

The Zambezi River flows over Victoria Falls in Africa. The falls are approximately 108 m high. If the river is flowing horizontally at 3.6 m/s just before going over the falls, what is the speed of the water when it hits the bottom? Assume the water is in freefall as it drops.

Page 50: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #13

An astronaut on the planet Zircon tosses a rock horizontally with a speed of 6.75 m/s. The rock falls a distance of 1.20 m and lands a horizontal distance of 8.95 m from the astronaut. What is the acceleration due to gravity on Zircon?

Page 51: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

For The Adventurous

Here are some more advanced equations.

They are not given on the equation sheet

You are free to use them if they are “memorized”

• You can have programs stored in your calc

Unlikely you will need them, but…

Page 52: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Vertical Position Equation

vo h

x

yVertical Position as a functionof vo, , and horizontal position

sin, oyo vv 2

, 2

1gttvy yo

2, 2

1tatvx xxo

cos, oxo vv

cosov

xt

2

cos2

1

cossin

ooo v

xg

v

xvy

22

2

cos2tan

ov

xgxy

0

Page 53: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Maximum Height

gtvv oy sin 0

g

vt otop

sin

vo h

Equation for the maximum Height of a projectile.

At max height,vy = 0 2

2

1sin tgtvy o

2

sin

2

1sinsin

g

vg

g

vvy ooo

g

vy o

2

sin 22

max

Page 54: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Range Equation

tvx o cos 2

2

1sin tgtvy o

g

vt o sin2

g

vvx oo

sin2cos

uuu cossin22sin

2sin2

g

vx o

cossin2 2

g

vx o

0

vo

d

Page 55: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Chapter 3Motion in Two Dimensions

Section 4:

Relative Velocity

Page 56: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Relative Motion Problems

Describe motion of an object from some fixed point

Relative motion problems are difficult to do unless one applies

vector addition concepts

Define a vector for an object velocity relative to the fluid, and

another for the velocity of the fluid relative to the observer.

Add two vectors together.

Page 57: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

TGPTPG vvv

velocity of personrelative to the ground

velocity of personrelative to the train

velocity of trainrelative to the ground

Page 58: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

The engine of a boat drives it across a river that is 1800m wide.The velocity of the boat relative to the water is 4.0m/s directed perpendicular to the current. The velocity of the water relativeto the shore is 2.0m/s.

(a) What is the velocity of the boat relative to the shore?

(b) How long does it take for the boat to cross the river?

Example 11 Crossing a River

Page 59: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

22 sm0.2sm0.4 BSv

WSBWBS vvv

0.2

0.4tan 1

x vBW vWS vBS t

1800m 4.0m/s 2.0m/s ? ?

22WSBWBS vvv

sm5.4BSv

WS

BW

v

v1tan

63

Page 60: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

sm4.0

m 1800t

x vBW vWS t

1800m 4.0m/s 2.0m/s ?

BWv

xt

s 450

2

2

1attvx BW

0

Page 61: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #14

You are trying to cross a river that flows due south with a strong current. You start out in your motorboat on the east bank desiring to reach the west bank directly west from your starting point. You should head your motorboat

a) due west.

b) due north.

c) in a southwesterly direction.

d) in a northwesterly direction.

Page 62: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #15

At an air show, three planes are flying horizontally due east. The velocity of plane A relative to plane B is vAB; the velocity of plane A relative to plane C is vAC; and the velocity of plane B relative to plane C is vBC. Determine vAB if vAC = +10 m/s and vBC = +20 m/s?

a) 10 m/s b) +10 m/s

c) 20 m/s d) +20 m/s

e) zero m/s

Page 63: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #16

A train is traveling due east at a speed of 26.8 m/s relative to the ground. A passenger is walking toward the front of the train at a speed of 1.7 m/s relative to the train. Directly overhead the train is a plane flying horizontally due west at a speed of 257.0 m/s relative to the ground. What is the horizontal component of the velocity of the airplane with respect to the passenger on the train?

a) 258.7 m/s, due west b) 285.5 m/s, due west

c) 226.8 m/s, due west d) 231.9 m/s, due west

e) 257.0 m/s, due west

Page 64: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #17Sailors are throwing a football on the deck of an aircraft carrier as it is sailing with a constant velocity due east. Sailor A is standing on the west side of the flight deck while sailor B is standing on the east side. Sailors on the deck of another aircraft carrier that is stationary are watching the football as it is being tossed back and forth as the first carrier passes. Assume that sailors A and B throw the football with the same initial speed at the same launch angle with respect to the horizontal, do the sailors on the stationary carrier see the football follow the same parabolic trajectory as the ball goes east to west as it does when it goes west to east?a) Yes, to the stationary sailors, the trajectory the ball follows is the same whether it is traveling west to east or east to west.b) No, to the stationary sailors, the length of the trajectory appears shorter as it travels west to east than when it travels east to west.c) No, to the stationary sailors, the ball appears to be in the air for a much longer time when it is traveling west to east than when it travels east to west.d) No, to the stationary sailors, the length of the trajectory appears longer as it travels west to east than when it travels east to west.e) No, to the stationary sailors, the ball appears to be in the air for a much shorter time when it is traveling west to east than when it travels east to west.

Page 65: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #18Cars A and B are moving away from each other as car A moves due north at 25 m/s with respect to the ground and car B moves due south at 15 m/s with respect to the ground. What are the velocities of the other car according to the two drivers?a) Car A is moving due north at 25 m/s; and car B is moving due south at 15 m/s.b) Car A is moving due south at 25 m/s; and car B is moving due north at 15 m/s.c) Car A is moving due north at 40 m/s; and car B is moving due south at 40 m/s.d) Car A is moving due south at 40 m/s and car B is moving due north at 40 m/s.e) Car A is moving due north at 15 m/s and car B is moving due south at 25 m/s.

Page 66: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #19John always paddles his canoe at constant speed v with respect to the still water of a river. One day, the river current was due west and was moving at a constant speed that was close to v with respect to that of still water. John decided to see whether making a round trip across the river and back, a north-south trip, would be faster than making a round trip an equal distance east-west. What was the result of John’s test?

a) The time for the north-south trip was greater than the time for the east-west trip.

b) The time for the north-south trip was less than the time for the east-west trip.

c) The time for the north-south trip was equal to the time for the east-west trip.

d) One cannot tell because the exact speed of the river with respect to still water is not given.

Page 67: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.

Question #20

A boat attempts to cross a river. The boat’s speed with respect to the water is 12.0 m/s. The speed of the river current with respect to the river bank is 6.0 m/s. At what angle should the boat be directed so that it crosses the river to a point directly across from its starting point?

BW

WS

v

v1sin

6.0m/s12.0m/s

sm

sm

12

0.6sin 1

Page 68: Newtonian Mechanics Chapter 3 Kinematics in Two Dimensions.