Chapter 7 Forces and Motion In Two Dimensions. Equilibrium An object is in equilibrium when the Net Force on the object is zero.  F Net = 0  Acceleration.

Slides:



Advertisements
Similar presentations
Section 3-5: Projectile Motion
Advertisements

Velocity v= v0 + at Position x = x0 + v0t + ½ at2 FORCES
7-2 Projectile Motion. Independence of Motion in 2-D Projectile is an object that has been given an intial thrust (ignore air resistance)  Football,
Projectile Motion. What Is It? Two dimensional motion resulting from a vertical acceleration due to gravity and a uniform horizontal velocity.
CBA #1 Review Graphing Motion 1-D Kinematics Projectile Motion Circular Motion Gravity Graphing Motion 1-D Kinematics Projectile Motion Circular.
Motion in Two Dimensions
Net Force Problems There are 2 basic types of net force problems
CHAPTER 3 PROJECTILE MOTION. North South EastWest positive x positive y negative x negative y VECTORS.
Applications of Newton’s Laws
Aim: How can we explain forces at an angle? Do Now: Solve for the x and y components: 10 N x y 30° x = 5 N x = 8.7 N.
Physics 111: Mechanics Lecture 3
Physics 2.2.
CBA #1 Review Graphing Motion 1-D Kinematics
CHAPTER 7 Rotational Motion and the Law of Gravity Angular Speed and Angular Acceleration s = arc length Θ = arc angle (radians) Θ = s ; where r = radius.
Gravity ISCI More Free Fall Free Fall Vertical and Horizontal Components of Free Fall.
Do now A B + = ? The wrong diagrams Draw the right diagram for A + B.
Projectile Motion Neglecting air resistance, what happens when you throw a ball up from the back of a moving truck? Front? Behind? In? GBS Physics Demo.
Glencoe Physics Chapter 7 Forces and Motion in Two Dimensions
Vectors and Direction In drawing a vector as an arrow you must choose a scale. If you walk five meters east, your displacement can be represented by a.
Forces On An Inclined Plane. FfFf FNFN FgFg 30° Think about the forces as she sleds down the hill in the laundry basket (if it is not a non-frictionless.
CHAPTER 4 The Laws of Motion Newton’s First Law: Newton’s First Law: An object at rest remains at rest and an object in motion continues in motion with.
Answer all questions on a piece of loose leaf and turn in at the end of the period for homework credit. Unit 4 Review.
vel 60 (m/s) time (sec)
Chapter 7 Forces In Two Dimensions. Equilibrant: Motion along an inclined plane x Θ y Θ.
More Projectile Motion Discussion: Examples
Ch. 7 Forces and Motion in Two Dimensions
Physics Lesson 6 Projectile Motion Eleanor Roosevelt High School Mr. Chin-Sung Lin.
Projectile Motion objectives 1.What is a Projectile?What is a Projectile? 2.Characteristics of a Projectile's TrajectoryCharacteristics of a Projectile's.
Uniform Circular Motion (UCM) The object travels in a circular path with a constant speed. Its velocity is tangent to the circle and is changing due to.
Chapter 5 Circular Motion; Gravitation. Centripetal Acceleration Centripetal means “Center Seeking” and the centripetal force on an object moving in a.
Physics 203 – College Physics I Department of Physics – The Citadel Physics 203 College Physics I Fall 2012 S. A. Yost Chapter 5 Circular Motion, Universal.
Vectors and Linear Motion. Vector Quantities: Have a magnitude And direction ex: meters, velocity, acceleration Scalar Quantities: Have only a magnitude.
Newton 2nd Law problems - Atwood Machines -Incline Planes -Tension Problems -Other Object Connected problems.
Kinematics. The 3 Kinematic equations There are 3 major kinematic equations than can be used to describe the motion in DETAIL. All are used when the acceleration.
Motion in Two Dimensions
UEQ When a object travels through the air, what variables defines its motion.
Motion in Two Dimensions Chapter 6. Motion in Two Dimensions  In this chapter we’ll use what we learned about resolving vectors into their x- and y-components.
Motion in Two Dimensions Chapter 7.2 Projectile Motion What is the path of a projectile as it moves through the air? ? . What forces act on projectiles?
CHAPTER 6 MOTION IN 2 DIMENSIONS.
Circular Motion r v F c, a c. Centripetal acceleration – acceleration of an object in circular motion. It is directed toward the center of the circular.
Physics Lab Agenda – Thursday 12/16/04 – Pick-up materials on front desks – Intro to Horizontal Motion Lab – Bring physics HW to do in class.
Motion in Two Dimensions Chapter 7.2 Projectile Motion What is the path of a projectile as it moves through the air? Parabolic? Straight up and down?
Projectile Motion.
Motion in Two Dimensions
2D Motion 2015 cjcb Angled Projectile Motion. RECAP: What is Projectile Motion? Projectile motion is the motion of an object that is being thrown or launched.
Push and Pull Newton’s Laws. Newton’s First Law An object at rest remains at rest, and an object in motion continues in motion with constant velocity.
Forces in Equilibrium & Motion along an Incline Chapter 7.1.
CHAPTER 4 The Laws of Motion Newton’s First Law: Newton’s First Law: An object at rest remains at rest and an object in motion continues in motion with.
Uniform Circular Motion (UCM) The object travels in a circular path with a constant speed. Its velocity is tangent to the circle and is changing due to.
Vector Objectives 1. Add and subtract displacement vectors to describe changes in position. 2. Calculate the x and y components of a displacement, velocity,
Physics Chapter 7 Forces and Motion in Two Dimensions.
ForcesGravityNet ForcesFree Body Diagrams Misc Forces and Motion FINAL JEOPARDY Go To Score Card.
Physics Fall Practice Final Exam 25 Questions Time = Less than 30 minutes.
Projectile Motion Introduction Horizontal launch.
Motion in Two and Three Dimensions Chapter 4. Position and Displacement A position vector locates a particle in space o Extends from a reference point.
Dynamics of Uniform Circular Motion  An object moving on a circular path of radius r at a constant speed, V  Motion is not on a straight line, the direction.
 Gravity is 9.8 or ~10 m/s 2  If dropped from rest: y = -½ gt 2.
CHAPTER - 7 Forces and Motion in Two Dimensions
Brain Teaser During the Little League baseball season, every team plays every other team in the league ten times. If there are ten teams in the league,
Projectile Review.
PROJECTILE MOTION 2-D MOTION.
Chapter Motion in Two and Three Dimensions
Projectile motion Projectile Motion Subject to Gravity Assumptions:
Projectile Motion AP Physics B.
Projectile Motion AP Physics C.
Projectile Motion.
Projectile Motion AP Physics C.
Projectile Motion AP Physics C.
Circular Motion r v Fc, ac.
DO NOW A steel beam is rotated in a horizontal plane to provide the centripetal acceleration for training pilots. If the pilot sits 2.0 m from the center.
Presentation transcript:

Chapter 7 Forces and Motion In Two Dimensions

Equilibrium An object is in equilibrium when the Net Force on the object is zero.  F Net = 0  Acceleration = 0  Constant Velocity  Velocity = 0

Equilibrium in 2 Dimensions  F x = 0  F y = 0

Static Equilibrium Objects are not moving.  F Net = 0  Acceleration = 0  Velocity = 0

Static Equilibrium 50N 20N F Net = 0 F x = 0 F y = 0

2kg 60°

2kg F g = mg F g = 2kgx9.8m/s 2 F g = 20N F1F1 F2F2

F1F1 F2F2 60° x direction F x = -F 1x + F 2x 0 = -F 1x + F 2x F 1x = F 2x F 1 cos60°= F 2 cos 60° F 1 = F 2 = F

F g = 20N F1F1 F2F2 60° y direction F y = F 1y + F 2y - F g F g = F 1 sin60°+ F 2 sin 60° 0 = F 1y + F 2y - F g F g = F 1y + F 2y F g = Fsin60°+ Fsin 60° F g = 2Fsin60°

__F g __ 2sin60° = F _20N__ 2sin60° = F 11.5N = F

Homework Finish Work Sheet

50kg FtFt FPFP FgFg

FtFt FPFP FgFg

FtFt FPFP FgFg 30° F g = 50kg·9.8m/s 2 F g = mg F g = 500N F tx F ty

F x = F px - F tx X - ComponentsY- Components 0 = F p - F tx F px = F tx F p = F t cos30° F y = F py - F g 0 = F py - F g F ty = F g F t sin30° = F g F g sin30° F t =

X - ComponentsY- Components F p = F t cos30° F g sin30° F t = 500N sin30° F t = F t = 1000N F p = 1000cos30° F p = 866N

Homework Finish Work Sheet

Incline Plane FgFg FNFN F N =F g

Incline Plane FNFN FgFg θ FfFf

FNFN FgFg θ FfFf

FNFN FgFg θ FfFf F y =F N – F g cosθ F x =F f – F g sinθ F N = F g cosθ

FNFN θ FfFf FgFg

θ FgFg FfFf θ FNFN

θ FgFg FfFf θ FNFN F gy F gx F y =F N – F g cosθ F x =F f – F g sinθ F N = F g cosθ

Problem In a block/inclined plane system, the inclined plane makes an angle of 60° with the ground. The coefficient of friction is 0.5. If the block has a mass of 1.02kg, what is the net force on the block? What is the blocks acceleration?

Incline Plane FNFN FgFg θ=60° FfFf 1.02kg F g =mg F g =1.02kg·9.8m/s 2 =10N Ff=μFNFf=μFN

θ FgFg FfFf θ FNFN

FgFg FfFf 60° FNFN F gy F gx F x =F f – F gx F y =F N – F g cosθ F y =F N – F gy F x =F f – F g sinθ

F y = F N – F g cosθ F N = F g cosθ 0 = F N – F g cosθ F N = 10cos60° F N = 5N

F x =F f – F g sinθ F f = μF N F x =μF N – F g sinθ F x =0.5·5N – 10N·sin60° F x =2.5 – 8.7N F x = –6.2N Net Force of 6.2N down the incline!!

F Net = ma 6.1m/s 2 = a F Net m = a 6.2N 1.02kg = a 6.1m/s 2 down the incline!!

Projectile Motion

Vertical Component Horizontal Component

Projectile Motion Projectile motion is the combination of two independent motions, the motion in the x direction and the motion in the y direction. These two motions are usually independent of each other.

Projectile Motion y component x component

Problem Solving Strategy 1. Break up the problem into two interconnected one-dimensional problems. y component x component

Problem Solving Strategy 2. Vertical motion (y component) is exactly that of an object being dropped or thrown straight up or down. (g - gravity!!!!!)

Problem Solving Strategy 3. Horizontal motion (x component) is the same as solving constant velocity problems.

Problem Solving Strategy 4. Vertical (y) and horizontal (y) components are connected by the variable time (t). Solving for time in one dimension, x or y, automatically gives you the time for the other dimension.

d = d 0 +1/2(v+v 0 )t v 2 = v a(d-d 0 ) v = v 0 + at d = d 0 +v 0 t + ½at 2 *Basic Equations*

Problem: A ball is kicked horizontally, with a velocity of 25m/s, off a 122.5m high cliff. How far from the cliff did the ball land?

Sketch the Problem y component x component v = 25 m/s y = m

y component (up is +) d = d 0 +v 0 t + ½at 2 d = ½at m = ½(-9.8m/s 2 )t 2 = t 2 2(-122.5m) (-9.8m/s 2 )

y component (up is +) = t 2(-122.5m) (-9.8m/s 2 ) √ 5.0s = t Use this to solve for distance in the x direction!!!

x component d = d 0 + v 0 t + ½at 2 d = v 0 t d = (25m/s)(5s) d = 125m

Projectiles Launched at an Angle θ Range

Launch Problem A football is thrown with a speed 15m/s at an angle of 60° with the horizontal. How far is the football thrown?

v = 15 m/s 60° Sketch the Problem y component x component

1. Known x 0 = 0 y 0 = 0 v 0 = 15m/s θ 0 = 60° a = -g =-9.8m/s 2 2. Unknown v y v x d x d y t

3. Find the x/y components of the velocity. v x0 = (15m/s)cos60° v x0 = 7.5m/s v y0 = (15m/s)sin60° v y0 = 13m/s

4. Break up the x/y components and find time, then distance.

y - component v y = v 0 + at v y will be zero at the top (9.8m/s 2 )t = 13m/s 0 = 13m/s + (-9.8m/s 2 )t 13m/s 9.8m/s 2 t =

13m/s 9.8m/s 2 t = t = 1.3s This is the time for half the trip!! t total = 2.6s

x component d x = d 0 +v x0 t + ½at 2 d x = v x0 t d x = (7.5m/s)(2.6s) d x = 19.5m

y - component Let’s find the height!! d y = d y0 +v y0 t + ½at 2 d y = v y0 t + ½at 2 d y = 13m/s(1.3s) + ½(-9.8/s 2 )(1.3s) 2 d y = 16.9m – 8.3m d y = 8.6m

Circular Motion

v r v = dtdt d = 2πr t = T T is the Period: the time it takes to make one revolution.

v = dtdt 2πrT2πrT

a c = v2rv2r 4π2rT24π2rT2 Centripetal Acceleration

Centripetal Force Centripetal Force is the force toward the center of the circle that keeps an object moving in a circle.

Centripetal Force FcFc

F c = ma c Centripetal Force 4π2rT24π2rT2 F c = m ( )

Example A 15g whistle is being swung on a lanyard 0.30m long. If one revolution takes 0.5s, what is the centripetal force?

Example

m = 15g =.015kg Given: F c = ? Find: T = 0.5s

4π2rT24π2rT2 F c = m ( ) 4π 2 (.3m) (0.5s) 2 F c =.015m ( ) F c = 0.7N

Homework Worksheet Due: 12/14/06

Universal Gravity

What does gravity depend on? Mass Distance G

m1m1 m2m2 m 1 m 2 F ∞

r

r 1 r 2

m1m1 m2m2 F ∞ r m 1 m 2 r 2

F = m 1 m 2 r 2 G G – Gravitational Constant

G – 6.67 X Nm 2 /kg 2

F = Mm r2 r2 G M m

What is the magnitude of the gravitational force that acts on each particle, m 1 is 12kg and m 2 is 25kg and the two are 1.2m away. m1m1 m2m2 r

F = Gm 1 m 2 r2 r2 F= (6.67x Nm 2 /kg 2 )(12kg)(25kg) (1.2m) 2 F= 1.4 x N

Acceleration due the Gravity(g) F = GM Earth m r2 r2 mg = GM Earth m r2 r2

Acceleration due the Gravity(g) g = GM Earth r2 r2 r

g= (6.67x Nm 2 /kg 2 )(5.97x10 24 kg) (6.38x10 6 m) 2 g= 9.8m/s 2 g = GM Earth r2 r2

Homework Page: 194 Prob: 20,27,28,35,37 Due: 12/18/06 Test: 12/21/06

Satellites 1km/s.6mi/s

Satellites

Satellites – 17500mi/hr

Lets find a satellite speed!!! Fc = Fg r

ma c = Gm E m r 2 Gm E r 2 = v2rv2r

Gm E r = v2v2 = v √

Homework Worksheets Page: 194 Prob: 23,24,25,50,51 Due: 12/20/06 Test: 12/21/06

Homework Review Worksheet Due: 12/21/06 Test: 12/21/06