Chapter 7 Rotational Motion and the Law of Gravity.

Slides:



Advertisements
Similar presentations
 The point or line that is the center of the circle is the axis of rotation.  If the axis of rotation is inside the object, the object is rotating (spinning).
Advertisements

Circular and Rotational Motion
Rotational Motion and the Law of Gravity
Warm-up: Centripetal Acceleration Practice
GRAVITATIONAL MOTION.
ROTATIONAL MOTION and the LAW of GRAVITY
Chapter 7 Rotational Motion and The Law of Gravity.
Circular Motion. Circular motion: when an object moves in a two- dimensional circular path Spin: object rotates about an axis that pass through the object.
Physics 111: Mechanics Lecture 09
Rotational Motion and The Law of Gravity
Measuring Rotational Motion
© 2010 Pearson Education, Inc. Lecture Outline Chapter 7 College Physics, 7 th Edition Wilson / Buffa / Lou.
Circular Motion and Gravitation
Rotational Motion and The Law of Gravity
Rotational Motion. Rotational motion is the motion of a body about an internal axis. In rotational motion the axis of motion is part of the moving object.
NAZARIN B. NORDIN What you will learn: Centripetal force: acceleration, centrifugal force/ acceleration, mass-radius polygons Centrifugal.
Uniform Circular Motion the motion of an object traveling in a circular path an object will not travel in a circular path naturally an object traveling.
Physics Ch. 7 Rotational Motion
Rotational Motion and The Law of Gravity
Holt Physics Chapter 7 Rotational Motion Measuring Rotational Motion Spinning objects have rotational motion Axis of rotation is the line about which.
Chapter 7 Rotational Motion.
Ch 7 - Circular Motion Circular motion: Objects moving in a circular path.
Chapters 7 & 8 Rotational Motion and The Law of Gravity.
Circular Motion. Questions for Consideration  How do we measure circular motion?  What is a radian?  What are the angular analogs of linear motion?
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.
Lecture 18 Rotational Motion
Chapter 10 Rotation of a Rigid Object about a Fixed Axis.
Rotation and Newton’s Universal Law of Gravitation
Ch. 7 (Section 7.3) Circular Motion.
Introduction to Uniform Circular Motion Uniform Circular Motion An object moves at uniform speed in a circle of constant radius. Uniform circular motion.
Chapter 7 Circular Motion.
Acceleration is equal to Δv/Δt. Velocity is a vector and there are two ways a vector can be changed: by changing magnitude or by changing direction.
Chapter 10 Rotation.
Tangential and Centripetal Accelerations
ROTATIONAL MOTION Uniform Circular Motion
CIRCULAR MOTION.
Circular Motion. Uniform Circular Motion Motion of an object at constant speed along a circular path.
Circular Motion Chapter 9. Circular Motion Axis – is the straight line around which rotation takes place. Internal Axis - is located within the body of.
Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.
Rotational Motion and the Law of Gravity.  = angle from 0 r = radius of circle s = arc length (in radians)  = (in radians)
CIRCULAR MOTION. Linear Motion d – distance (in meters) v – velocity (in meters/second) a – acceleration (in meters/second 2 ) Distance = 2  r.
CIRCULAR MOTION. WHAT IS UNIFORM CIRCULAR MOTION The motion of an object in a circle at constant speed. However, direction and therefore velocity are.
Chp. 7 Rotational Motion. Rotational Motion When an object spins or moves about an axis of rotation it has rotational motion. Ɵ Ɵ = S = angular displacement.
Uniform Circular Motion. Acceleration When an object moves at a constant speed in a circular path, it is constantly changing direction – accelerating.
Chapter 10 Rotational Motion.
Chapter 7 Rotational Motion and The Law of Gravity.
Lecture 15: Rotational Motion. Questions of Yesterday 1) A piece of clay traveling north with speed v collides perfectly inelastically with an identical.
Phys 250 Ch5 p1 Rotational Motion: in close analogy with linear motion (distance/displacement, velocity, acceleration) Angular measure in “natural units”
Chapter 8 Rotational Motion.
Proportionality between the velocity V and radius r
Uniform Circular Motion the motion of an object traveling in a circular path an object will not travel in a circular path naturally an object traveling.
Chapter 7 Rotational Motion and The Law of Gravity.
Chapter 5 Circular Motion. MFMcGraw-PHY 1401Ch5b-Circular Motion-Revised 6/21/ Circular Motion Uniform Circular Motion Radial Acceleration Banked.
Chapter 7: Rotational Motion and the Law of Gravity Angular Speed & Acceleration  A unit of angular measure: radian y x P r  s = r  where s,r in m,
Circular Motion Physics Mr. Padilla. Rotation and Revolution Both rotation and revolution occur by an object turning about an axis. Rotation - The axis.
Circular Motion and Other Applications of Newton’s Laws
Chapter 7 Circular Motion. Chapter Objectives Relate radians to degrees Calculate angular quantities such as displacement, velocity, & acceleration Differentiate.
Concept Summary. Circular Motion Terms  The point or line that is the center of the circle is the axis of rotation.  If the axis of rotation is inside.
In mathematics and physics, a specific form of measurement is used to describe revolution and fractions of revolutions. In one revolution, a point on.
Alta High Conceptual Physics Chapter 9 Circular Motion.
Section 7-1 Circular Motion Acceleration can be produced by a change in magnitude of the velocity and/or by a change in ____________________ of the velocity.
Chapter 7 Rotational Motion and the Law of Gravity.
Ying Yi PhD Chapter 7 Rotational Motion and the Law of Gravity 1 PHYS HCC.
Chapter 7 Rotational Motion and The Law of Gravity.
Centripetal Force Copyright Sautter 2003.
Basic Mechanics. Units Velocity and Acceleration Speed: Time rate of change of position. Velocity: Speed in a specific direction. Velocity is specified.
Chapter 7: Rotational Motion and the Law of Gravity.
Circular Motion Chapter 12.
Circular Motion.
Circular Motion Unit
Presentation transcript:

Chapter 7 Rotational Motion and the Law of Gravity

7–1 Measuring Rotational Quantities

Rotational Motion Motion of a body that spins about an axis.

Axis of rotation Is the line about which the rotation occurs.

Angles can be measured in radians (rads). Radians – an angle whose arc length is equal to its radius, which approximately equal to 57.3 degrees.

1 radian = 57.3 o s  = ---- r

1 radian = 57.3 o s  = ---- r s = arc length r = length of radius  = angle of rotation

The angle of 360 o is one revolution. (1 rev = 360 o ) One revolution is equal to the circumference of the circle of rotation.

Circumference is 2  r so, 1 rev = 360 o = 2  rads Radius is half the diameter (d).

Angular Displacement (  ) The angle through which a point, line, or body is rotated in a specified direction and about a specified axis.

Describes how far an object has rotated. Change Angular in arc length Displacement = radius

Counterclockwise (CCW) rotation is considered (+) Clockwise (CW) rotation is considered (-)

Ex 1: John Glenn, in 1962, circled the earth 3 times in less than 5 hours. If his distance from the center of the earth was 6560 km, what arc length did he travel through?

G:  = 3 rev = 6  rads, r = 6560km U:  s = ? E:  s =  r S:  s = (6  )(6560) S:  s = km

Angular Speed  The rate at which a body rotates about an axis, usually expressed in radians per second. (rads/sec)

Angular Average displacement Angular = Speed time interval

Ex 2: In 1975, an ultra-fast centrifuge attained an average angular speed of 2.65 x 10 4 rads/sec. What was the angular displacement after 1.5 sec?

G:  avg = 2.65 x 10 4 rads/sec,  t = 1.5 sec U:  = ? E:  =  avg  t S:  = (2.65 x 10 4 )(1.5) S:  = radians

How fast is the earth rotating? The Earth rotates at a moderate angular velocity of ×10 -5 rads/s

Ex 3: A water supply tunnel in NYC is 1.70 x 10 5 m long and a radius of 2 m. If an electronic eye sensor moves around the perimeter of the tunnel at an average angular speed of 5.9 rads/sec. How long will it take the beetle to travel the equivalent of the length of the tunnel?

G:  avg = 5.9 rads/sec, r = 2 m,  s = 1.70 x 10 5 m U:  t = ? E:  t =  /  avg We need to find .

 =  s / r  = 1.70 x 10 5 m / 2 m  = rads

S:  t = rads 5.9 rads/sec

S:  t = rads 5.9 rads/sec S:  t = sec

Angular Acceleration  The time rate of change of angular speed, expressed in rads/sec 2.

 f  i   t

 f  final angular speed  i  initial angular speed  angular acceleration  t = elapsed time

Equation is rearranged just like the linear acceleration equation: ALWAYS multiply by ‘  t’ first! Then isolate what you are looking for.

Ex 4: A brake is applied to a flywheel for 5 seconds, reducing the angular velocity of the wheel uniformly from 2.2 rads/sec to 1.8 rads/sec. What is the angular acceleration?

G:  t = 5 sec,  2  rads/sec, and  1  rads/sec U:  E:  2  1   t

1.8 rads/sec – 2.2 rads/sec  = sec  = rads/sec 2

In comparing angular and linear quantities, they are similar. LinearAngular Rotational Displacement  x (m)  rads  Velocity v (m/s)  rads/s  Acceleration a  m/s 2  rads/s 2 

Looking back to Ch 2 equations:  x = v i  t + ½ a  t 2  x = ½ (v i + v f )  t v f = v i + a  t v f 2 = v i 2 + 2a  x

We apply angular notation to these equations and get:  =  i  t + ½   t 2  = ½ (  i +  f )  t  f =  i +  t  f 2 =  i 

Ex 5: A wheel on a bike moves through 11.0 rads in 2 seconds. What is the angular acceleration of the initial angular speed is 2.0 rads/sec?

G:  = 11 rads,  t = 2 sec,  i = 2 rads/sec U:  = ? E:  =  i  t + ½  t 2  = 2(  i  t) /  t 2 S:  = 2[11 – (2)(2)] /2 2 S:  = 3.5 rads/sec 2

7-2 Tangential and Centripetal Acceleration

Objects in motion have a tangential speed. Tangent – a line that lies in a plane of circle that intersects at one point.

Tangent line

Tangential Speed (v t ) The instantaneous linear speed of an object directed along the tangent to the object’s path.

r = distance from axis  = angular speed v t = tangential speed

Ex 6: The radius of a CD is 0.06 m. If a microbe riding on the disc’s rim has a tangential speed of 1.88 m/s, what is the microbe’s angular speed?

G: r =0.06 m, v t =1.88 m/s U:  = ? E:  = v t / r S:  = 1.88 m/s / 0.06 m S:  = 31.3 rads/sec

Tangential Acceleration (a t ) The instantaneous linear acceleration of an object directed along the tangent to the objects circular path

a t = tangential acceleration r = distance from axis  = angular acceleration

Ex 7: To ‘crack’ a whip requires its tip to move at supersonic speed. This was achieved with a whip m. If the tip moved in a circle and it accelerated from 6.0 rads/sec to 6.3 rads/sec in 0.6 sec. What would the tangential acceleration be?

G: r =56.24 m,  t =0.6 sec  i = 6 rads/sec,  f = 6.3 rads/sec, U: a t = ? E: a t = r 

We need to find angular acceleration (a) E:  f  i  t

S:   0.6 S:  rads/sec 2

S: a t = (56.24)(0.5) S: a t = m/s 2

Centripetal Acceleration (a c ) Acceleration directed toward the center of a circular path.

r = distance from axis (m) a c = centripetal accel. (m/s 2 ) v t = tangential speed (m/s)

r = distance from axis (m) a c = centripetal accel. (m/s 2 )  = angular speed (rads/sec)

Ex 8:Calculate the orbital radius of the Earth, if its tangential speed is 29.7 km/s and the centripetal acceleration acting on the Earth is 5 x m/s 2 ?

G: v t =29.7 km/s = m/s a c = 5 x m/s 2 U: r = ? E: v t 2 r = ---- acac

S: r = x S: r =1.764 x m

Tangential and centripetal accelerations are perpendicular. acac atat a total

The total acceleration can be found by using the Pythagorean Theorem.

If you need to find the angle  use the inverse tangent function (tan -1 )

7-3 Causes of Circular Motion

If a mass undergoes an acceleration, there must be a force causing it. (Newton’s 2 nd Law)

A force directed toward the center is necessary for circular motion.

This force causing circular motion is called Centripetal Force (F c ) r m v FcFc

With a centripetal force, an object in motion will be accelerated and change its direction.

Work Done by the Centripetal Force Since the centripetal force on an object is always perpendicular to the object’s velocity, the centripetal force never does work on the object - no energy is transformed.

Without a centripetal force, an object in motion continues along a straight- line path.

“Centrifugal Force  “centrifugal force” is a fictitious force - it is not an interaction between 2 objects, and therefore not a real force. Nothing pulls an object away from the center of the circle.

“Centrifugal Force” What is erroneously attributed to “centrifugal force” is actually the action of the object’s inertia - whatever velocity it has (speed + direction) it wants to keep.

From Newton’s 2 nd Law F = ma F c = ma c

From Newton’s 2 nd Law F = ma F c = ma c

From Newton’s 2 nd Law F = ma F c = ma c

Ex 9: Joe attaches a 0.5 kg mass to a 1m rope. Joe swings the rope in a horizontal circle above his head with a speed of 4 m/s. What force is exerted to keep the mass moving in a circle?

G:m = 0.5 kg v t = 4 m/s r = 1 m U: F c = ? E:F c = m(v t 2 / r)

S: F c =.5 kg x(4 m/s) 2 /(1 m) S: F c = 8 N

Gravitational Force The mutual force of attraction between particles of matter.

This is a field force that always exists between any two objects, regardless of their sizes.

The gravitational force (F g ) depends upon the distance between the two masses.

Newton’s Law of Universal Gravitation

m 1 = mass 1 (kg) m 2 = mass 2 (kg) r = distance between center of masses. (m) G = Constant of Universal Gravitation.

Units will cancel out with others leaving just force units of Newtons (N).

The universal gravitational constant (G) can be used to find the gravitational force between any two particles.

This is what is known as the inverse-square law. The force between the two masses decreases as the masses move farther apart.

The acceleration due to gravity, ‘g’, decreases with distance from the earth’s center as 1/d 2.

As an object moves away from the center of the Earth, by a distance equivalent to the earth’s radius.

Distance Force of Gravity RERE FgFg 2 R E 1/4 F g 3 R E 1/9 F g 4 R E 1/16 F g 5 R E 1/25 F g

Ex 10: What is the force of attraction between Adam and Jason, gravitational of course. If they are 12 m apart and Jason mass is 82 kg and Adam is 74 kg.

G: m 1 = 82 kg, m 2 = 74kg, r = 12 m, G = 6.673x n-m 2 /kg 2 U: F g = ?

G: m 1 = 82 kg, m 2 = 74kg, r = 12 m, G = 6.673x n-m 2 /kg 2 U: F g = ? E:

S: F g = 2.81 x N

Ex 11: The sun has a mass 2 x kg and a radius of 7 x 10 5 km. What mass must be located on the sun’s surface for gravitational force of 470 N to exist between the mass and the sun?

G: m 1 = 2 x kg, r =7 x 10 5 km=7 x 10 8 m G = 6.673x n-m 2 /kg 2 F g = 470 N U: m 2 = ?

E:

S: m 2 = 1.7 kg

PlanetRadius (m)Mass (kg)g (m/s 2 ) Mercury2.43 x x Venus6.073 x x Mars3.38 x x Jupiter6.98 x x Saturn5.82 x x Uranus2.35 x x Neptune2.27 x x Pluto1.15 x x