Chapter 5 Applications of Newton’s Law

Slides:



Advertisements
Similar presentations
Uniform circular motion: examples include
Advertisements

Newton’s Laws of Motion and Free Body Analysis
CBA #1 Review Graphing Motion 1-D Kinematics Projectile Motion Circular Motion Gravity Graphing Motion 1-D Kinematics Projectile Motion Circular.
Normal Force Force on an object perpendicular to the surface (Fn)
Applications of Newton’s Laws
As the ball revolves faster, the angle increases
Forces and the Laws of MotionSection 4 Click below to watch the Visual Concept. Visual Concept Everyday Forces.
Lecture 14 Monday, September 29 Using Newton’s Laws.
Applications of Newton’s Laws
 Calculate the acceleration that this object experiences 30 kg 150 N.
Inclined Plane Problems
A 6. 0-kg object undergoes an acceleration of 2. 0 m/s2
FRICTION!.
4.1 Resistance in Mechanical Systems
Chapter 3 Forces.
Chapter 5 Newton’s Second Law of Motion – Force and Acceleration
CHAPTER 3. Newton’s Second Law of Motion F = m × a Force = mass × acceleration The faster you run into a wall, the more force you exert on that wall Units.
Newton’s Laws of Motion 1. If the sum of all external forces on an object is zero, then its speed and direction will not change. Inertia 2. If a nonzero.
Newton’s Second Law of Motion. Force and Acceleration Force is a push or a pull acting on an object. Acceleration occurs when the VELOCITY of an object.
Chapter 4 Forces and the Laws of Motion. Newton’s First Law An object at rest remains at rest, and an object in motion continues in motion with constant.
Chapter 4 Dynamics: Newton’s Laws of Motion
CHAPTER 4 FORCES IN 1-D FORCE Force is anything which causes a body to start moving when it is at rest, or stop when it is moving, or deflect once it.
Circular Motion Uniform circular motion: examples include Objects in orbit (earth around the sun Driving a car around a corner Rotating a ball around on.
Newton’s Second Law of Motion. Newton’s Second Law Newton’s Second Law of Motion- Acceleration depends on the objects mass and the net force acting on.
Physics 207: Lecture 11, Pg 1 Lecture 11 l Goals:  Employ Newton’s Laws in 2D problems with circular motion  Relate Forces with acceleration Assignment:
Remember!!!! Force Vocabulary is due tomorrow
Advanced Physics Chapter 4 Motion and Force: Dynamics.
Friction Ffriction = μFNormal.
Friction What is friction?. Answer Me!!! Think of two factors that affect friction.
Newton’s Second Law of Motion – Force & Acceleration
Announcement Exam 1 Next Thursday –Rooms CR 302 and 306.
The tendency of objects to resist change in their state of motion is called inertia  Inertia is measured quantitatively by the object's mass.  Objects.
 Friction – force that opposes motion  Caused by microscopic irregularities of a surface  The friction force is the force exerted by a surface as an.
Homework Read pages 96 – 101 Answer practice problems
Chapter 3. Force, Mass, and Acceleration Newton’s first law of motion states that the motion of an object changes only if an unbalanced force acts on.
Chapter 3 Newton’s 1st Law of Motion Inertia. Net Forces cause changes in motion.
Chapter 4 Review. Question What is the SI unit of force?
 Gravity is 9.8 or ~10 m/s 2  If dropped from rest: y = -½ gt 2.
Newton’s Laws. Newton’s First Law: The Law of Inertia An object at rest will stay at rest unless acted upon by a force, and an object in motion will stay.
“Law of Acceleration” Forces can be BALANCED or UNBALANCED Balanced forces are equal in size (magnitude) and opposite in direction UNbalanced.
NEWTON'S LAWS OF MOTION Philosophiae Naturalis Principia Mathematica (1686)
Dynamics: Newton’s Laws of Motion
Newton’s Second Law Continued
Forces in Nature.
Aristotle 4th Century Natural Motion Up or down Violent Motion
M Friction.
Forces Chapter 3.
Chapter 5 Applications of Newton’s Law
2. Positive and negative work
Intro problem (p.145 #1-2, p.147 #1-4)
Chapter 5:Using Newton’s Laws: Friction, Circular Motion, Drag Forces
Frictional Forces.
Newton’s Laws Acceleration
Forces.
Forces.
Friction is one of the most important opposing forces.
Objectives Chapter 4 Section 4 Everyday Forces
More Friction.
Uniform Circular Motion
Circular Motion Uniform circular motion: examples include
CHAPTER 4 FORCES IN 1-D.
Gravity: A force with which to be reckoned.
Newton’s Laws of Motion Chapters 2,3,6,7
Aim: How do we explain motion along an inclined plane?
1. A ball of mass m is suspended from two strings of unequal length as shown above. The magnitudes of the tensions T1 and T2 in the strings must satisfy.
Forces.
Forces FORCEMAN.
Motion on Inclined Planes
Chapter 3 Forces.
Circular Motion and Other Applications of Newton’s Laws
Presentation transcript:

Chapter 5 Applications of Newton’s Law

2d equilibrium Find the tensions in terms of the mass m of the engine.

Tension

Static friction vs Kinetic friction

Static Friction Kinetic friction is the friction when the object is moving. Static friction is when it is at rest.

Example: Incline It is found that the object starts sliding once the angle θ becomes greater than θc. Find μs in terms of θc.

Kinetic Friction (more useful) Kinetic friction is the friction when the object is moving. Static friction is when it is at rest.

Example Find the horizontal acceleration of the box of 3kg on a surface given μk = 0.5 and F = 20N.

Pulling a crate Given mg =500N and μk=0.4. How hard do you have to pull to keep the crate moving at constant velocity?

Solution

The Sliding Crate Find the acceleration given θ =30°, μk=0.192.

Centripetal force and acceleration According to Newton’s Laws, anything that is not moving in a straight line must have a net force acting on it and must be accelerating. When an object is moving in a circle, there must be a net force, causing the “centripetal acceleration”. Even though the speed of the object is constant, the velocity is constantly changing because of the changing direction. That is why the acceleration is non-zero. r v x y (x,y)

Centripetal force and acceleration

Must remember this: Using this you can convert freely among ω, T, f and v.

Centripetal force and acceleration

Centripetal force and acceleration Centripetal force is the force required to keep an object in circular motion. Without it the object will resume moving in a straight line. In this case, the centripetal force is the tension in the string.

How fast can it spin? The cord breaks when tension is greater than 50N. Given m=0.5kg, r =1.5m, how fast can it spin? In this case, the centripetal force is the tension in the string. What is the tension when v =7m/s?

Examples of centripetal force

Gravity as centripetal force In this case, the gravitational force (i.e. the weight) is the centripetal force. However, you must remember that in outer space, g <9.8m/s2!!! The value of g (acceleration under free fall) is usually given, and you will also learn how to calculate it in Chapter 13.

What you have learned Static and kinetic friction Centripetal force and acceleration