More Fun with Newton’s Laws Friction, Inclined Planes, N.T.L.

Slides:



Advertisements
Similar presentations
Friction & Inclined Planes
Advertisements

Newton’s First & Second Law
Newton’s Laws - continued
FORCE A force is any influence that can change the velocity of a body. Forces can act either through the physical contact of two objects (contact forces:
Newton’s Laws of Motion and Free Body Analysis
Chapter 5 – Force and Motion I
 The force that act on the object are balanced in all direction.  The force cancel each other, so that the resultant force or net force is zero.  Newton’s.
1 Chapter Four Newton's Laws. 2  In this chapter we will consider Newton's three laws of motion.  There is one consistent word in these three laws and.
Normal Force Force on an object perpendicular to the surface (Fn)
Newton’s Laws.
Sliding Friction A force that opposes motion Acts parallel to the
Forces in Two Dimensions - Objectives 1.Addition of ForcesAddition of Forces 2.Resolution of ForcesResolution of Forces 3.Equilibrium and StaticEquilibrium.
Constant Force Motion and the Free Body Diagram Teacher Excellence Workshop June 19, 2009.
Instructor: Dr. Tatiana Erukhimova
Newton’s First & Second Law AP Physics C. Unit is the Newton(N) or pound (lb) Is by definition a ….. push or a pull Can exist during physical contact.
Friction Level 1 Physics. TWO types of Friction Static – Friction that keeps an object at rest and prevents it from moving Kinetic – Friction that acts.
Newton’s Laws - continued
College Physics, 7th Edition
Newton’s Laws.
Aim: More Law of Inertia
Newton’s Laws The Study of Dynamics.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 13, 14, 15.
Newton’s Laws - continued Friction, Inclined Planes, N.T.L., Law of Gravitation.
SECOND LAW OF MOTION If there is a net force acting on an object, the object will have an acceleration and the object’s velocity will change. Newton's.
Newton’s Laws - continued Friction, Inclined Planes, N3L, Law of Gravitation.
Dynamics of force and motion
PAP Physics. Unit is the NEWTON(N) Is by definition a push or a pull Can exist during physical contact (Tension, Friction, Applied Force) Can exist with.
1 Some application & Forces of Friction. 2 Example: When two objects of unequal mass are hung vertically over a frictionless pulley of negligible mass,
Newton’s First Law Honors Physics. Net force – combination of all forces acting on an object. (F net ) Balanced forces – forces that are equal in magnitude.
Frictional Forces  Two types: - static – applies to stationary objects - kinetic – applies to sliding (moving) objects  Like F N, the Frictional Force.
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.
Aim: More Atwood Machines Answer Key HW 6 Do Now: Draw a free-body diagram for the following frictionless inclined plane: m2m2 m1m1 M θ Mg m2m2 m1m1 M.
Ch 4 – Forces and the Laws of Motion. What is a force? A force is a push or pull A force causing a change in velocity –An object from rest starts moving.
Free Body diagrams and problem solving
Friction. Biblical Reference And they pulled him up with the ropes and lifted him out of the cistern. Jeremiah 38:13.
AP Physics 1 – DYNAMICS OF FORCE AND MOTION NEWTON’S THIRD LAW & MORE FRICTION! (IT’S BACK!)
Newton’s First & Second Law AP Physics C. Unit is the NEWTON(N) Is by definition a push or a pull Can exist during physical contact(Tension, Friction,
Multiple Object Systems 1. Analyze the system as one object. 2. Analyze each object individually. 3. Create multiple equations to solve for multiple unknowns.
Aim: How do we explain the force of friction?. Visualizing Friction.
CP Physics Chapter 4 Newton’s Laws Force Force (F) is a push or a pull Measured in Newtons (N) for SI, pounds (lb) in US. (4.45 N = 1 lb) It has magnitude.
Chapter 4 Dynamics: Aim: How can we describe Newton’s Laws of Motion? © 2014 Pearson Education, Inc.
Weight = mass x acceleration due to gravity
1 Newton’s Third Law Readings: Chapter 8. 2 Newton’s Third Law When you have more than 1 system the Newton’s Third Law can provide an additional information.
Inclined Plane Problems. Axes for Inclined Planes X axis is parallel to the inclined plane Y axis is perpendicular to the inclined plane Friction force.
4-8 Applications Involving Friction, Inclines
Force Problems. A car is traveling at constant velocity with a frictional force of 2000 N acting opposite the motion of the car. The force acting on the.
Raymond A. Serway Chris Vuille Chapter Four The Laws of Motion.
-A force that opposes motion -Acts parallel to the surfaces in contact.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures
Unit is the NEWTON(N) Is by definition a push or a pull Can exist during physical contact(Tension, Friction, Applied Force) Can exist with NO physical.
NEWTON'S LAWS OF MOTION Philosophiae Naturalis Principia Mathematica (1686)
Friction & Inclined Planes
Newton’s Laws - continued
More Fun with Newton’s Laws
Newton’s Laws - continued
Newton’s Laws - continued
Forces of Friction When an object is in motion on a surface or through a viscous medium, there will be a resistance to the motion This is due to the interactions.
Newton’s Laws - continued
Friction & Inclined Planes
Newton’s Laws - continued
Newton’s Laws - continued
Newton’s Laws - continued
Newton’s Laws - continued
Newton’s Laws - continued
Newton’s Laws - continued
Newton’s Laws - continued
Newton’s Laws - continued
Newton’s 3rd Law and Law of Gravitation
Presentation transcript:

More Fun with Newton’s Laws Friction, Inclined Planes, N.T.L.

TWO types of Friction Static – Friction that keeps an object at rest and prevents it from moving Kinetic – Friction that acts during motion

Force of Friction The Force of Friction is directly related to the Force Normal. Mostly due to the fact that BOTH are surface forces Note: Friction ONLY depends on the MATERIALS sliding against each other, NOT on surface area. The coefficient of friction is a unitless constant that is specific to the material type and usually less than one.

Example A 1500 N crate is being pushed across a level floor at a constant speed by a force F of 600 N at an angle of 20° below the horizontal as shown in the figure. a) What is the coefficient of kinetic friction between the crate and the floor? mg FNFN FaFa 20 FfFf F ay F ax

Example 2: Angled force with acceleration If the 600 N force is instead pulling the block at an angle of 20° above the horizontal as shown in the figure, what will be the acceleration of the crate. Assume that the coefficient of friction is still mg FNFN FfFf 20 FaFa F ax F ay

Example 2: Angled force with acceleration If the 600 N force is instead pulling the block at an angle of 20° above the horizontal as shown in the figure, what will be the acceleration of the crate. Assume that the coefficient of friction is still mg FNFN FfFf 20 FaFa F ax F ay

Inclines mg  FNFN FfFf      Tips Rotate Axis Break weight into components Write equations of motion or equilibrium Solve

Example m2m2 m1m1 Masses m 1 = 4.00 kg and m 2 = 9.00 kg are connected by a light string that passes over a frictionless pulley. As shown in the diagram, m 1 is held at rest on the floor and m 2 rests on a fixed incline of angle 40 degrees. The masses are released from rest, and m 2 slides 1.00 m down the incline in 4 seconds. Determine (a) The acceleration of each mass (b) The coefficient of kinetic friction and (c) the tension in the string. T T 40

Example m2m2 m1m1 Masses m 1 = 4.00 kg and m 2 = 9.00 kg are connected by a light string that passes over a frictionless pulley. As shown in the diagram, m 1 is held at rest on the floor and m 2 rests on a fixed incline of angle 40 degrees. The masses are released from rest, and m 2 slides 1.00 m down the incline in 4 seconds. Determine (a) The acceleration of each mass (b) The coefficient of kinetic friction and (c) the tension in the string. m1gm1g m2gm2g FNFN T T FfFf 40 m 2 gcos40 m 2 gsin40

Example

Newton’s Third Law “For every action there is an EQUAL and OPPOSITE reaction. This law focuses on action/reaction pairs (forces) They NEVER cancel out All you do is SWITCH the wording! PERSON on WALL WALL on PERSON

N.T.L This figure shows the force during a collision between a truck and a train. You can clearly see the forces are EQUAL and OPPOSITE. To help you understand the law better, look at this situation from the point of view of Newton’s Second Law. There is a balance between the mass and acceleration. One object usually has a LARGE MASS and a SMALL ACCELERATION, while the other has a SMALL MASS (comparatively) and a LARGE ACCELERATION.

N.T.L Examples Action: HAMMER HITS NAIL Reaction: NAIL HITS HAMMER Action: Earth pulls on YOU Reaction: YOU pull on the earth

An interesting friction/calc problem…YUCK! Suppose you had a 30- kg box that is moving at a constant speed until it hits a patch of sticky snow where it experiences a frictional force of 12N. a) What is the acceleration of the box? b) What is the coefficient of kinetic friction between the box and the snow? mg FNFN FfFf 0.4 m/s/s 0.04

The “not so much fun” begins…. Now suppose your friend decides to help by pulling the box across the snow using a rope that is at some angle from the horizontal. She begins by experimenting with the angle of pull and decides that 40 degrees is NOT optimal. At what angle, , will the minimum force be required to pull the sled with a constant velocity? mg FNFN FfFf  F Let’s start by making a function for “F” in terms of “theta” using our equations of motion. Fcos  Fsin 

What does this graph look like? ThetaForce Does this graph tell you the angle needed for a minimum force?

What does this graph look like? thetaForce Could this graph tell you the angle needed for a minimum force? What do you notice about the SLOPE at this minimum force?

Taking the derivative Here is the point. If we find the derivative of the function and set the derivative equal to ZERO, we can find the ANGLE at this minimum. Remember that the derivative is the SLOPE of the tangent line. The tangent line’s slope is zero at the minimum force and thus can be used to determine the angle we need. This tells us that our minimum force is somewhere between 2 & 3 degrees.

Taking the derivative using the Chain Rule Derivative of outside function Leave inside function alone Derivative of inside function

Taking the derivative using the Chain Rule Now we set the derivative equal to ZERO and solve for theta!

Setting the derivative equal to zero 2.29 °