USSC2001 Energy Lecture 1 Coordinates and Kinematics Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore.

Slides:



Advertisements
Similar presentations
Kinematics The branch of mechanics that studies the motion of a body without caring about what caused the motion.
Advertisements

Kinematics of Particles
Objectives Describe motion in terms of frame of reference, displacement, time, and velocity. Calculate the displacement of an object traveling at a known.
USSC2001 Energy Lecture 2 Kinetic Energy in Motion Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore.
© 2013 Pearson Education, Inc. Chapter Goal: To learn how to solve problems about motion in a straight line. Chapter 2 Kinematics in One Dimension Slide.
Physics 111: Mechanics Lecture 09
Physics 106: Mechanics Lecture 01
1 AP Physics Chapter 2 Motion Along a Straight Line.
Motion Along a Straight Line
Unit 8 POE Ballistic Device
USSC2001 Energy Lecture 2 Elastic Energy and Work Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore.
Chapter 2 Preview Objectives One Dimensional Motion Displacement
Chapter 2 Motion in One Dimension. Kinematics Describes motion while ignoring the agents that caused the motion For now, will consider motion in one dimension.
Chapter 2 Motion Along a Straight Line. Linear motion In this chapter we will consider moving objects: Along a straight line With every portion of an.
Motion of an object is the continuous change in the position of that object. In this chapter we shall consider the motion of a particle in a straight.
Motion in One Dimension
Chapter 2 Table of Contents Section 1 Displacement and Velocity
Fundamental Concepts and Principles
Chapter 11 Angular Momentum.
PHYSICS MR BALDWIN Speed & Velocity 9/15/2014
Problems Ch(1-3).
Ch 2. Motion in a Straight Line Definitions 1. Kinematics - Motion Kinetic Energy - Energy associated with motion 2. Motion in physics is broken down.
Kinetic Energy, Work, Power, and Potential Energy
Kinetic Energy, Work, Power, and Potential Energy
General physics I, lec 1 1 Chapter (1,2). general physics I, lec 1 2 Physical quantities (in mechanics) Basic quantities : in mechanics the three fundamental.
Chapter 10 Rotation of a Rigid Object about a Fixed Axis.
MA4248 Weeks 1-3. Topics Coordinate Systems, Kinematics, Newton’s Laws, Inertial Mass, Force, Momentum, Energy, Harmonic Oscillations (Springs and Pendulums)
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu To View the presentation as a slideshow with effects select “View”
Professional Development Series June 18, 2005 The Physics of Tops presented by Luis A. Martínez-Pérez, Ph.D. Associate Professor Science Education Florida.
Problems Ch(1-3).
© Houghton Mifflin Harcourt Publishing Company The student is expected to: Chapter 2 Section 1 Displacement and Velocity TEKS 4A generate and interpret.
One Dimensional Kinematics: Problem Solving Kinematics in Two-Dimensions: Law of Addition of Velocities Projectile Motion 8.01 W02D1.
Chapter 3 Acceleration Lecture 1
Chapter 2 Motion in One Dimension. Kinematics Describes motion while ignoring the external agents that might have caused or modified the motion For now,
Two-Dimensional Rotational Kinematics 8.01 W09D1 Young and Freedman: 1.10 (Vector Products) , 10.5.
motiontranslationaverage speed Rotation kinematics center of mass Center of gravity gravitational force Gravity displacement direction Vector quantity.
Distance is the space between two points, commonly measured in metres (m). Distances between two points can depend on the path taken. Time (t) is the duration.
Chapter 10 Rotational Motion.
USSC3002 Oscillations and Waves Lecture 10 Calculus of Variations Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science.
USSC2001 Energy Lecture 2 Kinetic Energy in Motion Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore.
© Houghton Mifflin Harcourt Publishing Company Preview Objectives One Dimensional Motion Displacement Average Velocity Velocity and Speed Interpreting.
USSC3002 Oscillations and Waves Lecture 10 Calculus of Variations Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science.
USSC2001 Energy Lecture 2 Kinetic Energy in Motion Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore.
In chapter 1, we talked about parametric equations. Parametric equations can be used to describe motion that is not a function. If f and g have derivatives.
POSITION AND COORDINATES l to specify a position, need: reference point (“origin”) O, distance from origin direction from origin (to define direction,
As a first step in studying classical mechanics, we describe motion in terms of space and time while ignoring the agents that caused that motion. This.
Kinematics The branch of mechanics that studies the motion of a body without caring about what caused the motion.
Chapter 11 Angular Momentum. The Vector Product and Torque The torque vector lies in a direction perpendicular to the plane formed by the position vector.
USSC2001 Energy Lecture 1 Potential and Kinetic Energy Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore.
Monday January 26, 2004PHYS , Spring 2004 Dr. Andrew Brandt 1 PHYS 1443 – Section 501 Lecture #2 Monday January 26, 2004 Dr. Andrew Brandt Chapter.
Chapter 2 Motion Along a Straight Line 2-0. Mathematical Concept 2.1. What is Physics? 2.2. Motion 2.3. Position and Displacement 2.4. Average Velocity.
Motion Along a Straight Line Chapter 3. Position, Displacement, and Average Velocity Kinematics is the classification and comparison of motions For this.
Part 2 Kinematics Chapter 3 Vectors and Two-Dimensional Motion.
Branches of Physics. Study of how things move without considering the cause of motion. This branch of physics only deals with describing how something.
Ying Yi PhD Chapter 3 Kinematics in Two Dimension 1 PHYS HCC.
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.
Section 1 Displacement and Velocity Chapter 2 One Dimensional Motion To simplify the concept of motion, we will first consider motion that takes place.
Physics 1: Mechanics Đào Ngọc Hạnh Tâm Office: A1
The student is expected to:
How to Use This Presentation
Motion In Two-Dimensional
Chapter 3 Kinetics in Two or Three Dimensions, Vectors (1 week)
Motion Along a Straight Line
Section 1 Displacement and Velocity
Chapter 2 Table of Contents Section 1 Displacement and Velocity
Motion in One Dimension
Section 1 Displacement and Velocity
Physics 111: Mechanics Lecture 2
Fundamentals of Physics School of Physical Science and Technology
Presentation transcript:

USSC2001 Energy Lecture 1 Coordinates and Kinematics Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore Tel (65)

CONTENTS The material in these five lectures is based on chapters 1-8 and chapter 38 of the magnificent textbook titled: Fundamentals of Physics by Halliday, Resnick, and Walker, Sixth Edition, extended, John Wiley & Sons, Inc. Singapore, Lecture 1: physical quantities, measurement and invariance, rulers and clocks and scales, units, changing units using conversion factors, motion along a straight line, average and instantaneous velocity, acceleration, coordinate systems, vectors, change of coordinates, projectile and circular motion, relative motion

PHYSICAL QUANTITIES AND THEIR MEASUREMENTS Physics is based on measurements of quantities: e.g. length, time, mass, temperature, pressure and electric current, each of which is measured in its own units by comparison with a standard. Example. The length of a rod is the distance between two points chosen from opposite ends. The lengths of two rods can be compared by alignment. AA B B

RULERS AND INVARIANCE Question: Why can the lengths of two rods be compared using alignment? Answer: Because the length of a rod does not change when the rod is translated and rotated. The length of a rod, or more generally the set of distances between pairs of fixed points on a rigid body, provides a ruler for measuring lengths because these distances are invariant under translations and rotations

GEOMETRY Question: How can the midpoint of a rod be found? Answer: Use a ruler and compass ABE C D Binary rulers can be built using this bisection method AB

TUTORIAL 1 1.In vufoil ‘GEOMETRY’, assume that length AC = length BC and length AD = length BD - prove angle XAE = angle XBE for X in {C, D} - prove that angle AEC = 90 degrees (hint: what is the sum of the interior angles in a triangle?) - compute length AE if length AB = 12m and length CE = 8m - in the binary ruler if length AB = 12m locate the point F so that length AF = 4m

GEOMETRY – THE LANGUAGE OF SCIENCE Physical objects/processes exist in space/time The philosopher Kant argued that space/time were so fundamental that conscious experience would be impossible without them (don’t leave home without them!) Geometry describes the structure of space\time, it is (indeed it must be) the language of science Geometric concepts – eg points, lines, are ‘a priori synthetic’ truths - facts that can not be derived

BASIC CONCEPTS ABOUT LINES Imagine a line L as a set of points in space Ifthen the set consists of two rays, each of which is connected If are distinct points then there exists a unique continuous real-valued function that satisfies intervalcan be translated into

COORDINATE SYSTEMS FOR LINES The choice of an ordered set of two distinct points on a line yields a coordinate system for the line Assume that (x,y) yields a coordinate system f and that (u,v) yields a coordinate system h Define r = f(v)-f(u), then |r| is the ratio of the length of the intervals [u,v] to the length of the interval [x,y] in any coordinate system and sign r is positive if and only if the intervals have the same orientation Furthermore

TUTORIAL 1 2. Two coordinate systems f, h are given for a line L such that for some pair (x,y) of distinct points in L f(x) = 312, f(y) = 512, h(x) = 125, h(y) = 290 Compute constants (real numbers) r and c such that f(p) = rh(p) + c, p in L Hint: derive and solve a system of two equations for r and c by choosing carefully certain values for the point p in the equation above

TWO ASPECTS OF TIME “When did it happen?” A point in time “What is its duration?” Distance between time points The duration of a process (that starts and finishes at points in time) is analogous to the length of a rod

CLOCKS AND INVARIANCE How can we compare two time durations that start at different times? Our duration-length analogy might provide a clue! Clue: Find a repeatable physical process whose start and finish are points in time. Examples: Sandclock, Pendulum, Spring

CLOCKS ARE COORDINATE SYSTEMS An ideal clock A assigns to each point p in L a real number, called its reading at p (in specified units), mathematically, we say that is a real-valued function with domain L, we often illustrate as below The geometry of time is that of a line in space, let us denote this line, whose points (in time), by L Here R denotes the set of real numbers

TUTORIAL 1 3. Three clocks A, B, C run at different (uniform) rates and have simultaneous readings, expressed in seconds, shown by the figure below? Express the readings of B and of C as functions of the reading of A. Hint: consider the previous tutorial problem A B C

CHANGING UNITS We can change the units in which physical quantities are expressed by using conversion factors – ratios of units that equal 1 Example How many seconds are there in 1 year ?

SCALES AND MASS MEASUREMENTS Masses of objects can be compared using a scale. Question: in which direction will the right side move ? A B Answer: up, down iff mass B mass A

TUTORIAL 1 4. The speed limit on a road in the United States is posted at 55 miles per hour. Compute the speed limit in units of meters per second? 5. Eight of nine coins have the same mass and one coin has more mass than the other coins. Describe how to determine the more massive coin by making two weighings using a perfect scale balance.

SYSTEMS OF UNITS SI (International System) of seven base units include: meter (m)– length or distance traveled by light in a vacuum during 1/ of a second second (s) – time taken by oscillations of the light (of a specified frequency) emitted by a cesium-133 atom kilogram (kg) – mass of a certain platinum-iridium cylinder These base units can be used to define derived units watt (W) - energy unit = (1 N) x (1 m) newton (N) – force unit =

TUTORIAL 1 6. We explained a geometric method to divide a ruler’s length by 2. Explain an approach to divide a clock’s duration by 2. Hint: what happens to the oscillation frequency of a pendulum if its length changes? What happens to an oscillator if its mass is changed? Devise a method to compute the ratio of the masses of two objects using a binary ruler and a scale with a movable top arm?

PLANAR AND SPATIAL COORDINATES Orthonormal coordinates can be constructed to represent points in a plane or in space by ordered pairs or ordered triplets of real numbers called coordinates Likewise, displacement vectors between ordered pairs of points can be represented by such pairs or triplets and the norm or magnitude of a vector defined as the distance between the points The Pythagorean theorem implies that the squared vector norm equals the sum of the squares of its coordinates

KINEMATICS A particle is an idealized object that has a location in space at each point in a specified time interval This means that a particles position in space is a function of its point in time Velocity vectors are the derivatives of these functions if time and space are given unit coordinate systems

MOTION IN ONE DIMENSION Consider a particle that moves along a line in space We can describe the time and the position of the particle using coordinates (clock and ruler) Then the particles position coordinate is a function of its time coordinate We can use analytic geometry to construct a plot of this function using orthonormal planar coordinates

MOTION IN ONE DIMENSION Consider a particle thrown upward from the ground We can use analytic geometry to construct a graph of this function using orthonormal planar coordinates

AVERAGE AND INSTANTANEOUS VELOCITIES The average velocity over the interval is the slope of the dotted line The instantaneous velocity at is the slope of the solid line and equals the derivative dh/dt evaluated at Tangent Secant

COMPUTING INSTANTANEOUS VELOCITIES The instantaneous velocity v(t) is computed using differential calculus If the graph of v is shown above

COMPUTING DISTANCE FROM VELOCITY The fundamental theorem of calculus says that h equals the signed area under the graph of v

ACCELERATION, VELOCITY, AND SPEED Acceleration is the derivative of velocity, therefore velocity is the integral of the acceleration, in the example on the preceeding page the accleration equals –g if the positive direction of height is measured away from the Earth, speed is the absolute value or magnitude of the velocity

TUTORIAL 1 7. Consider the preceeding example of motion in one dimension and - compute the value of time when the object is at a maximum height - explain why the average speed over the time interval is larger than the magnitude of the average velocity over the same interval - graph the possible velocity given air friction (to show the qualitative effect of the air friction)

MOTION IN TWO AND THREE DIMENSIONS Motion can be described coordinatewise, for Example: if the position of a particle moving in a plane is expressed as function of time using an orthonormal coordinate system Then its velocity, acceleration and speed are

TUTORIAL 1 8. A particle moves with constant speed 5 m/s along a path in a plane described in terms of orthonormal coordinates x,y by the equation Compute the two possible velocity vectors for the particle when its x coordinate equals A gun is fired directly at an object thrown directly upward when its height is maximum height. Show that the bullet will strikes the target unless it hits the ground before the object hits the ground (ignore air friction and assume that the ground is flat). 10. Compute the acceleration and speed of a particle moving in a circle of radius R and angle