Frequent Questions www site is at:

Slides:



Advertisements
Similar presentations
Motion in One Dimension
Advertisements

Physics: Principles with Applications, 6th edition
Describing Motion: Kinematics in One Dimension
Motion in One Dimension
Copyright © 2009 Pearson Education, Inc. PHY093 – Lecture 2a Motion with Constant Acceleration 1 Dimension 1.
Copyright © 2009 Pearson Education, Inc. PHY430 Lecture 3a – Kinematics in 1- Dimension.
Sect. 2-5: Motion at Constant Acceleration
Motion in One Dimension
Motion in One Dimension
Motion in One Dimension
Motion in One Dimension
Chapter 2 Motion in One Dimension. Quantities in Motion Any motion involves three concepts Displacement Velocity Acceleration These concepts can be used.
Chapter 2 Motion in One Dimension. Dynamics The branch of physics involving the motion of an object and the relationship between that motion and other.
Motion in One Dimension
Motion in One Dimension. The branch of physics involving the motion of an object and the relationship between that motion and other physics concepts Kinematics.
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.
Describing Motion. the study of motion motion is a change in position two branches Mechanics.
Acceleration 1D motion with Constant Acceleration Free Fall Lecture 04 (Chap. 2, Sec ) General Physics (PHYS101) Sections 30 and 33 are canceled.
Kinematics in One Dimension. Mechanics Kinematics (Chapter 2 and 3) The movement of an object itself Concepts needed to describe motion without reference.
Describing Motion: Kinematics in One Dimension
Kinematics Velocity and Acceleration. Motion Change in position of object in relation to things that are considered stationary Usually earth is considered.
Chapter 2 One Dimensional Kinematics
Motion in One Direction Chapter : Displacement and Velocity Main Objectives:  Describe motion in terms of frame of reference, displacement, time,
Describing Motion: Kinematics in One Dimension. Sub units Reference Frames and Displacement Average Velocity Instantaneous Velocity Acceleration Motion.
Chapter 2 Describing Motion: Kinematics in One Dimension.
Chapter 2: Kinematics in one Dimension Displacement Velocity Acceleration HW2: Chap. 2: pb.3,pb.8,pb.12,pb.22,pb.27,pb.29,pb.46 DUE on Wednesday, Sept.
Thursday, May 31, 2007PHYS , Summer 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 001 Lecture #3 Thursday, May 31, 2007 Dr. Jaehoon Yu One Dimensional.
Raymond A. Serway Chris Vuille Chapter Two Motion in One Dimension.
Motion with Constant Acceleration. Constant Acceleration In many practical situations: –The magnitude of the acceleration is uniform (constant) –The motion.
Chapter 2 Describing Motion: Kinematics in One Dimension.
Monday, Sept. 10, 2007 PHYS , Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #4 Monday, Sept. 10, 2007 Dr. Jaehoon Yu Acceleration.
Motion with Constant Acceleration. Constant Acceleration In many practical situations: –The magnitude of the acceleration is uniform (constant) –The motion.
Chapter 2 Homework #1 Questions: 4,6,7,9,10,13,18, 19 Problems: 1,2,3,6-9,13,14,19, 20,22,23,24 Due Sept 22 Quiz on Section 1-6 on Sept 22.
Chapter 3 Describing Motion: Kinematics in One Dimension.
Acceleration. Definition Any change in velocity is acceleration What are the possible causes of acceleration? Speeding up Slowing down Changing direction.
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 in One Dimension. Kinematics Describes motion while ignoring the external agents that might have caused or modified the motion (Dynamics.
Dynamics The branch of physics involving the motion of an object and the relationship between that motion and other physics concepts Kinematics is a part.
Introduction to Motion
Ch 2 Describing Motion: Kinematics in One Dimension
KINEMATICS ACCELERATION.
Describing Motion with Equations
Vectors and Linear Motion
ST.JOSEPH'S HIGHER SECONDARY SCHOOL
Motion in One Dimension
Chapter 2 Straight Line Motion
Chapter 2 Motion Along a Straight Line
PHYS 1441 – Section 002 Lecture #4
Chap. 2: Kinematics in one Dimension
Describing Motion: Kinematics in One Dimension
Chapter 2 Describing Motion: Kinematics in One Dimension
Motion with Constant Acceleration
Motion in One Dimension
Motion in One Dimension
Chapter 2 Describing Motion: Kinematics in One Dimension
Describing Motion: Kinematics in One Dimension
Introduction to Motion
Motion in One Dimension
Motion in One Dimension
ACCELERATION.
Unit 1b: Motion in One Dimension-Constant Acceleration
Introduction to Motion
Chapter 2 Describing Motion: Kinematics in One Dimension
Describing Motion: Kinematics in One Dimension
PHYS 1441 – Section 501 Lecture #2
Describing Motion: Kinematics in One Dimension
Kinematics in One Dimension
Presentation transcript:

Frequent Questions www site is at: http://nicadd.niu.edu/people/blazey/Physics_253_2006/Physics_253_2006.htm Problems, extra credit all due at the time of the test. Next test is Feb 7th, but is in your interests to keep up! 1/12/2019 Physics 253

Tips on how to do well redux! Read the material before lectures Listen in class, take notes sparingly Do the problems, these are key to understanding Read the material again after doing problems, this locks down the concepts Take advantage of the extra credit If you don’t understand, ask! 1/12/2019 Physics 253

How is lim(Dt0) Dx/Dt a derivative? 1/12/2019 Physics 253

Status: Unit 1, Chapter 2 Reference Frames and Displacement Average Velocity Instantaneous Velocity Acceleration Extending our tool kit to include change of velocity with respect to time Motion of Constant Acceleration A mathematical description of simple linear motion Contains many of the elements necessary to describe the kinematic world! Solving Problems Technique applies to many arenas Shows predictive aspect of physics. 1/12/2019 Physics 253

Acceleration Acceleration is a quantitative statement about how fast the velocity of an object is changing. Complete analog to velocity Instead of change of distance with respect to to time: We consider change of velocity with respect to time: The equation says it all: an object with changing velocity is accelerating. 1/12/2019 Physics 253

Average and Instantaneous Acceleration Average Acceleration Change in velocity divided by the time taken for the change A vector, for 1-D motion indicated by a plus or minus sign. Instantaneous Accel. Limiting value of the ave. accel. as time interval goes to zero. Again a derivative: this time of the velocity wrt to time! 1/12/2019 Physics 253

Example 1: Average Acceleration A car accelerates along Lincoln Highway from rest to 75m/hr in 5.0s. What is the average acceleration? Plug-and-chug! Which reads: “15 km/hr per second” Or on average the velocity changes 15 km/hr every second. Which is a statement of how fast the velocity changes with time. The mixed units are non standard much prefer 1/12/2019 Physics 253

Example 1: Average Acceleration A car accelerates along Lincoln Highway from rest to 75m/hr in 5.0s. What is the average acceleration? Plug-and-chug! Which reads: “15 km/hr per second” Or on average the velocity changes 15 km/hr every second. Which is a statement of how fast the velocity changes with time. The mixed units are non standard much prefer We’ll see later if you’d get a ticket 1/12/2019 Physics 253

Example 2: Average Acceleration An auto is moving to the right (+x) and the brakes are applied. If the initial velocity is 15.0 m/s and 5.0 s are required to slow down to 5.0 m/s what is the average acceleration? Note the negative sign appears because the final velocity is less than the initial velocity. The green arrows or vectors indicate velocity and the orange acceleration. 1/12/2019 Physics 253

Three comments on deceleration First, spelled with one “c”. Second, occurs whenever an object is slowing down. Third, occurs whenever velocity and acceleration point in opposite directions Consider, the following observations 5 seconds apart Even though the car is moving to the left because it’s slowing down it has positive acceleration 1/12/2019 Physics 253

Instantaneous Acceleration Defined as Limiting value of the ave. accel. as time interval goes to zero: Average acceleration is just the slope of the line connecting the points in the graph. As the time interval vanishes the line becomes the tangent to the curve. 1/12/2019 Physics 253

Instantaneous Acceleration Recall velocity was the derivative of position wrt time Similarly acceleration is the derivative of velocity wrt time v t P1 P2 P3 P4 1/12/2019 Physics 253

Acceleration as a second derivative 1/12/2019 Physics 253

Example: Acceleration A particle position along a straight line is given by: x = (2.10 m/s2 )t2 + 2.80 m. Calculate its average acceleration between t1 = 3.00 s and t2 = 5.00 instantaneous acceleration as a function of time. The velocity at time t is given by v=dx/dt= (4.20 m/s2)t, thus At t1 = 3.00s, v = (4.20m/s2)(3.0s) = 12.6 m/s At t2 = 5.00s, v = (4.20m/s2)(5.0s) = 21.0 m/s And, the average acceleration, 1/12/2019 Physics 253

Note the acceleration is constant and has no time dependence. Since velocity is v=dx/dt= (4.20 m/s2)t the acceleration is a = dv/dt = 4.20 m/s2 Note the acceleration is constant and has no time dependence. The three plots at the left show the time dependence of x, v and a. 1/12/2019 Physics 253

Average Speed Distance/Elapsed Time Velocity Average Velocity (Displacement/Elapsed Time) Instantaneous Velocity Acceleration Average Acceleration Instantaneous Accel. 1/12/2019 Physics 253

Motion at Constant Acceleration Ok now that we’ve got general (and actually quite rigorous) definitions of displacement, velocity, and acceleration we can derive equations of motion. Initially we’ll limit ourselves to constant acceleration, although not general, the resulting equations of motion are still extremely useful. For instance near the surface of earth the acceleration of gravity can be taken as a constant, thus we can easily describe the basic kinematics of falling objects. We’ll begin with a derivation of 1-dimensional equations and then move onto illustrative problems and later 2-dimensions. 1/12/2019 Physics 253

The Setup Assumptions: Notation: Motion in a straight line Constant acceleration  average and instantaneous acceleration are equal. Notation: Set initial time to zero. That is, t1 = 0. Start with “t-naught” not “t-one” x1  x0 and v1  v0 And we can simplify notation t2  t, x2  x, and v2  v 1/12/2019 Physics 253

Starting Point As a result And Since acceleration is assumed constant 1/12/2019 Physics 253

First Equation The last result can be easily rewritten: Which gives the velocity of an object after a given time and constant acceleration Remember accelerating along Lincoln Highway from rest to 75 m/hr in 5.0 s? Would you get a ticket? We determined the average acceleration was 4.2 m/s2. Assuming the acceleration was constant v = 0 + (4.2 m/s2)(5.0 s) = 0 + 21.0 m/s = 21.0 m/s Converting to mph we see v = (21.0m/s)(3600s/hr) (1km/1000m)(0.6km/mi)= 45.4 mi/hr 1/12/2019 Physics 253

First Equation BUSTED!!! The last result can be easily rewritten: Which gives the velocity of an object after a given time and constant acceleration Remember accelerating along Lincoln Highway from rest to 75 m/hr in 5.0 s? Would you get a ticket? We determined the average acceleration was 4.2 m/s2. Assuming the acceleration was constant v = 0 + (4.2 m/s2)(5.0 s) = 0 + 21.0 m/s = 21.0 m/s Converting to mph we see v = (21.0m/s)(3600s/hr) (1km/1000m)(0.6km/mi)= 45.4 mi/hr BUSTED!!! 1/12/2019 Physics 253

Second and Third Equations Rewriting the first result: Not so helpful since it doesn’t give us the position in terms of velocity and acceleration. So, substitute for the average velocity with: And use our first equation of motion to inject acceleration And now using this to eliminate the average velocity from the expression for position: Which gives us position in terms of velocity and acceleration. Note the quadratic dependence on time 1/12/2019 Physics 253

Fourth Equation The three equations derived relate position, velocity, and acceleration as functions of time. Useful to relate the three variables alone. To do so we use the three equations just derived to eliminate time. Starting with Substituting for the average velocity: Substituting for t using 1/12/2019 Physics 253

Fourth Equation We get Now solving for the square of the velocity Which gives a result independent of time 1/12/2019 Physics 253

The Four Equations (constant acceleration): Memorize these, put them on your mirror, write a song about them, whatever! 1/12/2019 Physics 253

First Example: 1-D Equations A jet plane has a takeoff speed of 250 km/h. The plane starts from rest, and has a constant acceleration of 1.25 x 104 km/h2 What is the length of the runway needed? We are given final velocity and acceleration and asked for the distance traveled. The third equation seems appropriate. We need to recast the equation, by solving for the distance traveled: Note the initial position and velocity are zero 1/12/2019 Physics 253

First Example: 1-D Equations A jet plane has a takeoff speed of 250 km/h. The plane starts from rest, and has a constant acceleration of 1.25 x 104 km/h2 What is the length of the runway needed? We are given final velocity and acceleration and asked for the distance traveled. The third equation seems appropriate. We need to recast the equation, by solving for the distance traveled: Note the initial position and velocity are zero Passes the smell test as well! 1/12/2019 Physics 253

2nd Example: Air bag estimate How fast must an airbag inflate to protect a driver within a 1 m crumple zone at a collision of 100 km/hr? First lets get everything into SI units: Now we have the initial velocity Vo=28m/s the final velocity V=0 The distance traveled x = 1m Looking at the equations we see to get time we need accel. And a 3rd eq gives the time They do deploy in milliseconds 1/12/2019 Physics 253

http://nicadd.niu.edu/people/blazey/Physics_253_2006/Physics_253_2006.htm 1/12/2019 Physics 253