Describing Motion: Kinematics in One Dimension AP Physics Chapter 2.

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Presentation transcript:

Describing Motion: Kinematics in One Dimension AP Physics Chapter 2

Describing Motion: Kinematics in One Dimension AP Physics Section 2-1 Reference Frames and Displacement

Describing Motion: Kinematics in One Dimension Mechanics – study of motion, force, energy Kinematics – how objects move Dynamics – why objects move Translational Motion – move without rotation 2-1

Describing Motion: Kinematics in One Dimension Reference Frames (Frames of Reference) Are we moving? Compared to what? Usually with “respect to the Earth” Unless otherwise specified All other cases, must specify the frame of reference Typically done with coordinate grid and x and y axis (only x or y for 1D motion) 2-1

Describing Motion: Kinematics in One Dimension Positive – up and right Negative – down and left 2-1

Describing Motion: Kinematics in One Dimension Defining Motion Position – relative to frame of reference (x or y) Displacement – change in position (meters)  x = x 2 -x 1 Not distance!! 2-1

Describing Motion: Kinematics in One Dimension Distance vs. Displacement 2-1

Describing Motion: Kinematics in One Dimension 1. Distance – scalar (magnitude) 2. Displacement – vector (magnitude and direction) a. Must give a direction For example East/West, up/down 2-1

Describing Motion: Kinematics in One Dimension AP Physics Section 2-2 Average Velocity

Describing Motion: Kinematics in One Dimension Average Speed – distance per unit time (scalar) Average Velocity – displacement per unit time (vector)(meters/second)  x = displacement  t = change in time 2-2

Describing Motion: Kinematics in One Dimension AP Physics Section 2-3 Instantaneous Velocity

Describing Motion: Kinematics in One Dimension Instantaneous Velocity – the average velocity during an infinitesimally short time interval We will only calculate situations with constant velocity or constant acceleration Calculus is required if acceleration is not constant 2-3

Describing Motion: Kinematics in One Dimension Slope of any displacement time graph is the instantaneous velocity 2-3

Describing Motion: Kinematics in One Dimension AP Physics Section 2-4 Acceleration

Describing Motion: Kinematics in One Dimension Average Acceleration – change in velocity per unit time (vector) (meters/second 2 ) v is final velocity v 0 is initial velocity (or at time 0) Sign of a indicates direction of vector Deceleration is just negative acceleration 2-4

Describing Motion: Kinematics in One Dimension Acceleration is the slope of the velocity time graph 2-4

Describing Motion: Kinematics in One Dimension AP Physics Section 2-5 Motion at Constant Acceleration

Describing Motion: Kinematics in One Dimension We are limited to calculations when acceleration is a constant We will use the mathematical definition of displacement, velocity, and acceleration to derive 4 Kinematic equations. **Memorize these equations – you will use them a lot 2-5

Describing Motion: Kinematics in One Dimension Assume t 0 = 0, it drops out of equations We rework the definition of acceleration to get our first working equation 2-5

Describing Motion: Kinematics in One Dimension For the second equation we first rework the definition of average velocity to solve for displacement 2-5

Describing Motion: Kinematics in One Dimension We define average velocity as the average of the initial and final velocity (only possible with constant acceleration) 2-5

Describing Motion: Kinematics in One Dimension Now we combine the last three equations 2-5

Describing Motion: Kinematics in One Dimension For the third equation we start by using a version of the definition of velocity 2-5

Describing Motion: Kinematics in One Dimension Combine with our average velocity definition 2-5

Describing Motion: Kinematics in One Dimension Solve the definition of acceleration for time 2-5

Describing Motion: Kinematics in One Dimension Combine and you get 2-5

Describing Motion: Kinematics in One Dimension Finally, solve for final velocity 2-5

Describing Motion: Kinematics in One Dimension The 4 th equation is not found in your book, but is in most others 2-5

Describing Motion: Kinematics in One Dimension AP Physics Section 2-6 Solving Problems

Describing Motion: Kinematics in One Dimension 1.Determine what the object is your are solving for. 2.Draw a diagram. Determine the positive and negative direction for motion. 3.Write down any known quantities. 4.Think about “The Physics” of the problem. 5.Determine what equation, or combination of equations will work under theses Physics conditions. 2-6

Describing Motion: Kinematics in One Dimension 6.Make your calculations. 7.See if your answer is reasonable. 8.Determine what units belong with the number, and what the direction should be if it is a vector. 2-6

Describing Motion: Kinematics in One Dimension A car slows down uniformly from a speed of 21.0 m/s to rest in 6.00s. How far did it travel in this time? 1.Object – car 2.Diagram 2-6

Describing Motion: Kinematics in One Dimension A car slows down uniformly from a speed of 21.0 m/s to rest in 6.00s. How far did it travel in this time? 1.Object – car 2.Diagram 3.Know v 0 =21.0m/s v =0m/s t=6.00s 2-6

Describing Motion: Kinematics in One Dimension A car slows down uniformly from a speed of 21.0 m/s to rest in 6.00s. How far did it travel in this time? 5.Physics – car is going through negative acceleration in 1D, acceleration is constant 6.Equation – needs v 0, v, t, x (define x 0 =0) So 2-6

Describing Motion: Kinematics in One Dimension A car slows down uniformly from a speed of 21.0 m/s to rest in 6.00s. How far did it travel in this time? 5.Physics – car is going through negative acceleration in 1D, acceleration is constant 6.Equation – needs v 0, v, t, x (define x 0 =0) Solve 2-6

Describing Motion: Kinematics in One Dimension A car is behind a truck going 25m/s on the highway. The car’s driver looks for an opportunity to pass, guessing that his car can accelerate at 1.0m/s 2. He gauges that he has to cover the 20 m length of the truck, plus 10 m clear room at the rear of the truck and 10 m more at the front of it. In the oncoming lane, he sees a car approaching, probably also traveling at 25 m/s. He estimates that the car is about 400 m away. Should he attempt to pass? 2-6

Describing Motion: Kinematics in One Dimension 1.Object – car 2.Diagram 2-6

Describing Motion: Kinematics in One Dimension 1.Object – car 2.Diagram 3.Known quantities Car relative truckCar relative to App. CarApp. Car v 0 =0m/s25m/s25m/s a=1m/s 2 1m/s 2 0m/s 2 x=40m 360m (why?) 4. Physics – car must travel 40 m to pass truck, approaching car can travel maximum of m in that same period of time, or their paths overlap 2-6

Describing Motion: Kinematics in One Dimension 5. Time for car to pass 2-6

Describing Motion: Kinematics in One Dimension 5. How far did the other car get in that time? 2-6

Describing Motion: Kinematics in One Dimension AP Physics Section 2-7 Falling Objects (the y-dimension)

Describing Motion: Kinematics in One Dimension We will ignore air friction We will learn the why later. Acceleration due to gravity at earths surface is 9.80 m/s 2 directed downward (-9.80m/s 2 ) Symbol g represents acceleration due to gravity Still use motion equations but x is replaced with y a is replaced with g 2-7

Describing Motion: Kinematics in One Dimension Two common problems 1.Acceleration and velocity are always in the same direction a. No, as an object is thrown upward, velocity is +y, acceleration is –y 2.Acceleration is zero at the highest point. a. No, at the highest point, the velocity is zero, but acceleration is always -9.80m/s 2 b. The object changes velocity, it must have an acceleration 2-7