Physics 101: Lecture 03 Kinematics Lecture Notes PDF

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Summary

These lecture notes cover kinematics, focusing on textbook sections 3.1-3.3 and some chapter 4 of a Physics 101 course. The notes include examples and explanations of concepts related to force, acceleration, and velocity. The notes will be of use to students enrolled or preparing for Physics 101.

Full Transcript

Physics 101: Lecture 03 Kinematics Today’s lecture will cover Textbook Sections 3.1-3.3 (and some Ch. 4) Physics 101: Lecture 3, Pg 1 Announcements HW 1 is due Tuesday February 1st at 6 am. No clicker points for Lect. 2? Re-register for this course! Of...

Physics 101: Lecture 03 Kinematics Today’s lecture will cover Textbook Sections 3.1-3.3 (and some Ch. 4) Physics 101: Lecture 3, Pg 1 Announcements HW 1 is due Tuesday February 1st at 6 am. No clicker points for Lect. 2? Re-register for this course! Office hours start Friday. Read the course description & FAQ on the course web site! Physics 101: Lecture 3, Pg 2 Force at Angle Example  A person is pushing a 15 kg block across a floor with k= 0.4 at a constant speed. If she is pushing down at an angle of 25 degrees, what is the magnitude of her force on the block? x- direction: Fx = max Combine: Fpush cos() – Ffriction = 0 Fpush cos() / –mg – FPush sin() = 0 Fpush cos() –  FNormal = 0 Fpush ( cos() /  - sin()) = mg FNormal = Fpush cos() /  Fpush = m g / ( cos()/ – sin()) y- direction: Fy = may Fpush = 80 N FNormal –Fweight – FPush sin() = 0 Normal FNormal –mg – FPush sin() = 0 Pushing y  x  Friction Weight Physics 101: Lecture 3, Pg 3 Homework 2 Example  Calculate the tension in the left string. y x x-direction: F=ma -TL+TR cos()= 0 TR TL  TL = TR cos() y-direction: F=ma W TR sin() – Mg = 0 Combine: TR = Mg / sin() TL = Mg cos()/sin() Physics 101: Lecture 3, Pg 4 Overview  Kinematics: Description of Motion Position and displacement velocity » average » instantaneous Acceleration » average » instantaneous Relative velocity (first pass) Physics 101: Lecture 3, Pg 5 Position vs Time Plots  Gives location at any time.  Displacement is change in position. x (m)  Slope gives instantaneous velocity. 3 Position at t=3, x(3) = 1 t Displacement between t=5 and t=1. x = -1.0 m 4 1.0 m - 2.0 m = -1.0 m -3 Average velocity between t=5 and t=1. v = -0.25 m/s -1 m / 4 s = -0.25 m/s Physics 101: Lecture 3, Pg 6 Velocity vs Time Plots  Gives velocity at any time. v (m/s)  Area gives displacement 3  Slope gives instantaneous acceleration. 6 1.5 t velocity at t=2, v(2) = 3 m/s 4 Displacement between t=0 and t=3: x= 7.5 m -3 t=0 to t=1: ½ (3m/s) (1 s) = 1.5 m t=1 to t=3: (3m/s) (2 s) = 6 m Average velocity between t=0 and t=3? v= 7.5 m / 3s = 2.5 m/s Change in v between t=5 and t=3. v = -2 m/s – 3 m/s = -5 m/s Average acceleration between t=5 and t=3: a = -5 m/s / (2 s) = -2.5 m/s2 Physics 101: Lecture 3, Pg 7 Acceleration vs Time Plots  Gives acceleration at any time.  Area gives change in velocity a (m/s2) 3 Acceleration at t=4, a(4) = -2 m/s2 6 Change in v between t=4 and t=1. v = +4 m/s t t=1-3: v = (3m/s2)(2s) = 6 m/s 24 t=3-4: v = (-2m/s2)(1s) = -2 m/s -3 Physics 101: Lecture 3, Pg 8 Acceleration Preflights Is it possible for an object to have a positive velocity at the same time as it has a negative acceleration? 88% 1 - Yes “the object could be slowing down.” 12% 2 - No If the velocity of some object is not zero, can its acceleration ever be zero ? 87% 1 - Yes “The velocity could be non-zero and constant. A constant velocity has no 13% 2 - No acceleration..” Physics 101: Lecture 3, Pg 9 Velocity ACT If the average velocity of a car during a trip along a straight road is positive, is it possible for the instantaneous velocity at some time during the trip to be negative? A - Yes B - No Drive north 5 miles, put car in reverse and drive south 2 miles. Average velocity is positive. Physics 101: Lecture 3, Pg 10 Dropped Ball y A ball is dropped from a height of x two meters above the ground.  Draw vy vs t v v v 9 A 9 B 9 C 0.5 t 0.5 t 0.5 t -6 -6 -6 v v 9 9 E D 0.5 t 0.5 t -6 -6 Physics 101: Lecture 3, Pg 11 Dropped Ball x A ball is dropped for a height of two meters above the ground. t v  Draw v vs t  Draw x vs t t  Draw a vs t a t Physics 101: Lecture 3, Pg 12 Tossed Ball A ball is tossed from the ground up a height of two meters above the ground. And falls back down y x  Draw v vs t v v v 9 A 9 B 9 C 1 t 1 t 1 t -6 -6 -6 v v 9 9 D E 1 t 1 t -6 -6 Physics 101: Lecture 3, Pg 13 Tossed Ball x A ball is tossed from the ground up a height of two meters above the ground. t And falls back down v  Draw v vs t  Draw x vs t t  Draw a vs t a t Physics 101: Lecture 3, Pg 14 ACT A ball is thrown straight up in the air and returns to its initial position. During the time the ball is in the air, which of the following statements is true? A - Both average acceleration and average velocity are zero. B - Average acceleration is zero but average velocity is not zero. C - Average velocity is zero but average acceleration is not zero. D - Neither average acceleration nor average velocity are zero. Vave = Y/t = (Yf – Yi) / (tf – ti) = 0 aave = V/t = (Vf – Vi) / (tf – ti) Not 0 since Vf and Vi are not the same ! Physics 101: Lecture 3, Pg 15 Relative Velocity (first pass) You are on a train traveling 40 mph North. If you walk 5 mph toward the front of the train, what is your speed relative to the ground? A) 45 mph B) 40 mph C) 35 mph 40 mph N + 5 mph N = 45 mph N 40 5 45 Physics 101: Lecture 3, Pg 16 Relative Velocity You are on a train traveling 40 mph North. If you walk 5 mph toward the rear of the train, what is your speed relative to the ground? A) 45 mph B) 40 mph C) 35 mph 40 mph N - 5 mph N = 35 mph N 40 5 35 Physics 101: Lecture 3, Pg 17 Relative Velocity You are on a train traveling 40 mph North. If you walk 5 mph sideways across the car, what is your speed relative to the ground? A) < 40 mph B) 40 mph C) >40 mph 40 mph N + 5 mph W = 41 mph N 5 | v | 402  52 40 Physics 101: Lecture 3, Pg 18 Relative Velocity  Sometimes your velocity is known relative to a reference frame that is moving relative to the earth. Example 1: A person moving relative to a train, which is moving relative to the ground. Example 2: a plane moving relative to air, which is then moving relative to the ground.  These velocities are related by vector addition: » vac is the velocity of the object relative    to the ground vac  vab vbc » vab is the velocity of the object relative to a moving reference frame » vbc is the velocity of the moving reference frame relative to the ground Physics 101: Lecture 3, Pg 19 Tractor Demo 1 Which direction should I point the tractor to get it across the table fastest? A) 30 degrees left B) Straight across C) 30 degrees right 1 2 3 Physics 101: Lecture 3, Pg 20 Tractor Demo (moving table)  Which direction should I point the tractor to get it across the table fastest? A) 30 degrees left B) Straight across C) 30 degrees right 1 2 3 Physics 101: Lecture 3, Pg 21 Summary of Concepts  kinematics: A description of motion  position: your coordinates  displacement: x = change of position  velocity: rate of change of position average : x/t instantaneous: slope of x vs. t  acceleration: rate of change of velocity average: v/t instantaneous: slope of v vs. t  relative velocity: vac = vab + vbc Physics 101: Lecture 3, Pg 22

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