i-clicker Question How many beans are in the 900 ml beaker? A. Fewer than 1000 B C D E.

Similar documents
Physics 123 Lecture 2 1 Dimensional Motion

i-clicker Question lim Physics 123 Lecture 2 1 Dimensional Motion x 1 x 2 v is not constant in time v = v(t) acceleration lim Review:

Physics 1200 Mechanics, Kinematics, Fluids, Waves

Projectile Motion. What is projectile? Projectile -Any object which projected by some means and continues to move due to its own inertia (mass).

1 Course Notes in Introductory Physics Jeffrey Seguritan

i-clicker!! x 2 lim Lecture 3 Motion in 2- and 3-Dimensions lim REVIEW OF 1-D MOTION

Chapter 2. Kinematics in One Dimension. Kinematics deals with the concepts that are needed to describe motion.

SPH3U1 Lesson 06 Kinematics

AP Physics Kinematic Wrap Up

Chapter 3 Kinematics in Two Dimensions; Vectors

PHYS 314 HOMEWORK #3

Yeu-Sheng Paul Shiue, Ph.D 薛宇盛 Professor and Chair Mechanical Engineering Department Christian Brothers University 650 East Parkway South Memphis, TN

Physics 2010 Motion with Constant Acceleration Experiment 1

20 Faraday s Law and Maxwell s Extension to Ampere s Law

EXAM #1 PHYSICAL SCIENCE 103 FALLF, 2017

Differentiation Applications 1: Related Rates

1.2.1 Vectors. 1 P age. Examples What is the reference vector angle for a vector that points 50 degrees east of south?

Being able to connect displacement, speed, and acceleration is fundamental to working

LAHS Physics Semester 1 Final Review Information

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System

Kinematics. Describing Motion. Reference Frames. Measurements of position, distance or speed must be with respect to a frame of reference.

EXAM #1 PHYSICAL SCIENCE 103 Spring, 2016

i-clicker i-clicker Newton s Laws of Motion First Exam Coming Up! Components of Equation of Motion

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System

Information for Physics 1201 Midterm I Wednesday, February 20

MODULE 1. e x + c. [You can t separate a demominator, but you can divide a single denominator into each numerator term] a + b a(a + b)+1 = a + b

Phys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1

PROJECTILES. Launched at an Angle

Math 105: Review for Exam I - Solutions

Would you risk your live driving drunk? Intro

Study Guide: PS. 10 Motion, Forces, Work & Simple Machines DESCRIBING MOTION SPEED

Solution to HW14 Fall-2002

Displacement, Time, Velocity

Physics 212. Lecture 12. Today's Concept: Magnetic Force on moving charges. Physics 212 Lecture 12, Slide 1

Faculty of Engineering and Department of Physics Engineering Physics 131 Midterm Examination February 27, 2006; 7:00 pm 8:30 pm

PHYSICS 151 Notes for Online Lecture #23

Lecture 2: Single-particle Motion

= m. Suppose the speed of a wave on a string is given by v = Κ τμ

Lecture 6: Phase Space and Damped Oscillations

Revised 2/07. Projectile Motion

Study Guide Physics Pre-Comp 2013

BASIC DIRECT-CURRENT MEASUREMENTS

Chapter 2: 1D Kinematics Tuesday January 13th

د.عبدالله محمد الزير

Feb 6, 2013 PHYSICS I Lecture 5

making triangle (ie same reference angle) ). This is a standard form that will allow us all to have the X= y=

CHAPTER 6 -- ENERGY. Approach #2: Using the component of mg along the line of d:

Lab #3: Pendulum Period and Proportionalities

Chapter 5: Force and Motion I-a

Phys101 First Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Wednesday, September 25, 2013 Page: 1

ENGI 4430 Parametric Vector Functions Page 2-01

1/2 and e0 e s ' 1+ imm w 4 M s 3 πρ0 r 3 m. n 0 ktr. .Also,since n 0 ktr 1,wehave. 4 3 M sπρ 0 r 3. ktr. 3 M sπρ 0

Welcome back to Physics 211

SKAA 1213 Engineering Mechanics

KINEMATICS OF A PARTICLE. Prepared by Engr. John Paul Timola

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?

Motion Along a Straight Line (Motion in One-Dimension)

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?

Experiment #3. Graphing with Excel

CHM112 Lab Graphing with Excel Grading Rubric

Lim f (x) e. Find the largest possible domain and its discontinuity points. Why is it discontinuous at those points (if any)?

CHAPTER 24: INFERENCE IN REGRESSION. Chapter 24: Make inferences about the population from which the sample data came.

a. Determine the sprinter's constant acceleration during the first 2 seconds.

Section 5.8 Notes Page Exponential Growth and Decay Models; Newton s Law

M thematics. National 5 Practice Paper D. Paper 1. Duration 1 hour. Total marks 40

Physics 1: Mechanics

2. The acceleration of a simple harmonic oscillator is zero whenever the oscillating object is at the equilibrium position.

READING STATECHART DIAGRAMS

4th Indian Institute of Astrophysics - PennState Astrostatistics School July, 2013 Vainu Bappu Observatory, Kavalur. Correlation and Regression

Lecture 5: Equilibrium and Oscillations

Math 9 Year End Review Package. (b) = (a) Side length = 15.5 cm ( area ) (b) Perimeter = 4xside = 62 m

CLASS XI SET A PHYSICS

Motion in Two and Three Dimensions

Lab 1 The Scientific Method

PHYSICS LAB Experiment 10 Fall 2004 ROTATIONAL DYNAMICS VARIABLE I, FIXED

MCAT Physics - Problem Drill 06: Translational Motion

Rutgers University Department of Physics & Astronomy. 01:750:271 Honors Physics I Fall Lecture 4. Home Page. Title Page. Page 1 of 35.

Accelerated Chemistry POGIL: Half-life

(a) During the first part of the motion, the displacement is x 1 = 40 km and the time interval is t 1 (30 km / h) (80 km) 40 km/h. t. (2.

Chapter 2: 1D Kinematics

Edexcel GCSE Physics

This chapter gets the ball rolling by discussing some fundamental physics measurements.

Review for the final exam (Math 127)

AP Physics Laboratory #4.1: Projectile Launcher

PLEASURE TEST SERIES (XI) - 07 By O.P. Gupta (For stuffs on Math, click at theopgupta.com)

CONSTRUCTING STATECHART DIAGRAMS

CHAPTER 8b Static Equilibrium Units

Motion in Two and Three Dimensions

Fall 2013 Physics 172 Recitation 3 Momentum and Springs

AP Statistics Practice Test Unit Three Exploring Relationships Between Variables. Name Period Date

Trigonometric Ratios Unit 5 Tentative TEST date

Thermodynamics and Equilibrium

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations

**DO NOT ONLY RELY ON THIS STUDY GUIDE!!!**

ASTRODYNAMICS. o o o. Early Space Exploration. Kepler's Laws. Nicolaus Copernicus ( ) Placed Sun at center of solar system

Charge of an Electron

CHAPTER 1 -- MATH REVIEW

Chemistry 114 First Hour Exam

Example 1. A robot has a mass of 60 kg. How much does that robot weigh sitting on the earth at sea level? Given: m. Find: Relationships: W

AP Physics. Summer Assignment 2012 Date. Name. F m = = + What is due the first day of school? a. T. b. = ( )( ) =

Transcription:

i-clicker Questin Hw many beans are in the 900 ml beaker? A. Fewer than 1000 B. 1000-1500 C. 1500-000 D. 000-500 E. Mre than 500

Reiew: Physics 13 Lecture 1 Dimensinal Mtin Displacement: Dx = x - x 1 (If Dx < 0, the displacement ectr pints t the left.) Aerage elcity: (Nt the same as aerage speed) a x t x t 1 1 Dx Dt slpe = a x 1 x x-t diagram: x = x(t) (t ) (t ) > (t 1 ) (t) Instantaneus elcity: lim Dt0 Dx Dt dx dt (t) is slpe f tangent t x-t plt at time t.

is nt cnstant in time = (t) acceleratin acceleratin: time rate f change f elcity aerage acceleratin: aa instantaneus acceleratin: (slpe f line tangent t (t) at time t ) a t t 1 1 lim Dt0 D Dt D Dt d dt a d dt d x dt a is slpe f (t) graph. a is curature f x(t) graph. In -t plt abe, (t) is a straight line cnstant acceleratin i.e.: (t) = [cnst]t d/dt = [cnst] Nt always true! Suppse: (t) = Ct 3 Then: a = a(t) = d/dt = 3Ct cnstant in time!

Finding acceleratin n a -t graph The (t) graph may be used t find the instantaneus acceleratin and the aerage acceleratin. Cpyright 01 Pearsn Educatin Inc.

Acceleratin frm x-t plt: > 0 > 0 (> A ) > 0 (> B ) > 0 (< C ) = 0 < 0 < 0 > 0 > 0 = 0 < 0 < 0 = 0 > 0 Slpe f -t plt gies instantaneus acceleratin

i-clicker Questin Shw mtin sensr!

Cnstant acceleratin is an imprtant special case! Deseres special attentin!! differentiate a * (t-t a ) (t) = (t a ) + a * (t-t a ) x (t a ) Let t a = 0 (t) = + at ½at t differentiate x x(t) = x + t + ½at

KINEMATIC EQUATIONS in 1D 1 (t) = + at x(t) = x + t + ½ at cnstant acceleratin Other helpful relatinships: 3 4 a xx ; a t cnst. acc. nly ALGEBRA: 3 x x = a t ax subst. frm 4 ( x x ) t 5 rewrite 1 t = ( - ) / a 6 plug 6 int 5 ( x x ) a ( x x ) a

Lets put these equatins t wrk! Drag race: Cnstant acceleratin alng 400 m track. = 150 m/s at end. What is the acceleratin? Knwn: (x x ) = 400 m; = 150 m/s; = 0 Need: a =? ( x x ) a (150 m/s) a (400 m) 8 m/s Hw lng des the race take? Knwn: (x x ),,, and a Need: t =? x(t) = x + t + ½at a ( x x ) 0 0 x - x = t + ½at 400 m = ½ (8 m/s ) t t = 5.3 s

Yellw Light Driing at 30 m/s Light turns yellw when yu are 30 m frm int. Decelerate at 10 m/s. Will yu stp befre intersectin? Knwn: = 30 m/s; a = -10 m/s ; f = 0 m/s; Need: (x f - x ) =? N! f 0 (30 m/s) ( x f x ) a ( 10 m/s ) 45 m What shuld a be? Knwn: (x f - x ) = 30 m; = 30 m/s; f = 0 m/s Need: a =? a f ( x f x ) 0 (30 m/s) (30 m) 15 m/s If a = -30 m/s, where will I stp? (x f - x ) ~ 1/a s (x f - x ) = 15 m

iclicker A mtrcycle traeling alng the x-axis is accelerating at a rate f a = -4m/s. a. The mtrcycle is speeding up. b. The mtrcycle is slwing dwn. c. The mtrcycle is neither speeding up nr slwing dwn. d. The mtrcycle is bth speeding up and slwing dwn. e. The mtrcycle may be slwing dwn r speeding up. a a Slwing dwn Speeding up

Freely falling bdies Free fall is the mtin f an bject under the influence f nly graity. In the figure, a strbe light flashes with equal time interals between flashes. The elcity change is the same in each time interal, s the acceleratin is cnstant. Cpyright 01 Pearsn Educatin Inc.

FREE FALL Mtin in 1-D under the influence f graity. acceleratin due t graity is cnstant (at Earth s surface) a = -g where g = 9.80 m/s graity acts ertically dwnward (chse y-axis as ertical) Same equatins f mtin BUT: a is replaced with g! (t) = - gt y(t) = y + t - ½gt ( y y ) g

EXAMPLE: REACTION TIME (red rulers) Knwn: y = 0 m; = 0 m/s ; a = -g ; y f = - 0.10 m Need: t =?? 0 0 y = y + t - ½gt y f = - ½gt t y g ( 0.10 m) 9.8 m/s t 0.0 s 0.14 s

EXAMPLE: Drp a penny frm tp f the Empire State Building! (DO NOT TRY THIS!) Obsere: The penny takes 8.1 s t hit grund Hw tall is building? Knwn: = 0 m/s; a = -g; t = 8.1 s; y = 0 Need: y - y 0 0 y = y + t - ½gt y = - ½gt = -(½)(9.8 m/s )(8.1 s) y = - 30 m What s the elcity f the penny just befre it hits the grund? Knwn: = 0 m/s; a = -g; t = 8.1 s; and (y - y )= -30 m = -gt = - (9.8 m/s )(8.1 s) = -79 m/s

What if I first thrw cin upward with speed f 67 mi/hr (=30 m/s)? When will cin reach max height? Knwn: = +30 m/s; a = -g Need: t when = 0 = - gt 0 = 30 m/s (9.8 m/s )t t g 30 m/s 9.8 m/s y = y + t - ½gt but y = y = 0 0 = t - ½gt = t ( - ½gt) t = 0 r t = 6 s (abe starting pint) When will it pass me n the way dwn? 3 s What is elcity just befre hitting grund? ( y y ) g = - 85 m/s

Things yu always wanted t knw but were afraid t ask 1. Can a penny drpped frm the Empire State Building embed itself in the sidewalk (r a persn s skull)?. Is it OK t neglect air resistance (drag)? Ask the Mythbusters! 18

EXAMPLE: Drp a penny frm tp f the Empire State Building! (DO NOT TRY THIS!) Obsere: The penny takes 8.1 s t hit grund Hw tall is building? Knwn: y = 0 m/s; a = -g; t = 8.1 s; y = 0 Need: y - y 0 0 y = y + y t - ½gt y = - ½gt = -(½)(9.8 m/s )(8.1 s) y = - 30 m What s the elcity f the penny just befre it hits the grund? Knwn: y = 0 m/s; a = -g; t = 8.1 s; and (y - y )= -30 m = -gt = - (9.8 m/s )(8.1 s) = -79 m/s BUT: Terminal elcity = -9 m/s!!!