Physics 18 Spring 2010 Midterm 1

Similar documents
Physics 8 Spring 2012 Midterm 1

Physics Lecture 12. P. Gutierrez. Department of Physics & Astronomy University of Oklahoma

Physics 9 Summer 2010 Midterm

Physics 9 Spring 2011 Midterm 1 Solutions

Physics 9 Spring 2012 Midterm 1 Solutions

3. A piece of candy is accelerated at 3.0 m/s 2 in the direction shown by a, over a frictionless horizontal surface. The acceleration is caused by 3

Reading Quiz. Chapter 5. Physics 111, Concordia College

After the spring losses contact with both masses, the speed of m is the speed of 3m.

Physics 18 Spring 2010 Midterm 2 Solutions

PHYSICS 221 SPRING EXAM 1: February 20, 2014; 8:15pm 10:15pm

A. B. C. D. E. v x. ΣF x

PHYSICS 221 SPRING 2015

PH201 Chapter 5 Solutions

Isaac Newton ( ) 1687 Published Principia Invented Calculus 3 Laws of Motion Universal Law of Gravity

Physics 121, Final Exam Do not turn the pages of the exam until you are instructed to do so.

Phys101 Lecture 5 Dynamics: Newton s Laws of Motion

AP Physics C: Work, Energy, and Power Practice

Q16.: A 5.0 kg block is lowered with a downward acceleration of 2.8 m/s 2 by means of a rope. The force of the block on the rope is:(35 N, down)

Chapter 4. Forces and Newton s Laws of Motion. continued

Physics Exam 2 October 11, 2007

= 40 N. Q = 60 O m s,k

Thursday February 8. Write these equations in your notes if they re not already there. You will want them for Exam 1 & the Final.

Question 01. A. Incorrect! This is not Newton s second law.

Name Student ID Phys121 Win2011

Physics 101. Hour Exam I Spring Last Name: First Name Network-ID Discussion Section: Discussion TA Name:

---- WITH SOLUTIONS ----

AP Physics 1: MIDTERM REVIEW OVER UNITS 2-4: KINEMATICS, DYNAMICS, FORCE & MOTION, WORK & POWER

Solution. will lead to a positive torque, while the bigger cat will give a negative torque. So,

Which, if any, of the velocity versus time graphs below represent the movement of the sliding box?

PHYSICS 221 SPRING EXAM 1: February 16, 2012; 8:00pm 10:00pm

PHY2053 General Physics I

Physics 2211 ABC Quiz #3 Solutions Spring 2017

Web practice Chapter 4 Newton's Laws of Motion

Physics 2101, First Exam, Spring 2006

UIC Physics 105. Midterm 1 Practice Exam. Summer 2013 Best if used by July 2 PROBLEM POINTS SCORE

AP Physics Multiple Choice Practice Torque

Lecture 6 Force and Motion. Identifying Forces Free-body Diagram Newton s Second Law

Equilibrium. For an object to remain in equilibrium, two conditions must be met. The object must have no net force: and no net torque:

PHYSICS 221 SPRING EXAM 2: March 30, 2017; 8:15pm 10:15pm

PHYSICS 111 SPRING EXAM 1: February 6, 2017; 8:15pm - 9:45pm

Lecture Outline Chapter 6. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Physics 207 Lecture 9. Lecture 9

AP/Honors Physics Take-Home Exam 1

Physics 18 Spring 2011 Homework 3 Wednesday February 2, 2011

AP PHYSICS 1 UNIT 4 / FINAL 1 PRACTICE TEST

Worksheet #05 Kinetic Energy-Work Theorem

Unit-1. Force & Motion. Solutions 1.6 Energy & Motion page a) W 1. = F.x = 1. = F.cos60!.2x =F.x W 2. b) = W 2 = 2. 2.m.v 1.

P F = ma Newton's Laws Hmk

Exam. Name. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Chapter 4. Forces and Newton s Laws of Motion. continued

Physics 1A, Summer 2011, Summer Session 1 Quiz 3, Version A 1

SECOND MIDTERM -- REVIEW PROBLEMS

Physics Mechanics. Lecture 11 Newton s Laws - part 2

Summer Physics 41 Pretest. Shorty Shorts (2 pts ea): Circle the best answer. Show work if a calculation is required.

SPH4U UNIVERSITY PHYSICS

Pre-AP Physics Review Problems

PHYSICS 221 SPRING 2014

PHY2048 Physics with Calculus I

Sample Final Exam 02 Physics 106 (Answers on last page)

OPEN ONLY WHEN INSTRUCTED

PHYS 101 Previous Exam Problems. Force & Motion I

Newton s Laws and Free-Body Diagrams General Physics I


Physics 116A, Section 2, Second Exam Version B, February 26, Name (Please print)

Physics 116A, Section 2, Second Exam A, February 26, Name (Please print)

Concept of Force Challenge Problem Solutions

Solution Videos to Physics Problems Mechanics

8.01x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology. Problem Set 2

Choose the best answer for Questions 1-15 below. Mark your answer on your scantron form using a #2 pencil.

Physics 201, Midterm Exam 2, Fall Answer Key

Webreview practice test. Forces (again)

Physics 101 Lecture 5 Newton`s Laws

Review: Newton s Laws

Physics 101 Hour Exam 1 March 3, 2014

PHYSICS 111 SPRING EXAM 2: March 6, 2018; 8:15-9:45 pm

(a) Draw the coordinate system you are using and draw the free body diagram of the block during rotation with constant speed.


PHYSICS - CLUTCH CH 04: INTRO TO FORCES (DYNAMICS)

PHYSICS - CLUTCH CH 07: WORK & ENERGY.

PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009

Materials: One of each of the following is needed: Cart Meter stick Pulley with clamp 70 cm string Motion Detector

Chapter 4 Force and Motion

Physics Pre-comp diagnostic Answers

PHYS 124 Section A1 Mid-Term Examination Spring 2006 SOLUTIONS

Lecture Presentation. Chapter 4 Forces and Newton s Laws of Motion. Chapter 4 Forces and Newton s Laws of Motion. Reading Question 4.

ω = k/m x = A cos (ωt + ϕ 0 ) L = I ω a x = ω 2 x P = F v P = de sys J = F dt = p w = m g F G = Gm 1m 2 D = 1 2 CρAv2 a r = v2

Lecture PowerPoints. Chapter 4 Physics: for Scientists & Engineers, with Modern Physics, 4th edition Giancoli

PHYSICS 221 SPRING 2015

A force is a push or a pull.

General Physics Physics 101 Test #2 Spring 2018 Wednesday 2/28/18 Prof. Bob Ekey

Fraser Heights Secondary Physics 11 Mr. Wu Practice Test (Dynamics)

1982B1. The first meters of a 100-meter dash are covered in 2 seconds by a sprinter who starts from rest and accelerates with a constant

Chapter 4 Dynamics: Newton s Laws of Motion

PHYSICS 111 SPRING EXAM 2: March 7, 2017; 8:15-9:45 pm

Newton s Laws of Motion. Chapter 4

Kinematics and Dynamics

Newton s 3 Laws of Motion

Physics 111. Lecture 15 (Walker: 7.1-2) Work & Energy March 2, Wednesday - Midterm 1

Practice. Newton s 3 Laws of Motion. Recall. Forces a push or pull acting on an object; a vector quantity measured in Newtons (kg m/s²)

PHYS207 Exam 1 20 January, 2016

Transcription:

Physics 18 Spring 2010 Midterm 1 For the midterm, you may use one sheet of notes with whatever you want to put on it, front and back. Please sit every other seat, and please don t cheat! If something isn t clear, please ask. You may use calculators. All problems are weighted equally. PLEASE BOX YOUR FINAL ANSWERS! You have the full length of the class. If you attach any additional scratch work, then make sure that your name is on every sheet of your work. Good luck! 1. A 75 kilogram base runner has an initial speed of 8 m/s (almost 18 miles per hour), and he then slides to a stop over 4 m. What is the coefficient of sliding friction between the runner and ground during the slide? 1

2. An accident victim with a broken leg is being placed in traction. The patient wears a special boot with a pulley attached to the sole. The foot and boot together have a mass of 4.0 kg, and the doctor has decided to hang a 6.0 kg mass from the rope. The boot is suspended by the ropes and does not touch the bed. (a) Determine the amount of tension in the rope by using Newton s laws to analyze the hanging mass. (b) The net traction force needs to pull straight out on the leg. What is the proper angle θ for the upper rope? (c) What is the net traction force pulling the leg? Hint: If the pulleys are frictionless, which we will assume, the tension in the rope is constant from one end to the other. 2

3. Astronauts use a centrifuge to simulate the acceleration of a rocket launch. The centrifuge takes 30 seconds to speed up from rest to its top speed of 1 rotation every 1.3 seconds. The astronaut is strapped into a seat 6.0 m from the axis. (a) What is the astronaut s tangential acceleration during the first 30 seconds? (b) How many g s of acceleration does the astronaut experience when the device is rotating at top speed (each 9.8 m/s 2 of acceleration is 1 g)? 3

4. Let s look the maximum safe heights that a person could jump from in two different landing cases. (a) First, suppose a person of mass m jumps from a height h, and lands with straight legs such that they stop in a small distance d, cushioned only by the padding on the bottom of their feet. Using conservation of energy, show that the force acting back up on them from the ground is F = mgh d. (b) Upon compression bones typical break when subjected to a force per area above about 1.7 10 8 N/m 2. If the tibia near the ankle has a radius of about 1 cm, estimate the maximum height from which a 70 kg person could just land without breaking any bones if the padding on the soles of their feet is about 1 cm. (c) Now, suppose the person lands at the end of the jump using the muscles in his knees to help cushion the collision. Now his center of mass falls a height h before his feet make contact with the ground, but then he bends down, dropping his center of mass a further distance s (we can ignore the padding on his feet now, since it s small compared to how much he bends). Show that the required force is now ( F = mg 1 + h ). s (d) If he bends down 0.5 meters, what is the maximum height that he could just land from without breaking any bones? (Kids - don t try this at home!) 4

The potential energy between a pair of neutral atoms or molecules is very well-approximated by the Lennard-Jones Potential, given by the expression [ (σ ) 12 ( σ ) ] 6 P E(r) = 4ɛ, r r where ɛ and σ are constants, and r is the distance between the molecules. The potential energy is plotted in the figure to the right. The vertical axis is in units of ɛ, while the horizontal axis is in units of σ. Extra Credit Question!! The following is worth 10 extra credit points! Energy 8 7 6 5 4 3 2 1 0-2 -3-4 Molcular Bond Energy 0.75 1 1.25 1.5 1.75 2 2.25 2.5 2.75 3 3.25-1 Distance (a) Why does the potential energy approach zero as the distance gets bigger? (b) At what separation distance, in terms of σ and ɛ, is the potential energy zero? (c) At approximately what distance is the system in equilibrium? What is the potential energy at that distance? (Express your answers in terms of σ and ɛ.) (d) How much energy would you need to add to the system at equilibrium in order to break the molecular bonds holding it together? Why? (e) How much energy is released in the breaking of those molecular bonds? Why? Note - no calculation is needed to answer these problems! 5