- •Preface
- •Textbook Layout and Design
- •Preliminaries
- •See, Do, Teach
- •Other Conditions for Learning
- •Your Brain and Learning
- •The Method of Three Passes
- •Mathematics
- •Summary
- •Homework for Week 0
- •Summary
- •1.1: Introduction: A Bit of History and Philosophy
- •1.2: Dynamics
- •1.3: Coordinates
- •1.5: Forces
- •1.5.1: The Forces of Nature
- •1.5.2: Force Rules
- •Example 1.6.1: Spring and Mass in Static Force Equilibrium
- •1.7: Simple Motion in One Dimension
- •Example 1.7.1: A Mass Falling from Height H
- •Example 1.7.2: A Constant Force in One Dimension
- •1.7.1: Solving Problems with More Than One Object
- •Example 1.7.4: Braking for Bikes, or Just Breaking Bikes?
- •1.8: Motion in Two Dimensions
- •Example 1.8.1: Trajectory of a Cannonball
- •1.8.2: The Inclined Plane
- •Example 1.8.2: The Inclined Plane
- •1.9: Circular Motion
- •1.9.1: Tangential Velocity
- •1.9.2: Centripetal Acceleration
- •Example 1.9.1: Ball on a String
- •Example 1.9.2: Tether Ball/Conic Pendulum
- •1.9.3: Tangential Acceleration
- •Homework for Week 1
- •Summary
- •2.1: Friction
- •Example 2.1.1: Inclined Plane of Length L with Friction
- •Example 2.1.3: Find The Minimum No-Skid Braking Distance for a Car
- •Example 2.1.4: Car Rounding a Banked Curve with Friction
- •2.2: Drag Forces
- •2.2.1: Stokes, or Laminar Drag
- •2.2.2: Rayleigh, or Turbulent Drag
- •2.2.3: Terminal velocity
- •Example 2.2.1: Falling From a Plane and Surviving
- •2.2.4: Advanced: Solution to Equations of Motion for Turbulent Drag
- •Example 2.2.3: Dropping the Ram
- •2.3.1: Time
- •2.3.2: Space
- •2.4.1: Identifying Inertial Frames
- •Example 2.4.1: Weight in an Elevator
- •Example 2.4.2: Pendulum in a Boxcar
- •2.4.2: Advanced: General Relativity and Accelerating Frames
- •2.5: Just For Fun: Hurricanes
- •Homework for Week 2
- •Week 3: Work and Energy
- •Summary
- •3.1: Work and Kinetic Energy
- •3.1.1: Units of Work and Energy
- •3.1.2: Kinetic Energy
- •3.2: The Work-Kinetic Energy Theorem
- •3.2.1: Derivation I: Rectangle Approximation Summation
- •3.2.2: Derivation II: Calculus-y (Chain Rule) Derivation
- •Example 3.2.1: Pulling a Block
- •Example 3.2.2: Range of a Spring Gun
- •3.3: Conservative Forces: Potential Energy
- •3.3.1: Force from Potential Energy
- •3.3.2: Potential Energy Function for Near-Earth Gravity
- •3.3.3: Springs
- •3.4: Conservation of Mechanical Energy
- •3.4.1: Force, Potential Energy, and Total Mechanical Energy
- •Example 3.4.1: Falling Ball Reprise
- •Example 3.4.2: Block Sliding Down Frictionless Incline Reprise
- •Example 3.4.3: A Simple Pendulum
- •Example 3.4.4: Looping the Loop
- •3.5: Generalized Work-Mechanical Energy Theorem
- •Example 3.5.1: Block Sliding Down a Rough Incline
- •Example 3.5.2: A Spring and Rough Incline
- •3.5.1: Heat and Conservation of Energy
- •3.6: Power
- •Example 3.6.1: Rocket Power
- •3.7: Equilibrium
- •3.7.1: Energy Diagrams: Turning Points and Forbidden Regions
- •Homework for Week 3
- •Summary
- •4.1: Systems of Particles
- •Example 4.1.1: Center of Mass of a Few Discrete Particles
- •4.1.2: Coarse Graining: Continuous Mass Distributions
- •Example 4.1.2: Center of Mass of a Continuous Rod
- •Example 4.1.3: Center of mass of a circular wedge
- •4.2: Momentum
- •4.2.1: The Law of Conservation of Momentum
- •4.3: Impulse
- •Example 4.3.1: Average Force Driving a Golf Ball
- •Example 4.3.2: Force, Impulse and Momentum for Windshield and Bug
- •4.3.1: The Impulse Approximation
- •4.3.2: Impulse, Fluids, and Pressure
- •4.4: Center of Mass Reference Frame
- •4.5: Collisions
- •4.5.1: Momentum Conservation in the Impulse Approximation
- •4.5.2: Elastic Collisions
- •4.5.3: Fully Inelastic Collisions
- •4.5.4: Partially Inelastic Collisions
- •4.6: 1-D Elastic Collisions
- •4.6.1: The Relative Velocity Approach
- •4.6.2: 1D Elastic Collision in the Center of Mass Frame
- •4.7: Elastic Collisions in 2-3 Dimensions
- •4.8: Inelastic Collisions
- •Example 4.8.1: One-dimensional Fully Inelastic Collision (only)
- •Example 4.8.2: Ballistic Pendulum
- •Example 4.8.3: Partially Inelastic Collision
- •4.9: Kinetic Energy in the CM Frame
- •Homework for Week 4
- •Summary
- •5.1: Rotational Coordinates in One Dimension
- •5.2.1: The r-dependence of Torque
- •5.2.2: Summing the Moment of Inertia
- •5.3: The Moment of Inertia
- •Example 5.3.1: The Moment of Inertia of a Rod Pivoted at One End
- •5.3.1: Moment of Inertia of a General Rigid Body
- •Example 5.3.2: Moment of Inertia of a Ring
- •Example 5.3.3: Moment of Inertia of a Disk
- •5.3.2: Table of Useful Moments of Inertia
- •5.4: Torque as a Cross Product
- •Example 5.4.1: Rolling the Spool
- •5.5: Torque and the Center of Gravity
- •Example 5.5.1: The Angular Acceleration of a Hanging Rod
- •Example 5.6.1: A Disk Rolling Down an Incline
- •5.7: Rotational Work and Energy
- •5.7.1: Work Done on a Rigid Object
- •5.7.2: The Rolling Constraint and Work
- •Example 5.7.2: Unrolling Spool
- •Example 5.7.3: A Rolling Ball Loops-the-Loop
- •5.8: The Parallel Axis Theorem
- •Example 5.8.1: Moon Around Earth, Earth Around Sun
- •Example 5.8.2: Moment of Inertia of a Hoop Pivoted on One Side
- •5.9: Perpendicular Axis Theorem
- •Example 5.9.1: Moment of Inertia of Hoop for Planar Axis
- •Homework for Week 5
- •Summary
- •6.1: Vector Torque
- •6.2: Total Torque
- •6.2.1: The Law of Conservation of Angular Momentum
- •Example 6.3.1: Angular Momentum of a Point Mass Moving in a Circle
- •Example 6.3.2: Angular Momentum of a Rod Swinging in a Circle
- •Example 6.3.3: Angular Momentum of a Rotating Disk
- •Example 6.3.4: Angular Momentum of Rod Sweeping out Cone
- •6.4: Angular Momentum Conservation
- •Example 6.4.1: The Spinning Professor
- •6.4.1: Radial Forces and Angular Momentum Conservation
- •Example 6.4.2: Mass Orbits On a String
- •6.5: Collisions
- •Example 6.5.1: Fully Inelastic Collision of Ball of Putty with a Free Rod
- •Example 6.5.2: Fully Inelastic Collision of Ball of Putty with Pivoted Rod
- •6.5.1: More General Collisions
- •Example 6.6.1: Rotating Your Tires
- •6.7: Precession of a Top
- •Homework for Week 6
- •Week 7: Statics
- •Statics Summary
- •7.1: Conditions for Static Equilibrium
- •7.2: Static Equilibrium Problems
- •Example 7.2.1: Balancing a See-Saw
- •Example 7.2.2: Two Saw Horses
- •Example 7.2.3: Hanging a Tavern Sign
- •7.2.1: Equilibrium with a Vector Torque
- •Example 7.2.4: Building a Deck
- •7.3: Tipping
- •Example 7.3.1: Tipping Versus Slipping
- •Example 7.3.2: Tipping While Pushing
- •7.4: Force Couples
- •Example 7.4.1: Rolling the Cylinder Over a Step
- •Homework for Week 7
- •Week 8: Fluids
- •Fluids Summary
- •8.1: General Fluid Properties
- •8.1.1: Pressure
- •8.1.2: Density
- •8.1.3: Compressibility
- •8.1.5: Properties Summary
- •Static Fluids
- •8.1.8: Variation of Pressure in Incompressible Fluids
- •Example 8.1.1: Barometers
- •Example 8.1.2: Variation of Oceanic Pressure with Depth
- •8.1.9: Variation of Pressure in Compressible Fluids
- •Example 8.1.3: Variation of Atmospheric Pressure with Height
- •Example 8.2.1: A Hydraulic Lift
- •8.3: Fluid Displacement and Buoyancy
- •Example 8.3.1: Testing the Crown I
- •Example 8.3.2: Testing the Crown II
- •8.4: Fluid Flow
- •8.4.1: Conservation of Flow
- •Example 8.4.1: Emptying the Iced Tea
- •8.4.3: Fluid Viscosity and Resistance
- •8.4.4: A Brief Note on Turbulence
- •8.5: The Human Circulatory System
- •Example 8.5.1: Atherosclerotic Plaque Partially Occludes a Blood Vessel
- •Example 8.5.2: Aneurisms
- •Homework for Week 8
- •Week 9: Oscillations
- •Oscillation Summary
- •9.1: The Simple Harmonic Oscillator
- •9.1.1: The Archetypical Simple Harmonic Oscillator: A Mass on a Spring
- •9.1.2: The Simple Harmonic Oscillator Solution
- •9.1.3: Plotting the Solution: Relations Involving
- •9.1.4: The Energy of a Mass on a Spring
- •9.2: The Pendulum
- •9.2.1: The Physical Pendulum
- •9.3: Damped Oscillation
- •9.3.1: Properties of the Damped Oscillator
- •Example 9.3.1: Car Shock Absorbers
- •9.4: Damped, Driven Oscillation: Resonance
- •9.4.1: Harmonic Driving Forces
- •9.4.2: Solution to Damped, Driven, Simple Harmonic Oscillator
- •9.5: Elastic Properties of Materials
- •9.5.1: Simple Models for Molecular Bonds
- •9.5.2: The Force Constant
- •9.5.3: A Microscopic Picture of a Solid
- •9.5.4: Shear Forces and the Shear Modulus
- •9.5.5: Deformation and Fracture
- •9.6: Human Bone
- •Example 9.6.1: Scaling of Bones with Animal Size
- •Homework for Week 9
- •Week 10: The Wave Equation
- •Wave Summary
- •10.1: Waves
- •10.2: Waves on a String
- •10.3: Solutions to the Wave Equation
- •10.3.1: An Important Property of Waves: Superposition
- •10.3.2: Arbitrary Waveforms Propagating to the Left or Right
- •10.3.3: Harmonic Waveforms Propagating to the Left or Right
- •10.3.4: Stationary Waves
- •10.5: Energy
- •Homework for Week 10
- •Week 11: Sound
- •Sound Summary
- •11.1: Sound Waves in a Fluid
- •11.2: Sound Wave Solutions
- •11.3: Sound Wave Intensity
- •11.3.1: Sound Displacement and Intensity In Terms of Pressure
- •11.3.2: Sound Pressure and Decibels
- •11.4: Doppler Shift
- •11.4.1: Moving Source
- •11.4.2: Moving Receiver
- •11.4.3: Moving Source and Moving Receiver
- •11.5: Standing Waves in Pipes
- •11.5.1: Pipe Closed at Both Ends
- •11.5.2: Pipe Closed at One End
- •11.5.3: Pipe Open at Both Ends
- •11.6: Beats
- •11.7: Interference and Sound Waves
- •Homework for Week 11
- •Week 12: Gravity
- •Gravity Summary
- •12.1: Cosmological Models
- •12.2.1: Ellipses and Conic Sections
- •12.4: The Gravitational Field
- •12.4.1: Spheres, Shells, General Mass Distributions
- •12.5: Gravitational Potential Energy
- •12.6: Energy Diagrams and Orbits
- •12.7: Escape Velocity, Escape Energy
- •Example 12.7.1: How to Cause an Extinction Event
- •Homework for Week 12
Week 9: Oscillations |
427 |
Homework for Week 9
Problem 1.
Physics Concepts: Make this week’s physics concepts summary as you work all of the problems in this week’s assignment. Be sure to cross-reference each concept in the summary to the problem(s) they were key to, and include concepts from previous weeks as necessary. Do the work carefully enough that you can (after it has been handed in and graded) punch it and add it to a three ring binder for review and study come finals!
Problem 2.
Harmonic oscillation is conceptually very important because (as has been remarked in class) many things that are stable will oscillate more or less harmonically if perturbed a small distance away from their stable equilibrium point. Draw an energy diagram, a graph of a “generic” interaction potential energy with a stable equilibrium point and explain in words and equations where, and why, this should be.
Problem 3.
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L |
Moon |
gmoon= gearth /6 |
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m |
A pendulum with a string of length L supporting a mass m on the earth has a certain period T . A physicist on the moon, where the acceleration near the surface is around g/6, wants to make a pendulum with the same period. What mass mm and length Lm of string could be used to accomplish this?
428 |
Week 9: Oscillations |
Problem 4.
k 1 |
k 2 |
m
k 1
m
k 2
m
k eff
In the figure above identical masses m are attached to two springs k1 and k2 in “series” – one connected to the other end-to-end – and in “parallel” – the two springs side by side. In the third picture another identical mass m is shown attached to a single spring with constant ke .
a) |
What should ke be in terms of k1 and k2 for the series combination of springs so that the |
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force on the mass is the same for any given displacement |
x from equilibrium? |
b) |
What should ke be in terms of k1 and k2 for the parallel combination of springs so that the |
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force on the mass is the same for any given displacement |
x from equilibrium? |
Note that this problem illustrates the scaling of Young’s modulus with length (series) or area (parallel). It also gives you a head start on how series and parallel addition of resistors and capacitors works next semester! It’s therefore well worth puzzling over.
Week 9: Oscillations |
429 |
Problem 5.
Pleft |
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L |
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P |
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right |
a |
Iv |
r |
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Pleft |
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Pright |
b |
Iv |
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P |
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Pright |
left |
Iv |
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c |
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Pleft Iv |
Pright |
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d |
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In this class we usually idealize fluid flow by neglecting resistance (drag) and the viscosity of the fluid as it passes through cylindrical pipes so we can use the Bernoulli equation. As discussed in class, however, it is often necessary to have at sound conceptual understanding of at least the qualitative e ects of including the resistance and viscosity. Use Poiseuille’s Law and the concepts of resistance, pressure, and flow from the online textbook to answer and discuss the following simple questions. Make sure your conceptual understanding of these concepts is qualitatively sound!
a)Is Pa = Pleft −Pright greater than, less than, or equal to zero in figure a) above, where blood flows at a rate Iv horizontally through a blood vessel with constant radius r and some length L against the resistance of that vessel?
b)If the radius r increases (while flow Iv and length L remain the same as in a), does the
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pressure di erence Pb increase, decrease, or remain the same compared to Pa? |
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c) |
If the length increases (while flow Iv and radius r remains the same as in a), does the pressure |
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di erence Pc increase, decrease, or remain the same compared to Pa? |
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d) |
If the viscosity η of the blood increases (where flow Iv , radius r, and length L are all unchanged |
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compared to a) do you expect the pressure di erence |
Pd di erence across a blood vessel to |
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increase, decrease, or remain the same compared to |
Pa? |
Blood viscosity is chemically related to things like the “stickiness” of platelets and their abundance in the blood. Viscosity and the radius r of blood vessels can be regulated or altered (within limits) by drugs, disease, diet and exercise – all of which have a completely understandable e ect upon blood pressure based on the simple ideas above.
430 |
Week 9: Oscillations |
Problem 6.
A
2H/3 H
water
This problem will help you learn required concepts such as:
•Static equilibrium
•Archimedes Principle
•Simple Harmonic Oscillation
so please review them before you begin.
rgb is fishing in still water o of the old dock. He is using a cylindrical bobber as shown. The bobber has a cross sectional area of A and a length of H, and is balanced so that it remains vertical in the water. When it is floating at equilibrium (supporting the weight of the hook and worm dangling underneath) 2H/3 of its length is submerged in the water. You can neglect the volume of the line, hook and worm (that is, their buoyancy is negligible), and neglect all drag/damping forces. Answer the following questions in terms of A, H, ρw (the density of water), g:
a)What is the combined mass M of the bobber, hook and worm from the data?
b)A fish gives a tug on the worm and pulls the bobber straight down an additional distance (from equilibrium) y. What is the net restoring force on the bobber as a function of y?
c)Use this force and the calculated mass M from a) to write Newton’s 2nd Law for the motion of the bobber up and down (in y) and turn it into an equation of motion in standard form for a harmonic oscillator.
d)Assume that the bobber is pulled down the specific distance y = H/3 and released from rest at time t = 0. Neglecting the damping e ects of the water, write an equation for the displacement of the bobber from its equilibrium depth as a function of time, y(t) (the solution to the equation of motion).
e)With what frequency does the bobber bob? Evaluate your answer for H = 10 cm, A = 1 cm2 (reasonable values for a fishing bobber).
Week 9: Oscillations |
431 |
Problem 7.
L θmax
M
This problem will help you learn required concepts such as:
•Simple Harmonic Oscillation
•Torque
•Newton’s Second Law for Rotation
•Moments of Inertia
•Small Angle Approximation
so please review them before you begin.
A grandfather clock is constructed with a pendulum that consists of a long, light (assume massless) rod and a small, heavy (assume point-like) mass M that can be slid up and down the rod changing L to “tune” the clock. The clock keeps perfect time when the period of oscillation of the pendulum is T = 2 seconds. When the clock is running, the maximum angle the rod makes with the vertical is θmax = 0.05 radians (a “small angle”).
a)Derive the equation of motion for the rod when it freely swings and solve for θ(t) assuming it starts at θmax at t = 0. You may use either force or torque.
b)At what distance L from the pivot should the mass be set so that the clock keeps correct time? As always, solve the problem algebraically first and only then worry about numbers.
c)In your answer above, you idealized by assuming the rod to be massless and the ball to be pointlike. In the real world, of course, the rod has a small mass m and the ball is a ball of radius r, not a point mass. Will the clock run slow or fast if you set the mass exactly where you computed it in part b)? Should you reduce L or increase L a bit to compensate and get better time? Explain.
432 |
Week 9: Oscillations |
Problem 8.
M |
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θ |
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h |
d |
d |
k |
k |
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pivot |
This problem will help you learn required concepts such as:
•Simple Harmonic Oscillation
•Springs (Hooke’s Law)
•Small Angle Approximation
so please review them before you begin.
The pole in the figure has mass M and length h is supported by two identical springs with spring constant k that connect its platform to a table as shown. The springs attach to the platform a distance d from the base of the pole, which is pivoted on a frictionless hinge so it can rotate only in the plane of the page as shown. Gravity acts down. Neglect the mass of the platform.
a)On a copy of the right-hand figure, indicate the forces acting on the pole and platform when the pole tips over as shown, deviating from the vertical by a (small) angle θ.
b)Using your answer to a), find the total torque acting on the system (pole and platform) about the hinged bottom of the pole, and note its direction. Use the small angle approximations sin(θ) ≈ θ; cos(θ) ≈ 1.
c)Find the minimal value for the spring constant k of the two springs such that the pole is stable in the vertical position. This means that a small deviation as above produces a torque that restores the pole to the vertical.
d)For M = 50 kg, h = 1.0 meter, d = 0.5 meter, and springs with spring constant k = 9600 N/m, find the angular frequency with which the pole oscillates about the vertical.
Week 9: Oscillations |
433 |
Advanced Problem 9.
P0 A
y P0
a
This problem will help you learn required concepts such as:
•Bernoulli’s Equation
•Torricelli’s Law
so please review them before you begin.
In the figure above, a large drum of water is open at the top and filled up to a height y above a tap at the bottom (which is also open to normal air pressure). The drum has a cross-sectional area A at the top and the tap has a cross sectional area of a at the bottom.
The questions below help you use calculus to determine how long it will take for the drum to empty. The first two questions and the last question anybody can answer. The one where you actually have to integrate may be di cult for non-math/physics/engineering students, but feel free to give it a try!
a)Find the speed with which the water emerges from the tap. Assume laminar flow without resistance. Compare your answer to the speed a mass has after falling a height y in a uniform gravitational field (after using A a to simplify your final answer, Torricelli’s Law).
b)Start by guessing how long it will take water to flow out of the tank by using dimensional analysis and the insight gained from a). That is, think about how you expect the time to vary with each quantity that describes the problem and form a simple expression with the relevant parameters that has the right units and goes up where it should go up and down where it should go down.
c)Next, find an algebraic expression for the velocity of the top. This is dy/dt.
d)Manupulate the expression and integrate dy on one side, an expression with dt on the other side, to find the time it takes for the top of the water to reach the bottom of the tank. Compare your answer to b) to your answer to d) and the time it takes a mass to fall a height y in a uniform gravitational field. Does the correct answer make dimensional and physical sense? You might want to think a bit about Toricelli’s Law here as well...
e)Evaluate the answers to a) and d) for A = 0.50 m2, a = 0.5 cm2, y(0) = 100 cm.
434 |
Week 10: The Wave Equation |
Optional Problems
Continue studying for the final exam! Only three “weeks” (chapters) to go in this textbook, finals are coming apace!