ic_class_090914

course PHY 201

12:06 AMMonday, September 21, 2009

Class 090914

Synopsis of what you should know to date, and the questions you need to get used to asking yourself:

At this point in your course everything you do is done in terms of the concept of an interval, using a few definitions (acceptable abbreviations for these definitions are included)

* the definition of average rate of change (abbreviation: rocDef)

* the definition of average velocity (abbreviation: vAveDef)

* the definition of average acceleration (abbreviation: aAveDef)

* the definition of a graph trapezoid (abbreviation: trapDef)

applied using a few principles

* the principle that all quantities with units must always be expressed in terms of units (abbreviation: unitsPrin)

* the principle that the change of a quantity on an interval is found by subtracting its initial value on that interval from its final value on that interval (abbreviation: changePrin)

expressed in terms of some basic mathematics

* basic arithmetic (including the arithmetic of fractions, and especially multiplication and division of fractions)

* the basic rules of algebra (rudimentary factoring (mostly of monomials), adding same quantity to both sides of an equation, multiplying both sides by same quantity)

* very basic geometry, especially the geometry of a trapezoid (average altitude at midpoint, average altitude average of initial and final altitudes, equal-area rectangle, slope of a line segment, area of a rectangle)

When considering an interval you should ask the following questions:

* What events define the beginning and end of the interval?

* What quantities are known at the beginning and end of the interval?

* Do we know the change in any quantity from the beginning to the end of the interval?

* Which of the known quantities are rates of change, and if any are, what is the definition of each rate of change?

If we represent the known information on a velocity vs. clock time trapezoid, that trapezoid has two altitudes, a width or base, a slope and an area. If we know any three of these quantities, we can figure out the rest.

* What are the units of each of these quantities?

* Do we know either, or both, of the quantities given by the 'graph altitudes' of the trapezoid?

* Do we know the quantity given by the slope of the trapezoid?

* Do we know the quantity given by the width, base or 'run' of the trapezoid (all three words refer to the same quantity)?

* Do we know the quantity given by the altitude of the equal-area rectangle (the same as the quantity represented by the average altitude of the trapezoid)?

* In summary, do we know three of the five quantities, and if so how do we find the other two?

If we consider the v0, vf, `dt trapezoid we get the equations of uniformly accelerated motion. If we consider the definitions of average velocity and average acceleration, we can verbally and/or algebraically work out the equations of uniformly accelerated motion. These equations allow us, if we know three of the quantities v0, vf, `dt, a and `ds, to find the other two.

* Of the five quantities v0, vf, `dt, a and `ds, which do we know?

* Which of the four equations of uniformly accelerated motion include three of these five quantities (depending on which three quantities we know, there might be one or two equations that include all three)?

* For every equation which includes three of the five quantities, there is a single unknown quantity. For each such equation, what is that quantity?

* Using basic Algebra I, solve each such equation for the unknown quantity (you may prefer to avoid solving the third equation for `dt, since that equation is quadratic in `dt and the solution might at this stage be confusing).

* Substitute your known values into the solved expression (including units with every quantity) and simplify (this includes the expressions for the units).

At this stage of the course, a few students completely understand these representations, and a few more are well on their way to doing so. The majority of the class could, however, benefit from checking their work on any problem involving motion against this list. With practice the puzzle of uniformly accelerated motion will fit together. When it does, you will have a good foundation for the rest of the course.

You will be asked this week to apply these ideas to a series of problems and experiments, while we also continue to work with the idea of forces.

Brief Experiments

Rotating Strap

Rotate a strap on top of a die and see through how many degrees it rotates (within +- 10 degrees, which you can easily estimate) and how long it takes to coast to rest (accurate to within 1/4 of a cycle of the fastest pendulum you can reasonably observe).

Do this for at least five trials, with as great a range as possible of rotational displacements.

Report your raw data (including data sufficient to determine the length of your pendulum in centimeters) &&&&

9 half-cycles, 810 degrees

4 half-cycles, 90 degrees

7 half-cycles, 250 degrees

20cm pendulum (on paper ruler)

Work out the average rate of change of rotational position (in degrees) with respect to clock time (in half-cycles of your pendulum). &&&&

Change in position with respect to clock time = ave. velocity

ave vel = `ds / `dt

= (810 degrees - 0 degrees) / (9 half-cycles - 0 half-cycles)

= 810 degrees / 9 half-cycles

= 90 degrees / half-cycle

= 90 degrees / 4 half-cycles

= 22.5 degrees / half-cycle

= 250 degrees / 7 half-cycles

= 35.714 degrees / half-cycle

Atwood machine

Your instructor will operate the apparatus and tell you the displacement of the system, and the number of excess paperclips. You time it for each trial. The displacement of the system is 80 cm from start to stop.

Report your raw data (including data sufficient to determine the length of your pendulum in centimeters) &&&&

8 half-cycles, 80cm

5.5 half-cycles, 80cm (+1 rubber band)

20cm pendulum (on paper ruler)

Work out the average rate of change of position (in cm) with respect to clock time (in half-cycles of your pendulum). &&&&

change in position with respect to clock time = ave velocity.

ave vel = `ds / `dt

= (80cm - 0cm) / (8 half-cycles - 0 half-cycles)

= 80 cm / 8 half-cycles

= 80 cm / half-cyles

= 80cm / 5.5 half-cycles

= 14.545 cm / half-cycle

Ball down two ramps

Set up a two-ramp system, the first with a 'two-quarter' slope and the second with a 'one-domino' slope.

Time the system from release at the start of the first ramp to the end of the first ramp, determining the time interval as accurately as possible, using synchronization between your pendulum and the initial and final events for each interval.

Do the same for the interval from release at the start of the first ramp to the end of the second ramp.

Report your raw data (including data sufficient to determine the length of your pendulum in centimeters) &&&&

4.5 half-cycles to end of first ramp

7.5 half-cycles to end of second ramp

30 cm pendulum

1ft (30.48 cm) displacement

Find the time spent on each ramp, seconds, using the approximate formula

* period = .2 sqrt(length).

&&&&

period = .2 sqrt(length)

= .2 sqrt(30 cm)

= 1.095 seconds

Assuming the period is 1 full cycle of the pendulum:

time on first ramp = 1.095 sec * (4.5 half-cycles / 2 half-cycles)

= 1.095 sec * 2.25

= 2.464 sec

time on second ramp = 1.095 sec * [(7.5 half-cycles - 4.5 half-cycles) / 2 half-cycles]

= 1.095 sec * (3 half-cycles / 2 half-cycles)

= 1.095 sec * 1.5

= 1.643 sec

Work out the average rate of change of position (in cm) with respect to clock time (in seconds) for the motion on each ramp. &&&&

first ramp ave vel = `ds / `dt

= (30.48cm - 0cm) / (2.464 sec - 0 sec)

= 30.48cm / 2.464 sec

= 12.37 cm / sec

second ramp ave vel = `ds / `dt

= 30.48cm / 1.643 sec

= 18.55 cm / sec

Work out the average rate of change of velocity (in cm/s) with respect to clock time (in seconds) for the motion on each ramp. &&&&

first ramp a_ave = (vf - v0) / `dt

= (12.37 cm / s - 0 cm / s) / 2.464 sec

= 12.37 cm / s / 2.464 sec

= 5.02 cm / s^2

second ramp a_ave = (vf - v0) / `dt

= (18.55 cm / s - 12.37 cm / s) / 1.643 sec

= 6.18cm / s / 1.643 sec

= 3.761 cm / s^2

Hotwheels car

The hotwheels car will be passed along from one group to the next. Make at least one good observation of the displacement and time required in both the north and south directions.

Report raw data: &&&&

54 cm, 4.5 half-cycles (north)

75cm, 4 half-cycles (south)

20cm (on paper ruler) pendulum

Indicate your choice of north or south as the positive direction, and stick with this choice for the rest of the analysis of this experiment: &&&&

north direction is positive direction

Find acceleration for both trials: &&&&

north:

a_ave = (vf - v0) / `dt

= [(`ds / `dt) - v0] / `dt

= [(54 cm / 4.5 half-cycles) - 0 cm / half-cycle] / 4.5 half-cycles

= [(12 cm / half-cycle) - 0 cm / half-cycle] / 4.5 half-cycles

= 12 cm / half-cycle / 4.5 half-cycles

= 2.667 cm / half-cycle^2

south:

a_ave = (vf - v0) / `dt

= [(`ds / `dt) - v0] / `dt

= [(-75 cm / 4 half-cycles) - 0 cm / half-cycle] / 4 half-cycles

= [(-18.5 cm / half-cycle) - 0 cm / half-cycle] / 4 half-cycles

= -18.5 cm / half-cycle / 4 half-cycles

= -4.625 cm / half-cycle^2

Dropped object timed using pendulum

Drop an object to the floor at the same instant you release a pendulum whose equlibrium position is the wall.

Adjust the length of the pendulum and/or the height of the object until the pendulum reaches equlibrium at the same instant the ball reaches the floor.

Report your raw data, including pendulum length and distance to floor (including distance units): &&&&

66cm pendulum dropped at 90 degrees

dime dropped at table height, 133cm

Figure out the acceleration of the falling object in units of distance (using whatever distance unit you specified above) and clock time (measured in number of half-cycles): &&&&

clock time is 1 quarter-cycle of a pendulum

change in position of dime is 133cm

ave vel = `ds / `dt

= 133 cm / 1 quarter-cycle

= 133cm / quarter-cycle

a_ave = (vf - v0) / `dt

= 133 cm / quarter-cycle / 1 quarter-cycle

= 133 cm / quarter-cycle^2

Opposing springs

Repeat the opposing-rubber-band experiment using springs.

Report your raw data: &&&&

1st measure (small stretch) 33.5cm to 40cm sm, 1 to 22cm lg

2nd measure (med stretch) 30cm to 40cm sm, 1 to 26cm lg

3rd measure (lg stretch) 24cm to 40cm sm, 1 to 30cm lg

Report the average slopes between the points on your graph: &&&&

slope = rise / run

= `dy / `dx

= (10 - 6.5) / (25 - 21)

= 3.5 / 4

= 0.875

= (16 - 10) / (29 - 25)

= 6 / 4

= 1.5

If you were to repeat the experiment, using three of the 'stretchier' springs instead of just one, with all three stretched between the same pair of paper clips, what do you think would be the slope of your graph? &&&&

The slope of the graph would even out and come closer to a 1/1 ratio.

terminology note: for future reference we will use the term 'parallel combination' to describe the three rubber bands in this question

If you were to repeat the experiment using three of the 'stretchier' springs (all identical to the first), this time forming a 'chain' of springs and paper clips, what do you think would be the slope of your graph? There are different ways of interpreting this question; as long as your answer applies to a 'chain', as described, and as long as you clearly describe what is being graphed, your answer will be acceptable (this of course doesn't imply that it will be correct): &&&&

I think the series of springs would all have a similar ""stretch"" factor, causing the slope to be close to 1/1.

terminology note: for future reference we will use the term 'series combination' to describe the three rubber bands in this question

We haven't yet defined force, energy and power, so you aren't yet expected to come up with rigorously correct answers to these questions. Just answer based on your current notions of what each of these terms means:

If each of the 'stretchier' springs starts at its equilibrium length and ends up stretched to a length 1 cm longer than its equilibrium length, then:

* Which do you think requires more force, the parallel or the series combination?&&&&

I think it might take more force to stretch the parallel strings since their strength is combined over a shorter disance.

* Which do you think requires more energy, the parallel or the series combination?&&&&

I think the parallel series will require more energy since it requires more force.

* Which do you think requires more power, the parallel or the series combination?&&&&

I think the parallel series will require more power since it requires more force and energy.

Solving Equations of Motion

Solve the third equation of motion for a, explaining every step. &&&&

`ds = V0 `dt + 1/2 a `dt^2 first subtract v0 `dt

`ds - v0 `dt = 1/2 a `dt^2 then divide by 1/2 `dt^2

a = (`ds - v0 `dt) / (1/2 `dt^2)

Solve the first equation of motion for `dt, explaining every step. &&&&

`ds = [(vf + v0) / 2 ] * `dt divide by [(vf + v0) / 2 ]

`dt = `ds / [(vf + v0) / 2 ]

Solve the fourth equation of motion for `ds, explaining every step. &&&&

vf^2 = v0^2 + 2 a_ave `ds subtract v0^2

vf^2 - v0^2 = 2 a_ave `ds divide by 2 a_ave

`ds = (vf^ - v0^2) / 2 a_ave

Solve the second equation of motion for v0, explaining every step. &&&&

a_ave = (vf - V0) / `dt mutliply by `dt

a_ave * `dt = vf - v0 subtract vf

a_ave * `dt - vf = - v0 multiply by -`

-a_ave * -`dt + vf = v0

Units calculations with symbolic expressions

Using SI units (meters and seconds) find the units of each of the following quantities, explaining every step of the algebra of the units:

a * `dt &&&&

m/s^2 * s

m/s^2 * s / 1 realize seconds as seconds - seconds / 1

m * s / s*s multiply fractions, realize s^2 as s * s

m / s 1 of the seconds divides out

1/2 a t^2 &&&&

1/2 m/s^2 s^2

1/2 * (m / s * s) * (s * s / 1) realize as fractions

(m * s * s) / 2 * s * s multiply fractions (eliminating 1's since multiplying)

m / 2 seconds divide out

(vf - v0) / `dt &&&&

(m/s - m/s) / s

m/s / s m/s - m/s = m/s

(m / s) / (s / 1) realize as fractions

(m / s) * (1 / s) invert and multiply

m / s * s

m / s^2

2 a `ds &&&&

2 m/s^2 * m

(2 / 1) * (m / s * s) * (m / 1) realize as fractions and factor power

(2 * m * m) / (s * s) multiply fractions

2 m^2 / s^2 combine terms

Identifying initial and final events and kinematic quantities

* Exercise 1: A ball is released from rest on a ramp of length 4 meters, and is timed from the instant it is released to the instant it reaches the end of the ramp. It requires 2 seconds to reach the end of the ramp.

What are the events that define the beginning and the end of the interval? &&&&

initial event = ball release

final event = ball reaches end of the ramp

Write down on your paper the symbols v0, vf, a, `dt, `ds.

From the given information you know the values of three of the five quantities. What are the known quantities? &&&&

v0 = 0 m/s

`ds = 4 m

`dt = 2 s

On your paper circle the symbols for the three quantities you know.

Now write down all four equations, and circle the symbols for the three quantities you know.

Write down an equation which includes all three symbols, and circle these symbols in the equation. Which equation did you write down, and which symbol was not circled? &&&&

`ds = [ (vf + v0) / 2 ] * `dt

vf is not circled

Solve this equation for the non-circled variable and describe the steps necessary to do so. If your algebra is rusty you might find this challenging, but as before make your best attempt. &&&&

`ds = [ (vf + v0) / 2 ] * `dt divide by `dt

`ds / `dt = (vf + v0) / 2 multiply by 2

(`ds / `dt) * 2 = vf + v0 subtract v0

vf = [(`ds / `dt) * 2] - v0

Having solved the equation as best you can, substitute the values of the three known quantities into that equation. Then simplify your expression to get the value of the unknown quantity. Again, do your best. &&&&

vf = [(`ds / `dt) * 2] - v0

vf = [(4m / 2s) * 2] - 0

vf = (2 m/s * 2)

vf = 4 m / s

* Exercise 2: A ball is dropped from rest and falls 2 meters to the floor, accelerating at 10 m/s^2 during its fall.

What are the events that define the beginning and the end of the interval? &&&&

initial event is ball dropped from rest

final event is ball reaches floor

Write down on your paper the symbols v0, vf, a, `dt, `ds.

From the given information you know the values of three of the five quantities. What are the known quantities? &&&&

`ds = 2m

a_ave = 10 m/s^2

v0 = 0

On your paper circle the symbols for the three quantities you know.

Now write down all four equations, and circle the symbols for the three quantities you know.

Write down the one equation which includes all three symbols, and circle these symbols in the equation. Which equation did you write down, and which symbol was not circled? &&&&

vf^2 = v0^2 + 2 a_ave `ds

vf is not circled

There are two equations which each contain three of the five symbols. Write down the other equation and circle the three known symbols in the equation. Which equation did you write down, and which symbol was not circled? &&&&

`ds = v0 `dt + `/2 a `dt^2

`dt is not circled

One of your equations has `dt as the 'uncircled' variable. You want to avoid that situation (though if you're ambitious you may give it a try). Solve the other equation for its non-circled variable (which should be vf) and describe the steps necessary to do so. If your algebra is rusty you might find this challenging, but as before make your best attempt. &&&&

vf^2 = v0^2 + 2 a_ave * `ds take the sqrt of both sides

vf = sqrt( v0^2 + 2 a_ave * `ds )

Having solved the equation as best you can, substitute the values of the three known quantities into that equation. Then simplify your expression to get the value of the unknown quantity. Again, do your best. &&&&

vf = sqrt( v0^2 + 2 a_ave * `ds )

vf = sqrt( 0m/s^2 + 2 (10m/s^2) * 2m )

vf = sqrt( 0m/s^2 + 20m/s^2 * 2m )

vf = sqrt(40m/s^2)

vf = 6.325 m/s

Additional Exercises

* Exercise 3: A pendulum completes 90 cycles in a minute. A domino is 5 cm long.

There are four questions, with increasing difficulty. Based on typical performance of classes at this stage of the course, it is expected that most students will figure out the first one, while most students won't figure out the last (your instructor will of course be happy if the latter is an underestimate).

Here are the questions:

* If an object travels through a displacement of 7 dominoes in 5 half-cycles, then what is its average velocity in cm/s? &&&&

Since a domino is 5 cm long, the displacement interval is 7 dominoes * 5 cm = 35 cm

Since the pendulum completes 90 cycles in a minute, it takes 90 cycles / 60 sec = 1.5 cycles to make a second.

Since 5 half-cycles is 2.5 cycles = 2.5 cycles * 1.5 sec = 3.75 seconds is our time interval.

ave vel = `ds / dt

= 35 cm / 3.75 seconds

= 9.333 cm/s

* If that object started from rest and accelerated uniformly, what was its average acceleration in cm/s^2? &&&&

we must solve the 1st equation of motion for vf to determine average acceleration (luckily we did this in exercise 1).

Since the object starts at rest, we know v0 = 0 cm/s

`ds = (vf + v0) / 2 * `dt

vf = [(`ds / `dt) * 2] - v0

vf = [(35 cm / 3.75 s) * 2] - 0 cm/s

vf = (9.333 cm/s) * 2

vf = 18.666 cm / 2

With a known vf, we have everything we need to find ave acceleration:

a_ave = (vf - v0) / `dt

= (18.666 cm / s - 9.333 cm / s) / 3.75 s

= (2 cm / s) / 3.75 s

= 0.533 cm/s^2

* From observations, the average velocity of the ball is estimated to be 9 dominoes per half-cycle. What is its average velocity in cm/sec? &&&&

9 dominoes * 5cm = 45 cm

9 dominoes / 1 half-cycle = 45 cm / x sec

9 dominoes * x s / 1 half-cycle = 45 cm

9 dominoes * x s = 45 cm

x = 5 s

45cm / 5s

9cm / s

* Its acceleration is observed to be 5 dominoes / (half-cycle)^2. What is its acceleration in cm/s^2? &&&&

5 dominoes * 5cm = 25cm

5 dominoes / 1 half-cycle^2 = 25 cm / x sec^2

5 dominoes * x sec^2 / 1 half-cycle^2 = 25 cm

5 dominoes * x sec^2 = 25 cm * 1 half-cycle^2

5 dominoes * x sec^2 = 25 cm

x sec^2 = 5 cm

x sec = `sqrt(5 cm)

x = 2.236 sec

25cm / 2.236 sec^2

5 cm / sec^2

That seems impossible, so I'm guessing I'm wrong.

Homework:

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