ic_class_090914

course 201

9/20, 7:52pm

Class 090914Synopsis 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) Pendulum – 6 inches(15.24cm), 70 cpm

1- 725 degrees, 2 pend. cycles

2- 750 degrees, 2.25 cycles

3 – 710 degrees, 2 cycles

4 – 800 degrees, 2.5 cycles

5- 700 degrees, 1.75 cycles

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

-175.4672d/hc

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)

-Pendulum = 15.24cm, 70cpm

- Run1-4cycles, Run2-4 cycles, Run3(w/ rubberband)- 3 cycles, Run4(w/ rubberband)-3 cycles

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

-11.4286cm/hc

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) &&&&

-Pendulum = 15.24cm, 70cpm Ramp 1 = 1ft, Ramp1&Ramp2 = 2 feet, inches to cm = 2.54

you haven't reported anything about how long the ball took to get from one point to another

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

• period = .2 sqrt(length).

&&&& -Each ramp is 1 foot long, or 30.48cm. So each one should take 1.1s.

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

-The average rate of change is 27.71cm/s.

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. &&&&

-The average rate of acceleration is 25.19cm/s^2.

your results aren't connected to your raw data, and you appear to have divided average velocity by change in clock time, which doesn't give you rate of change of velocity with respect to clock time

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: &&&&

-Pendulum = 15.24cm, 70cpm Run 1 = 3 cycles, and 80cm South Run 2 = .5 cycles, 10cm North

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 is positive.

Find acceleration for both trials: &&&&

-Trial 1 = 12.8cm/s^2, Trial 2 - -62.5cm/s^2

it doesn't appear that these accelerations follow from your data; you haven't shown how you got from raw data to conclusions but it looks a lot like the same error I pointed out above.

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): &&&&

- 4.5 blocks up the wall(31cm,each), 1 floor tile away from wall(30.48), pendulum = 18 inches(45.72cm)

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): &&&&

-558cm/hc

Opposing springs

Repeat the opposing-rubber-band experiment using springs.

Report your raw data: &&&&

-Tight rubber band – 10cm to 31cm, 10cm to 34cm, 20cm to 47.5cm

-Loose rubber band – 36cm to 44cm, 38 to 47cm, 52cm to 61.5cm

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

-X = Tight, Y = Loose

-Slope 1 = 3, Slope 2 = 7

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? &&&&

-It’d be much closer to a slope of 1 because the stretch would be spread out among three of the springs instead of just one.

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): &&&&

-The slope would be slightly less due to having paper clips in the chain, which wouldn’t stretch at all, lowering the length you stretch it.

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?

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

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

Solving Equations of Motion

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

-Vo*dT + 1/2A*dT = dS First, we will move Vo*dT over to the other side. 1/2A*dT = dS-Vo*dT Now we’ll get 1/2A by itself. (dS/dT) – Vo = 1/2A Finally, just multiply by 2. A = 2((dS/dT) – 2Vo)

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

-dS=((Vf+Vo)/2)*dT The only thing you have to do is divide both sides by ((Vf+Vo)/2). dS/((Vf+Vo)/2) = dT

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

-Vf^2 = (dS*2a) + Vo^2 First off, we subtract by Vo^2. Vf^2 – Vo^2 = dS*2a The last step is to divide by 2a. (Vf^2 – Vo^2)/2a = dS

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

-A = (Vf-Vo)/dT The first step is to multiply by dT. A*dT = Vf-Vo The final step is to subtract Vf and multiply by -1. –(A*dT) + Vf = Vo

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 Multiply m/s^2 by s. m/s^3

m/s^2 * 1/s = m/s^3, but m/s^2 * s is not equal to m/s^3

1/2 a t^2 &&&&

-1/2m/s^2 * s^2 Multiply 1/2m/s^2 by s^2. 1/2m/s^4

similar error to previous

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

-(m/s –m/s) / s Find the difference of final and initial velocity, then subtract by s. m/s^2

right

2 a `ds &&&&

-m/s^2 * s Multiply m/s^2 by s. m/s^3

m/s^2 * s is not m/s^3 (see previous note)

`ds isn't measure in seconds in the first place

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? &&&&

-Releasing the ball onto the ramp and the ball hitting the bottom 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? &&&&

-Vf = 0m/s, `dT = 2s, `dS = 4m

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? &&&&

-Eq. 1, Vo

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. &&&&

-(deltaS = ((Vf+ Vo)/2)deltaT) The first step will be to bring the deltaT over from the right-hand side to the left side by dividing both sides by deltaT. ((deltaS/deltaT) = (Vf+Vo)/2) The next step is get rid of the fraction on the right side by multiplying both sides by 2. (2(deltaS/deltaT) = (Vf + Vo)) The last step is to get Vf by itself by subtracting Vo by both sides. (2(deltaS/deltaT) -Vo = Vf)

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. &&&&

-(4m = ((Vf + 0m/s)/2)2s) Divide by 2s. (2m/s = (Vf + 0m/s)/2) Multiply by 2. (4m/s = Vf + 0m/s) Subtract 0m/s. (4m/s = Vf)

* 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? &&&&

-Dropping the ball and the ball hitting the 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? &&&&

-A = 10m/s^2, Vo = 0m/s, `ds = 2m

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? &&&&

-Eq. 4, Vf

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? &&&&

-Eq. 3, `dT

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. &&&&

-You start out with the equation, (Vf^2 = (dS * 2A) + Vo^2). Your first step is to multiply the dS and 2A. (Vf^2 = (2AdS) + Vo^2) The last thing you will do is get the square root of everything. (Vf = (2AdS)^.5 + Vo)

(Vf^2 = (2m * 2(10m/s^2)) + 0m^2/s^2) Multiply 2 by 10m/s^2. (Vf^2 = (2m * 20m/s^2) + 0m^2/s^2) Multiply 2m by 20m/s^2. (Vf^2 = 40m^2/s^2 + 0m^2/s^2) Square root everything. (Vf = 40m/s + 0m/s) The answer is *Vf = 40m/s.*

sqrt(40) is not 40, it's about 6.4

otherwise very well done

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? &&&&

-20.9cm/s

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

-12.4cm/s^s

• 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? &&&&

-135.1cm/s

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

-405.8cm/s^s

some of these are off a bit, though the errors are probably minor; however I can't tell what you did from just the final answer so I can't go into detail