ic_class_091007

course 201

10/11 11 pm

Class 091007The first 6 questions are about the experiment we did Monday, allowing a ball to back and forth on a pair of oppositely-inclined ramps until it comes to rest. Most of the remaining questions involve sketches, estimates and explanations. The last problem is a review of something everyone should now know (but it ain't always so).

`q001. Give your raw data for the experiment conducted Monday, with a ball traveling down one incline then up another, until it finally comes to rest.

Report you numbers in the form of an easily-table, including an explanation before or after the table of what the numbers mean.

****

The middle of a sixty centimeter ramp was aligned with the midpoint of a meter stick (50 cm). Thus, our endpoints of the ramps were recorded as 20 cm and 80 cm.

Start at 20 cm, headed in the positive direction

+ to 66 cm

-to 43 cm

+to 58 cm

-to 46 cm

+to 53.5 cm

-to 48.5 cm

+to 52 cm

-to 49 cm

+to 51 cm

-to 50 cm

Then oscillations were too small to record

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`q002. How much distance did the ball cover between the instant of release and the instant at which it came to rest? Give the distance, then explain how you got it from the data you reported in the preceding.

****

164.5 cm

I first subtracted 20 cm from all of our raw data recordings to obtain a start from 0 cm. I then found the difference between each number set, disregarding sign, and added these differences together.

The differences were as follows: 46 cm, 23 cm, 15 cm, 12 cm, 7.5 cm, 5.5 cm, 3.5 cm. 3 cm, 2 cm, 1 cm.

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`q003. The distance down the first ramp is about 30 cm, and the domino supporting it has a thickness of a little less than 1 cm. So the distance the ball traveled on the first ramp alone is more than 30 times the distance of its vertical descent.

Between release and coming to rest (after rolling back and forth for a time) the ball sometimes descends and sometimes ascends, but it ends up lower than it starting point by a vertical distance equal to the thickness of a single domino.

How many times the distance of its vertical descent is the total distance traveled by the ball?

****

Assuming the incline was .9 cm, the total distance traveled is 182.8 times the vertical distance traveled.

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`q004. When the ball descends, does it potential energy increase or decrease? Does its kinetic energy increase or decrease?

When it ascends, does its potential energy increase or decrease? Does its kinetic energy increase or decrease?

Sketch a graph you think might represent the potential energy of the ball vs. clock time, from the instant of release to the instant it comes to rest.

Describe your graph:

****

My graph looks like stair steps, starting high up and descending down to the right. This is because at first, the ball starts up high, with great potential energy, and then as it reaches the base of the first ramp it’s potential energy is lower, but it raises again as it reaches the top of the second ramp, but as it lost some energy propelling itself up the incline, it did not get as far up and its value for potential energy is not as high as it was the first time. This repeats, with potential energy depreciating but still increasing as it reaches its top point on the ramps.

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`q005. On the same graph, sketch the kinetic energy vs. clock time.

Describe this graph, and describe how the two graphs compare.

****

This graph is a series of hills that decrease in size. Kinetic energy starts at zero, then increases significantly as it rolls down the first ramp. Coming up the second ramp causes the kinetic energy to drop, because the ball is slowing, until it comes to baseline at zero when the ball stops to roll back down. The graph then increases again, but not as much as the first hill. As the ball never gets as high as it was the first time, it never gets the chance to build up that much kinetic energy again, and the size of the subsequent hills is much smaller.

Both graphs are approaching zero as time goes on, but the kinetic energy graph reaches zero repeatedly and climbs again over the course of the experiment, while potential energy doesn’t reach zero until the ball stops completely at the end.

&&&&

`q006. Sketch two more graphs, on representing the ball's velocity vs. clock time, and another representing the ball's position vs. clock time.

Describe your graphs.

****

Velocity versus clock time graph is a lot like the graph of kinetic energy versus clock time, as velocity increases as the ball rolls down the ramp and decreases as it rolls up the ramp, until it reaches zero at the top of the ramp. Velocity never reaches the value it had at first again, creating a graph of hills of decreasing size.

Position versus clock time is a graph that increases dramatically at first, then palpitates up and down in a decreasing amount over time. It skyrockets up to 46 cm, then drops to 23 cm, then goes up to 38 cm, then down to 26 cm, then up to 33.5 cm, etc. before eventually flattening out at 30 cm.

`q007. The sketch you copied from the board in class depicts an incline rising from left to right at angle alpha with horizontal. The x axis is directed up the incline. The weight vector is vertical, and makes angle beta with the y axis. Theta is the angle from the positive x axis to the weight vector, as measured in the counterclockwise direction.

Sketch the same figure, but adjust your angles so that the angle of the incline with horizontal is 15 degrees. (If you divide a 90 degree angle into three equal angles, then take half of one of these angles, you will have a 15 degree angle. Using this method you should be able to hand-sketch a 15 degree angle within a couple of degrees.)

Sketch the projection lines for the weight vector, and estimate the lengths of the arrows representing the x and y components of this vector as percents of the length of the arrow representing the weight vector.

Give the following numbers below, in the specified order, with one number to a line:

1. the angle alpha in degrees

2. the angle beta in degrees

3. the angle theta in degrees

4. the angle, in degrees, between the x axis and the horizontal direction

5. the angle, in degrees, between the x axis and the vertical direction

6. the angle, in degrees, between the y axis and the horizontal direction

7. the angle, in degrees, between the y axis and the vertical direction

8. the x component of the weight as a percent of the weight

9. the y component of the weight as a percent of the weight

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1. 15

2. 15

3. 255

4. 15

5. 75

6. 105

7. 15

8. 30%

9. 85%

****

`q008. Repeat the preceding exercise for angle alpha = 10 degrees. You should identify all the quantities you did before, but report here only the x component of the weight as a percent of the weight:

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1. 10

2. 10

3. 260

4. 10

5. 80

6. 100

7. 10

8. 20%

****

`q009. Repeat the preceding exercise for angle alpha = 5 degrees. You should identify all the quantities you did before, but report here only the x component of the weight as a percent of the weight:

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1. 5

2. 5

3. 265

4. 5

5. 85

6. 95

7. 5

8. 15%

****

`q010. Explain how your pictures show why an increasing slope implies and increasing acceleration.

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An increasing slope increases the y component of the graph, the acceleration of gravity in the downward direction, increases, giving the system more potential energy as it rolls down the ramp. This implies increasing acceleration.

****

`q011. Suppose the ball had a weight of 8 Newtons.

Using the percents you estimated previously:

What would be the x component of its weight on the 15 degree ramp?

What would be the x component of its weight on the 10 degree ramp?

What would be the x component of its weight on the 5 degree ramp?

****

On the 15 degree ramp, I estimated an x component of 30%

8 Newtons *.3= 2.4 Newtons

On the 10 degree ramp I estimated an x component of 20%

8 N *.2= 1.6 N

On the 5 degree ramp I estimated an x component of 15%

8 N *.15=1.2 N

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`q012. Suppose the ball had a mass of 3 kilograms. What would be its weight, in Newtons?

Using the percents you estimated previously:

What would be the x component of its weight on the 15 degree ramp?

What would be the x component of its weight on the 10 degree ramp?

What would be the x component of its weight on the 5 degree ramp?

Using Newton's Second Law, assuming that the net force on the ball is equal to the x component of its weight, what then would be its acceleration on the 15 degree ramp?

What would be its acceleration on each of the other ramps?

****

Force in Newtons=m*a

Newtons=3kg (9.8 m/sec^2)

N= 29.4 kg*m/sec^2

On the 15 degree ramp, I estimated an x component of 30%

29.4 Newtons *.3= 8.82 Newtons

On the 10 degree ramp I estimated an x component of 20%

29.4 N *.2= 5.88 N

On the 5 degree ramp I estimated an x component of 15%

29.4 N *.15= 4.41 N

On the 15 degree ramp:

Fnet=m*a

8.82 kg*m/sec^2=3 kg*a

A=2.94 m/sec^2

On the 10 degree ramp:

5.88 kg*m/sec^2=3 kg*a

A=1.96 m/sec^2

On the 5 degree ramp:

4.41 kg*m/sec^2=3 kg*a

A=1.47 m/sec^2

&&&&

`q013. Assume that the weight of the ball is 8 Newtons, as on one of the preceding problems.

Based on your estimates of the x component of the weight:

How much work would be done on the ball by this force if it rolled 5 meters down the ramp?

Assuming it started from rest, how fast would it be going after rolling 5 meters down the ramp?

Assuming it started from rest, what would be its kinetic energy after rolling 5 meters down the ramp?

****

On the 15 degree ramp, I estimated an x component of 30%

29.4 Newtons *.3= 8.82 Newtons

Work=Fnet*`ds

Work=8.82 kg*m/sec^2 (5 m)

Work= 44.1 kg*m^2/sec^2

I am unsure how to find the velocity of the ball or its kinetic energy.

&&&&

`q014. Assume that the weight of the ball is 8 Newtons, as before.

Based on your estimates of the x component of the weight:

How much work would be done on the ball by this force if it rolled 3 meters up the ramp?

Assuming it started with a speed of 6 meters / second, how fast would it be going after rolling 3 meters up the ramp?

Assuming it started with a speed of 6 meters / second, what would be its kinetic energy after rolling 3 meters up the ramp?

****

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`q015. Sketch the tension force for a pendulum which is displaced to an angle of 15 degrees with vertical.

Using an x-y coordinate system with the x axis horizontal, estimate the x component of the tension as a percent of the tension.

Repeat for angles of 10 degrees and 5 degrees.

Give your three estimates below:

****

20%

15%

12%

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`q016. Based on your answers to the preceding, would you expect the acceleration of the pendulum to increase, decrease or remain the same as it swings back to its equilibrium position? Be sure to explain your reasoning.

****

I would expect acceleration to increase because the x component of the graph, Tensionx, increases in length as the angle away from equilibrium increases.

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`q017. Explain why it would or would not be a good idea to use the equations of uniformly accelerated motion to model the motion of a freely swinging pendulum.

****

Unlike the ball on the ramp, the forces on the pendulum change as the pendulum changes position, meaning that it is not accelerating uniformly

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`q018. You should be able to do these review problems in a couple of minutes each. If not, you still have some work to do on projectile motion:

If an object falls freely from rest through a vertical distance of 2 meters, while traveling at a constant horizontal velocity of 250 cm/second, then how far does it travel in the horizontal direction as it falls?

If another object falls freely from rest through the same distance, and in the process of falling travels 40 cm in the horizontal direction, then what is its horizontal velocity?

YYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY

Your solution:

A=9.8 m/sec^2

V0=0

`ds=2m

fV=2.5 cm/sec

`ds horizontal=?

Vf^2=V0^2+2(a)(`ds)

Vf^2=0+2(9.8 m/sec^2)(2 m)

Vf^2= 39.2 m^2/sec^2

Vf=6.3 m/s

Vave=`ds/dt

Vave=vf+v0/2

Vave=6.3 m/sec +0/2

Vave=3.2 m/sec

3.2 m/sec=2 m/`dt

`dt= .63 sec

250 cm/sec *.63 sec= 158 cm/sec

Next:

`dt=.63 sec

V=`ds/`dt

V=40 cm/.63 sec=63.5 cm/sec

confidence rating:

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.............................................

Given solution: Let downward be the positive direction.

The vertical displacement is therefore 2 meters, the vertical acceleration 980 cm/s^2, the initial vertical velocity zero. We can work in units of cm or meters, but should decide this at the beginning. Either express 2 meters as 200 cm, or 980 cm/s^2 at 9.8 m/s^2, then simply use the equations.

The fourth equation gives us vf^2 = v0^2 + 2 a `ds. Substituting the quantities we get vf = 6.4 m/s, approximately. We also get a negative solution, but discard it since it is clear the final velocity is downward.

The average vertical velocity is therefore vAve_y = (0 m/s + 6.4 m/s) / 2 = 3.2 m/s, and the time of fall is

`dt = `ds / vAve = 2 m / (3.2 m/s) = .63 sec, approx..

The horizontal velocity is constant, since gravity doesn't act in that direction and we are neglecting air resistance and other possible forces in the horizontal direction.

Thus the horizontal displacement is

`ds = vAve_x * `dt = 250 cm/s * .63 sec = 160 cm, approx.. This can also be expressed as 1.6 meters.

For the second question the initial vertical velocity and displacement are the same as before so `dt is still .63 sec.

The horizontal displacement is 40 cm, so the constant horizontal velocity is

vAve_x = 40 cm / (.63 s) = 60 cm/s, approx..

Self critique:

ok

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Self-critique rating:

ok

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Homework:

Your label for this assignment:

ic_class_091007

Copy and paste this label into the form.

Report your results from today's class using the Submit Work Form. Answer the questions posed above.

The topics we addressed today in class relate to q_a_'s #11 through 14.

Today q_A_12 and q_a_13 are assigned for the weekend.

class 091007

Class 091007

The first 6 questions are about the experiment we did

Monday, allowing a ball to back and forth on a pair of oppositely-inclined ramps

until it comes to rest.  Most of the remaining questions involve sketches,

estimates and explanations.  The last problem is a review of something

everyone should now know (but it ain't always so).

`q001.  Give your raw data for the experiment

conducted Monday, with a ball traveling down one incline then up another, until

it finally comes to rest.

Report you numbers in the form of an easily-read table,

including an explanation before or after the table of what the numbers mean.

****

&&&&

`q002.  How much distance did the ball cover between

the instant of release and the instant at which it came to rest?  Give the

distance, then explain how you got it from the data you reported in the

preceding.

****

Typically the 25 mm ball will have traveled perhaps 50 cm

when rolling down one 30-cm incline and up another, then will travel about 40 cm

the other way, maybe 32 cm on the next down-and-up roll, etc..  The total

distance usually reported is between about 1.5 m and 3 m.

If you used a smaller ball, as did some groups, the total

distance will be significantly less.

&&&&

`q003.  The distance down the first ramp is about 30

cm, and the domino supporting it has a thickness of a little less than 1 cm. 

So the distance the ball traveled on the first ramp alone is more than 30 times

the distance of its vertical descent.

Between release and coming to rest (after rolling back and

forth for a time) the ball sometimes descends and sometimes ascends, but it ends

up lower than it starting point by a vertical distance equal to the thickness of

a single domino.

How many times the distance of its vertical descent is the

total distance traveled by the ball?

****

The vertical descent is about a centimeter.

A 200 cm total distance would be about 200 times the

vertical descent.

&&&&

`q004.  When the ball descends, does its potential

energy increase or decrease?  Does its kinetic energy increase or decrease? 

When it ascends, does its potential energy increase or

decrease?  Does its kinetic energy increase or decrease? 

Sketch a graph you think might represent the potential

energy of the ball vs. clock time, from the instant of release to the instant it

comes to rest.

Describe your graph:

****

The ball gets lower as it descends, so its gravitational

PE decreases.  (a fuller explanation:  the component of the

gravitational force along the incline is in the same direction as the

displacement so gravity does positive work on the ball; the change in PE being

equal and opposite to the work done ON the ball by gravity, the PE therefore

decreases)

Its speed increases as it descends, so its KE increases.

&&&&

`q005.  On the same graph, sketch the kinetic energy

vs. clock time.

Describe this graph, and describe how the two graphs

compare.

****

KE is up when the ball reaches the bottom of the ramp,

down at the ends.

The ball reaches the 'low' point with less speed each time

than before, so the 'up' KE gets smaller and smaller each time.

The ball takes less and less time to reach the 'low'

point, so the 'up' KE occurs more and more frequently (the horizontal distance

between the 'ups' will get closer and closer to one another).

&&&&

`q006.  Sketch two more graphs, one representing the

ball's velocity vs. clock time, and another representing the ball's position vs.

clock time.

Describe your graphs.

****

no 'given solution' will be provided for this question,

but we will likely look at this in class

&&&&

`q007.  The sketch you copied from the board in class

depicts an incline rising from left to right at angle alpha with horizontal. 

The x axis is directed up the incline.  The weight vector is vertical, and

makes angle beta with the y axis.  Theta is the angle from the positive x

axis to the weight vector, as measured in the counterclockwise direction.

Sketch the same figure, but adjust your angles so that the

angle of the incline with horizontal is 15 degrees.  (If you divide a 90

degree angle into three equal angles, then take half of one of these angles, you

will have a 15 degree angle.  Using this method you should be able to

hand-sketch a 15 degree angle within a couple of degrees.)

Sketch the projection lines for the weight vector, and

estimate the lengths of the arrows representing the x and y components of this

vector as percents of the length of the arrow representing the weight vector.

Give the following numbers below, in the specified order,

with one number to a line:

  1. the angle alpha in degrees
  2. the angle beta in degrees
  3. the angle theta in degrees
  4. the angle, in degrees, between the x axis and the

    horizontal direction
  5. the angle, in degrees, between the x axis and the

    vertical direction
  6. the angle, in degrees, between the y axis and the

    horizontal direction
  7. the angle, in degrees, between the y axis and the

    vertical direction
  8. the x component of the weight as a percent of the

    weight
  9. the y component of the weight as a percent of the

    weight

&&&&

For the 20-degree incline sketched on the board we would

have the following values:

alpha = 20 deg

beta = 20 deg

theta = 250 deg

between the x axis and the

horizontal direction the nearest angle is 20 deg, with the angle from the

axis to the horizontal direction directed clockwise; in the counterclockwise

direction the angle is 160 deg

between the x axis and the

vertical direction the nearest angle is 70 deg, with the angle from the axis

to the horizontal direction directed counterclockwise; in the clockwise

direction the angle is 110 deg

between the y axis and the

horizontal direction the nearest angle is 70 deg, with the angle from the

axis to the horizontal direction directed counterclockwise; in the clockwise

direction the angle is 110 deg

between the y axis and the vertical direction the nearest

angle is 20 deg, with the angle from the axis to the vertical direction directed

clockwise; in the counterclockwise direction the angle is 160 deg

the x component is in the neighborhood of 40% of the

weight

the y component is in the neighborhood of 90% of the

weight

Based on these results you should be able to figure the

results for a 15 degree angle.

For the 15 degree angle, the x and y components will be

about 30% and something over 90%, the latter perhaps as great at 95%.

Your estimates may well have varied somewhat from the

estimates used here.

****

`q008.  Repeat the preceding exercise for angle alpha

= 10 degrees.  You should identify all the quantities you did before, but

report here only the x component of the weight as a percent of the weight:

&&&&

No detailed solution is provided here.

However the x component of the weight will be in the

neighborhood of 20% of the weight, and the y component will be 95% or more of

the weight.

Your estimates may well have varied somewhat from the

estimates used here.

****

`q009.  Repeat the preceding exercise for angle alpha

= 5 degrees.  You should identify all the quantities you did before, but

report here only the x component of the weight as a percent of the weight:

&&&&

No detailed solution is provided here.

However the x component of the weight will be in the

neighborhood of 10% of the weight, and the y component will be nearly equal to

the weight (just a bit less than 100%).

Your estimates may well have varied somewhat from the

estimates used here.

****

`q010.  Explain how your pictures show why an

increasing slope implies and increasing acceleration.

&&&&

The ball accelerates along the ramp, which if the axes are

rotated to the specified position, is in the x direction.

The x component of the weight was seen above to decrease

with decreasing slope, and will therefore increase with increasing angle of

slope.

The ball is accelerated by the x component of the weight,

so increasing slope implies increasing acceleration.

****

`q011.  Suppose the ball had a weight of 8 Newtons.

Using the percents you estimated previously:

What would be the x component of its weight on the 15

degree ramp?

What would be the x component of its weight on the 10

degree ramp?

What would be the x component of its weight on the 5

degree ramp?

****

Assuming that the respective x components are 30%, 20% and

10% of the weight, we would conclude that the components are

.30 * 8 N = 2.4 N (15 deg ramp)

.20 * 8 N = 1.6 N (10 deg ramp)

.10 * 8 N = .8 N (5 deg ramp).

Your estimates may well have varied somewhat from the

estimates used here.

&&&&

`q012.  Suppose the ball had a mass of 3 kilograms. 

What would be its weight, in Newtons?

Using the percents you estimated previously:

What would be the x component of its weight on the 15

degree ramp?

What would be the x component of its weight on the 10

degree ramp?

What would be the x component of its weight on the 5

degree ramp?

Using Newton's Second Law, assuming that the net force on

the ball is equal to the x component of its weight, what then would be its

acceleration on the 15 degree ramp?

What would be its acceleration on each of the other ramps?

****

If released from rest gravity would accelerate the ball at

9.8 m/s^2, so it is exerting force

F = m g = 3 kg * 9.8 m/s^2 = 29 N

on the ball. 

Weight being the force exerted by gravity, this is

therefore the weight of the ball.

On a 15 deg ramp the x component of the weight would be

30% of the weight, according to the estimate being used here, and would

therefore be

.30 * 29 N = 9 N .

On a 10 deg ramp the x component of the weight would be

20% of the weight, according to the estimate being used here, and would

therefore be

.20 * 29 N = 6 N .

On a 5 deg ramp the x component of the weight would be 10%

of the weight, according to the estimate being used here, and would therefore be

.10 * 29 N = 3 N .

&&&&

`q013.  Assume that the weight of the ball is 8

Newtons, as on one of the preceding problems.

Based on your estimates of the x component of the weight:

How much work would be done on the ball by this force if

it rolled 5 meters down the ramp?

Assuming it started from rest, how fast would it be going

after rolling 5 meters down the ramp?

Assuming it started from rest, what would be its kinetic

energy after rolling 5 meters down the ramp?

****

On the 15-degree ramp the x component of the weight would

be 2.4 N, according to the estimates used here.

The x component would be directed down the ramp, so would

be in the same direction as the displacement.

work = force * displacement would therefore be positive,

and we would have

 

The question of how fast the ball is moving is probably

premature at this point.  Theoretically you know enough to figure this out,

but if you did manage it you're doing exceptionally well.

One way to figure out the speed is to notice that the x

component is about 30% of the gravitational force, so if that's the only force

acting in the x direction the acceleration must be 30% that of gravity. 

(So acceleration would be .30 * 9.8 m/s^2 = 3 m/s^2, approx.; `ds is 5 meters

and v0 is 0, and the fourth equation of unif accel motion would give us vf = 5.4

m/s.)

 

We could reason out the KE of the ball using the

work-kinetic energy theorem, or we could just calculate it using the velocity:

Since no other forces act in the x direction, and

since the net force in the y direction is zero (normal force is equal and

opposite to the vertical component of the gravitational force), the net

force is the x component of the gravitational force, which we have estimated

to be 2.4 N.

Since the ball started from rest, its initial KE is

zero. 

The work 12 kg m^2 / s^2 was done by the net force, so

is equal to the change in KE. 

We could therefore conclude that its final KE is 12 kg

m^2 / s^2.

&&&&

`q014.  Assume that the weight of the ball is 8

Newtons, as before.

Based on your estimates of the x component of the weight:

How much work would be done on the ball by this force if

it rolled 3 meters up the ramp?

Assuming it started with a speed of 6 meters / second, how

fast would it be going after rolling 3 meters up the ramp?

Assuming it started with a speed of 6 meters / second,

what would be its kinetic energy after rolling 3 meters up the ramp?

****

&&&&

`q015.  Sketch the tension force for a pendulum which

is displaced to an angle of 15 degrees with vertical.

Using an x-y coordinate system with the x axis horizontal,

estimate the x component of the tension as a percent of the tension.

Repeat for angles of 10 degrees and 5 degrees.

Give your three estimates below:

****

&&&&

`q016.  Based on your answers to the preceding, would

you expect the acceleration of the pendulum to increase, decrease or remain the

same as it swings back to its equilibrium position?  Be sure to explain

your reasoning.

****

&&&&

`q017.  Explain why it would or would not be a good

idea to use the equations of uniformly accelerated motion to model the motion of

a freely swinging pendulum.

****

&&&&

`q018.  You should be able to do these review

problems in a couple of minutes each.  If not, you still have some work to

do on projectile motion: 

If an object falls freely from rest through a vertical

distance of 2 meters, while traveling at a constant horizontal velocity of 250

cm/second, then how far does it travel in the horizontal direction as it falls?

If another object falls freely from rest through the same

distance, and in the process of falling travels 40 cm in the horizontal

direction, then what is its horizontal velocity?

Your solution:

 

 

 

 

 

 

 

 

Confidence rating:

 

Given solution:  Let downward be the positive

direction.

The vertical displacement is therefore 2 meters, the

vertical acceleration 980 cm/s^2, the initial vertical velocity zero.  We

can work in units of cm or meters, but should decide this at the beginning. 

Either express 2 meters as 200 cm, or 980 cm/s^2 at 9.8 m/s^2, then simply use

the equations.

The fourth equation gives us vf^2 = v0^2 + 2 a `ds. 

Substituting the quantities we get vf = 6.4 m/s, approximately.  We also

get a negative solution, but discard it since it is clear the final velocity is

downward.

The average vertical velocity is therefore vAve_y = (0 m/s

+ 6.4 m/s) / 2 = 3.2 m/s, and the time of fall is

`dt = `ds / vAve = 2 m / (3.2 m/s) = .63 sec, approx..

The horizontal velocity is constant, since gravity doesn't

act in that direction and we are neglecting air resistance and other possible

forces in the horizontal direction.

Thus the horizontal displacement is

`ds = vAve_x * `dt = 250 cm/s * .63 sec = 160 cm, approx.. 

This can also be expressed as 1.6 meters.

 

For the second question the initial vertical velocity and

displacement are the same as before so `dt is still .63 sec.

The horizontal displacement is 40 cm, so the constant

horizontal velocity is

vAve_x = 40 cm / (.63 s) = 60 cm/s, approx..

Self critique:

 

 

 

 

 

Self-critique rating:

 

 

 

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Very good. The annotated commentary above is for your reference.