Tuesday, May 26, 2015

4-May 2015 Angular Acceleration

Purpose: Part 1: Draw some numerically specific conclusions about the effect on the acceleration of the system of increasing the hanging mass, the radius of the torque pulley, and the rotating mass. Part 2: Determine the experimenta values for the moments of inertia of the disks (or disk combinations) from the data of part 1.

Theory: Part one that a change in mass of the pully, hanging or spinning disk, as well as the radius of the pulley will effect to angular acceleration. Part 2 the moment of inertia for the apparatus can be determined using the data collected in Part 1

Procedure: Determine the mass and radius' of the various disks and pulleys of the apparatus, get the apparatus to spin with both disks and just one, attach a pulley with a string to the apparatus and tie the other end to a known mass, allow the mass to "bob" up and down from the apparatus, and measure for angular acceleration. Compare results for Part 1 and calculate the moments of inertia for Part 2.

Apparatus


Measurements

*The radius and mass of the top steel disk, 6.323 cm and 1361 gams respectively.

*The radius and mass of the bottom steel disk, 6.332 cm and 1348 gams respectively.

*The radius and mass of the top aluminum disk, 6.330 cm and 466 gams respectively.

*The radius and mass of the small pulley, 2.5 cm and 10 gams respectively.

*The radius and mass of the large pulley, 5 cm and 37 gams respectively.

*The hanging mass 25 grams.

Acceleration Graph (lower)


Data


Expt #
grams hanging
Pulley
Disk
rad/s^2 down
rad/s^2 up
average rad/s^2
1
hanging mass
25
small
top steel
0.6026
-0.6522
0.6274
2
hanging mass*2
50
small
top steel
1.207
-1.311
1.259
3
hanging mass*3
75
small
top steel
1.758
-1.949
1.8535
4
hanging mass
25
large
top steel
1.161
-1.272
1.2165
5
hanging mass
25
large
top Al
3.293
-3.595
3.444
6
hanging mass
25
large
Top+ Bottom steel
0.5888
-0.6408
0.6148


Graph of Velocity of spinning disk and hanging mass


"Calculations" Part 1

*Since the pivot is at the center of mass of the apparatus and the acceleration is constant, we know angular acceleration= acceleration/radius of pulley, so the smaller the radius of the pulley the larger angular acceleration.

*Greater tension on the sting should equal a larger torque, and since torque= moment of inertia*angular acceleration, we should conclude that a greater hanging mass (therefore greater tension in the string) should cause higher torque value which would mean a higher angular acceleration.

*From the Velocity graph's we can determine the acceleration and angular acceleration from the falling mass and apparatus respectively from looking at the slopes.

*The acceleration of the mass is 0.02874 m/s^2, and the angular acceleration 0.6124 rad/s^2, while using the large pulley (0.05 m radius). So Angular acceleration equals acceleration divided by the radius(0.02874/0.05), and we get 0.5748 rad/s^2

Conclusion Part 1.

 *The first "calculation" isn't confirmed from the data, when a trail was conducted using the same mass but different radius pulley, the greater radius produced a higher angular acceleration. This was not expected. I believe something must have gone wrong, but I don't know what.

*The second "calculation" was confirmed by the data, as a larger hanging mass did result in a greater angular acceleration.

*The final calculation was "close" to the actual measured angular acceleration, so that confirms the hanging mass' acceleration is the same to the tangential acceleration of the apparatus.

Calculation Part 2

 *Sample



*Results

calculated from Data
0.004663131
0.004642941
0.004870745
0.005034936
0.001448455
-0.000735616


 Conclusion Part 2

*My numbers were far off, I can only assume serious error occurred during measurements of the pulley's and disks, therefore none of my data is useful.

*Ideally the moment of inertia should have matched with the calculations, but they did not.

*Also my calculations didn't take into account friction in the system

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