LR - Centripetal Force - lab reports PDF

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Steeven Imbaquingo 06/20/17 PHY 215 Prof. Kibrewossen Tesfagiorgis Centripetal Force Introduction: Centripetal Forces means “center-seeking”, it is provided by gravitational and electrical interactions, correspondingly, for each of these cases. For example, the Earth revolves around the Sun. Another example is the electrons move around the nucleus. Therefore, the centripetal force is what is keeping these objects in orbit. The object has a constant speed when it moves around, but velocity is changing in terms of direction because it is moving in circular motion, so the velocity of the direction is perpendicular to the circular motion. This change is velocity results from centripetal acceleration because of the centripetal force. Objectives: Our objective in this lab is to describe why the centripetal force is necessary for the circular motion. Also, our objective is to explain how the frequency of rotation of the object, mass, and radius affects the magnitude of the centripetal force to form a constant circular motion. Procedures: Manual Centripetal Force Apparatus: 1. First, determine the mass of the bob. Then, modify the position of the vertical pointer rod to the smallest radius as possible. Finally measure the distance of the radius and record it on Data Table 1. 2. Now, attach the bob on the horizontal support along with spring. Then, practice rolling the rotor between your thumb and fingers so that the bob revolves around and passes over the pointer. 3. Next, simultaneously we are going to revolve the bob about 25 revolutions and measure the time. Then, record on table 1. 4. We are going to repeat step 3 three times. After that, we have to calculate the time per revolution of the bob for each trial, and find the average time per revolution of the three 2 πr ; T is the average time per revolution (period). trials: v = T m v2 5. Afterward, we are going to find the centripetal force by using this equation: Fc = r 6. Subsequently, we are going to attach a string to the bob on opposite side with a weight hanger. Then, we are going to add weights to the hanger until the bob is directly aligned with the pointer. Later, we are going to measure of the total weight we added on the

hanger and record it. This weight is directly measure of the centripetal force supplied by the string during rotation. 7. Then, calculate the percent difference between the computed value of centripetal force and the direct measurement of centripetal force. 8. Variation of mass – unscrew the nut that is on top of bob and place 100g, then lock the screw very tightly. We are going to repeat step 3-7. Finally, record it on Data Table 2. 9. Variation of the radius – remove the 100g that was on top of the bob, and lock it. Then, we are going to move the horizontal support arm farther away to provide a larger radius. We are going to repeat step 3-7. Finally record it on Data table 3. Data Table: Data Table 1: to determine period of revolution for computation of centripetal force.

Number of revolution Total Time (s) Time/ Revolution (s/rev)

Trial 1 25rev

Trial 2 25rev

Trial 3 25rev

26.43s 26.16s 26.40s 1.06 s/rev 1.05 s/rev 1.06 s/rev

Mass of bob: 0.4547kg Radius of circular path: 0.150m Average time per revolution: 1.06 s/rev Average speed of bob (v): 0.89m/s Computed value of centripetal force: 2.40N Direct measurement of centripetal force: 2.21N Percent difference: 8.2%

Data Table 2: to observe the effect of varying mass.

Number of revolution Total Time (s) Time/ Revolution (s/rev)

Trial 1 25rev

Trial 2 25rev

Trial 3 25rev

28.13s 28.60s 28.09s 1.13 s/rev 1.14 s/rev 1.12 s/rev

Mass of bob: 0.5547kg Radius of circular path: 0.150m Average time per revolution: 1.13 s/rev Average speed of bob (v): 0.83m/s Computed value of centripetal force: 2.50N Direct measurement of centripetal force: 2.20N Percent difference: 12.8%

Data Table 3: To observe the effect of varying radius

Number of revolution Total Time (s) Time/ Revolution (s/rev)

Trial 1 25rev

Trial 2 25rev

Trial 3 25rev

22.50s 22.14s 22.18s 0.90 s/rev 0.89 s/rev 0.89 s/rev

Mass of bob: 0.4547kg Radius of circular path: 0.185m Average time per revolution: 0.89 s/rev Average speed of bob (v): 1.31m/s Computed value of centripetal force: 4.22N Direct measurement of centripetal force: 4.02N Percent difference: 4.85%

Calculations: Data Table 1: Average time per revolution: 1.06 + 1.05 + 1.06 =1.06 s /rev 3

Average speed of the bob:

v=

2 πr T

2 π (0.150 m) =0.89m/ s 1.06 s/rev Computed value of the centripetal force:

Fc =

m v2 r

(0.4547 kg)( 0.89 m/ s)2 =2.40 N (0.150 m) Directed measurement of centripetal force: m ( 0.225 kg ) 9.81 2 =2.21 N s

(

)

|x 1−x 2| Percent Difference:

 F =m a

(

x1 + x 2 2

)

x 100

|2.21 −2.40 | x 100=8.2 %

( 2.21+22.40 )

Conclusion: In conclusion, we can see that radius, mass, and frequency of the rotation affected the centripetal force. For example, when we kept the radius was in short distance the velocity kept changing direction. However, when we added more mass on the bob the velocity decreased. But, what if we move the radius farther away and remove the extra mass we recently added? Then, the velocity is going to increase because we added more force, and the more force we add in the center, the more acceleration we are going to get. Therefore, the centripetal force is happening in the center, just like in space, the more mass you have in space the more stuff you are going to attract and orbit around you because you have that force and you are pulling to its center....