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The rotational analogue to r F = mr a is r = I r where r is the torque, I is the moment of inertia and r is the angular acceleration.
Typology: Lab Reports
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Objective:
To investigate the relationship between torque and angular acceleration and to verify the work- energy theorem for rotational motion.
Theory:
The rotational analogue to
r F = m
r a is^
r = I
r where^
r is the torque,^ I^ is the moment of inertia and r is the angular acceleration. If we apply a torque to a body that can rotate about a fixed axis, it will undergo an angular acceleration and a change in its angular velocity. Therefore, its rotational kinetic energy will increase. The rotational kinetic energy is given by KE = 1/2 I ^2 , where is the angular velocity (radians per second).
Procedure:
DO NOT ROTATE THE DISK UNTIL AIR PRESSURE IS SUPPLIED
Your instructor will demonstrate proper operation of the apparatus. A steel disk spins about a vertical axis, supported by a thin layer of air that provides a virtually frictionless support. An optical scanner counts stripes on the rim to measure the linear speed of the rim. Angular acceleration is produced by the tension in a cord attached to a small load mass. Although you will work in groups of two, each student should record his or her own data using a different value for the small load mass.
down. That is, the angular acceleration of the disk goes from positive to negative. Add plus and minus signs to your scanner readings to denote clockwise and counterclockwise motion.
Analysis:
Rd where f is the counter frequency in counts per second from the optical scanner, and Rd is the radius of the disk in mm.
the angular acceleration dt
d =.
T x r v v v = , but in our case the tension in the string is perpendicular to the radius of the spool so (^) = Tr.
I =.^ Compute your
experimental value for the inertia of the disk and compare it to the known value: 2 2
I = Md Rd.