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Brand: AELAB
The 3axis gyroscope is used for demonstration and experimental quantitative derivation of the laws of gyrostatics. The following topics can be dealt with experimentally:
• Moment of inertia of the disc
• Turning moment/angular momentum
• Precession
• Nutation
High quality precision3axis gyroscope for demonstration as well as for quantitative determination of gyroscopic laws by means of practical experiments. Experiment apparatus with a shaft that can be tilted and rotated while attached to a stand rod. On one side of the shaft there is a disc mounted on dual ball bearings, while on the opposite side there is a movable counterweight for establishing equilibrium. Fine adjustment is performed by thumb screw at the end of the shaft. To generate external torque an additional weight is provided that can also be moved along the shaft. The shaft’s angle of inclination can be read from an easily readable scale. The disc can be set rotating by hand or by means of a cord. The dual ball bearing system ensures that rotation is nearly frictionless and that rotation continues for lengthy periods of time. The open construction of the gyroscope allows gyroscopic phenomena to be observed easily and clearly.
Specifications:
3Axis Gyroscope: balance status
Demonstration gyroscope: Angle scale
Demonstration gyroscope: Unbalance
Gyroscope disk
Test gyroscope friction
Investigate gyroscope.
From picture above, t_{flywheel} = t_{2; }t_{weight} = t_{1}
if effective Torque t_{eff} = zero (Torque of flywheel and torque of weight are destructive), no Precession happen
See the clip below:
If flywheel is heavier than weight, the gyros deviate to the flywheel, direction of roation like picture below (similar theory above), Precession is clip below:
If flywheel is lighter than weight, the gyros deviate to the weight, then Precession is clip below:
We find out: The larger the deviation between the flywheel and the weight, the higher the frequency of precession.
Because:
if The larger t_{eff}, then the larger dL, according to Equation (6), then the greater Angular velocity W. Watch the clip below:
From formula (6):
Torque t = r x F is constant.
When angular velocity of flywheel w is reduced, then angular momentum L = I. w is reduced.
Leading to an increase in W .
So the frequency of precession is inversely proportional to the speed of the flywheel
See clip below:
NUTATION