This page (revision-6) was last changed on 2021-06-24 23:16 by Murray Altheim

This page was created on 2021-06-24 22:55 by Murray Altheim

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Version Date Modified Size Author Changes ... Change note
6 2021-06-24 23:16 2 KB Murray Altheim to previous
5 2021-06-24 23:15 2 KB Murray Altheim to previous | to last
4 2021-06-24 23:15 2 KB Murray Altheim to previous | to last
3 2021-06-24 23:14 2 KB Murray Altheim to previous | to last
2 2021-06-24 22:59 2 KB Murray Altheim to previous | to last
1 2021-06-24 22:55 2 KB Murray Altheim to last

Page References

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Robot Chassis Dynamometer
RobotChassisDynamometer

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At line 5 removed one line
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[{Image src='attach/RobotChassisDynamometer/20200924_163518.jpg' link='attach/RobotChassisDynamometer/20200924_163518.jpg' caption='Robot Chassis Dynamometer (click to enlarge)' width='400' align='right' class='imgFloatRight'}]
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In theory, the inertia that a robot’s wheels see is roughly the robot’s mass ({{Mr}}) times its wheel radius ({{Rr}}) squared, i.e.,
In theory, the inertia that a robot’s wheels see is roughly the robot’s mass (Mr) times its wheel radius (Rr) squared, i.e.,
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Mr * Rr²
Mr * Rr **2
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[{Image src='attach/RobotChassisDynamometer/20200924_163705.jpg' link='attach/RobotChassisDynamometer/20200924_163705.jpg' caption='Robot Chassis Dynamometer, with robot (click to enlarge)' width='400' align='right' class='imgFloatRight'}]
The inertia of a solid flywheel is one half its mass ({{Mrcd}}) times its radius ({{Rrcd}}) squared, i.e.,
The inertia of a solid flywheel is one half its mass (Mrcd) times its radius (Rrcd) squared, i.e.,
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( Mrcd / 2 ) * Rrcd²
( Mrcd / 2 ) * Rrcd **2
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This page (revision-6) was last changed on 2021-06-24 23:16 by Murray AltheimTop