Kinetics of Rigid Bodies: Work and Energy

Example: Falling Rod

Example

A 10 kg slender rod of length L=2L=2 m is released from rest from a horizontal position. It rotates about a pin at one end OO. Find its angular velocity when it is vertical.

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Example: Sphere Rolling Down an Incline

Example

A solid sphere of mass m=5m=5 kg and radius r=0.2r=0.2 m is released from rest at the top of an incline of height h=2h=2 m. It rolls without slipping. Determine the velocity of its center of mass at the bottom of the incline.

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Example: Work of a Couple Moment

Example

A constant couple moment M=50 NmM = 50 \text{ N}\cdot\text{m} is applied to a flywheel of mass m=20 kgm=20 \text{ kg} and radius of gyration k=0.3 mk=0.3 \text{ m}. The flywheel starts from rest. Using the principle of work and energy, determine the angular velocity of the flywheel after it has completed 5 full revolutions.

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Example: Conceptual Case Study - Energy Dissipation in Braking Systems

Example

Disc brakes on a car utilize friction pads to slow down the rotation of a wheel hub. Analyze the operation of disc brakes using the work-energy principle for a rigid body. Discuss the transformation of kinetic energy and the thermal implications of non-conservative work during emergency braking.

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Example: Conceptual Case Study - Energy Storage in Flywheels

Example

Flywheel energy storage systems (FESS) are used to store energy electrically by converting it into rotational kinetic energy. They are often used for grid load-leveling or uninterrupted power supplies (UPS). Analyze the design parameters that dictate a flywheel's energy capacity and the primary limitations based on rigid body kinetics and material strength.

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