Difference between revisions of "M2"
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| − | [[M2 Centre of Mass|Centre of Mass]] | + | ==[[M2 Centre of Mass|Centre of Mass]]== |
| − | + | {{:M2 Centre of Mass}} | |
| − | [[M2 Collisions|Collisions]] | + | ==[[M2 Collisions|Collisions]]== |
| − | + | {{:M2 Collisions}} | |
| − | [[M2 Kinematics|Kinematics]] | + | ==[[M2 Kinematics|Kinematics]]== |
| − | + | {{:M2 Kinematics}} | |
| − | [[M2 Statics|Statics]] | + | ==[[M2 Statics|Statics]]== |
| − | + | {{:M2 Statics}} | |
| − | [[M2 Work, Energy and Power|Work, Energy and Power]] | + | ==[[M2 Work, Energy and Power|Work, Energy and Power]]== |
| + | {{:M2 Work, Energy and Power}} | ||
Revision as of 09:18, 25 June 2014
Centre of Mass
- Centre of mass of a discrete mass distribution in one or two dimensions
- Centre of mass of uniform plane figures and simple composite plane figures
- Equilibrium of a plane lamina
Collisions
- The impulse-momentum principle (in vector form)
- Conservation of linear momentum
- Newton's law of restitution for impact of elastic particles
- Loss of mechanical energy due to impact
- Successive impacts of up to three particles or two particles and a smooth plane surface
Kinematics
- Motion in a vertical plane with constant acceleration, e.g. under gravity
- Simple cases of motion of a projectile
- Velocity and acceleration when displacement is a function of time
- Differentiation and integration of a vector wrt time
Statics
- Moment of a force
- Equilibrium of rigid bodies
Work, Energy and Power
- Kinetic and potential energy
- Work and power
- The work-energy principle
- Principle of conservation of mechanical energy
