Kinematics
| Symbol | Measured in | Description |
|---|---|---|
| S | m | distance travelled |
| v | m/s | velocity |
| t | s | time |
| x | m | coordinate |
| a | m/s2 | acceleration |
| ω | s-1 | angular velocity |
| T | s | period |
| ν | Hz | frequency |
| ε | s-2 | angular acceleration |
| R | m | radius |
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Uniform motion: ν = const
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Uniformly accelerated motion:
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Curvilinear motion:
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Rotational motion:
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Velocity and acceleration:
Dynamics and statics
| Symbol | Measured in | Description |
|---|---|---|
| F | N | force |
| P | kg*m/s | momentum |
| a | m/s2 | acceleration |
| m | kg | mass |
| v | m/s | velocity |
| p | N | the weight of a body |
| g | m/s2 | acceleration of free fall |
| E | J | energy |
| A | J | work |
| N | W | power |
| t | s | time |
| I | kg*m2 | moment of inertia |
| L | kg*m2/s | angular momentum |
| M | N*m | torque |
| ω | s-1 | angular velocity |
When ∑ F = 0 => v = const
Newton's second law:
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Newton's third law:
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The fundamental law of dynamics for non-inertial frames of reference.
ma=ma0+Finert ,where a is the acceleration in the non-inertial frame and a0 that in the inertial frame of reference.
The velocity of the centre of mass:
ma=ma0+Finert ,where a is the acceleration in the non-inertial frame and a0 that in the inertial frame of reference.
The velocity of the centre of mass:
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The law of universal gravitation:
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The weight of a body:
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The force of friction:
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Hooke's law:
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Hooke's law: σ = Eε, where E is Young's modulus.
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The dynamics and statics of rotational motion:
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| system | axis | I |
| a point on a circle | the axis of symmetry | mR2 |
| a rod | through the middle | 1/12 mR2 |
| a rod | through the end | 1/3 mR2 |
| a solid sphere | through the centre of the sphere | 2/5 mR2 |
| a spherical shell | through the centre of the shell | 2/3 mR2 |
| a ring or a thin-walled cylinder | the axis of symmetry | mR2 |
| a disc, a solid cylinder | the axis of symmetry | 1/2 mR2 |
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Potential and kinetic energy. Power:
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The law of conservation of energy:
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