Index: A B C D E F G H I J K L M N O P Q R S T U V W X Y Z
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This page gives a summary of important equations in classical mechanics.1 Nomenclature
- a = acceleration (m/s²)
- F = force (N = kg m/s²)
- KE = kinetic energy (J = kg m²/s²)
- m = mass (kg)
- p = momentum (kg m/s)
- s = position (m)
- t = time (s)
- v = velocity (m/s)
- v0 = velocity at time t=0
- W = work (J = kg m²/s²)
- s(t) = position at time t
- s0 = position at time t=0
- runit = unit vector pointing from the origin in polar coordinates
- θunit = unit vector pointing in the direction of increasing values of theta in polor coordinates
Note: All quantities in bold represent vectors.
2 Defining Equations
2.1 Center of Mass
In the discrete case:
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where is the number of mass particles.
Or in the continuous case:
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where ρ(s) is the scalar mass density as a function of the position vector.
2.2 Velocity
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2.3 Acceleration
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-
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(R = radius of the circle, ω = v/R angular velocity)
2.4 Momentum
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2.5 Force
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- (Constant Mass)
2.6 Impulse
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- if F is constant
2.7 Moment of Intertia
For a single axis of rotation:
2.8 Angular Momentum
- iff v is perpendicular to r
Vector form:
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(Note: I can be treated like a vector if it is diagonalized first, but it is actually a 3×3 matrix)
r is the radius vector
2.9 Torque
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-
if |r| and the sine of the angle between r and p remains constant.
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This one is very limited, more added later. α = dω/dt
2.10 Precession
2.11 Energy
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- if m is constant
- (near the earth's surface)
g is the acceleration due to gravity, one the physical constants.
2.12 Central Force Motion
3 Useful derived equations
3.1 Position of an accelerating body
- if a is constant.
3.2 Equation for velocity
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Classical mechanics
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