physics

Conservation of levamentum

In a recent post, I defined levamentum as the lenticity divided by the mass (or times the vass). Here I show that levamentum is conserved, as momentum is. I will do this in 1D with a result that may be generalized to 3D time. Consider the equation of motion for a particle: (1/m) dℓ/dr = […]

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Dynamics for 3D time

The kinematics of 3D duration (3D time) have been explored here over the past year. Now let’s look at the dynamics of 3D duration. This will be done in 1D in order to allow generalizations to 3D length or 3D duration. Start with momentum, the mass times velocity: p = mv. According to Newton’s second

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Switching space and time

You can measure distance by time. How far away is it? Oh about 20 minutes. But it doesn’t work the other way. When do you get off work? Around 3 miles. – Jerry Seinfeld Actually, you can measure time by distance, as was done above but expressing the time by distance requires that time be

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Space and time expanded

Space-time is relativistic 3D space + 1D time. It obscures the 3D nature of time. The opposite is time-space with 3D time + 1D space, which obscures the 3D nature of space. Both of these have their advantages and disadvantages. To avoid the disadvantage of obscuring 3D space or 3D time use 3D space +

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Synchrony conventions

Reichenbach and Grünbaum noted that “the relation of simultaneity within each inertial reference frame contains an ineradicable element of convention which reveals itself in our ability to select (within certain limits) the value to be assigned to the one-way speed of light in that inertial frame.” (John A. Winnie, “Special Relativity without One-Way Velocity Assumptions:

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