iSoul Time has three dimensions

Tag Archives: Physics

Motion measurements

As described in the previous post here, the three dimensions of motion are axes for traveling along (length) or revolving around (time).

A measure of motion may be either (1) dependent on the the target motion, or (2) independent of the target motion. A measure that is independent is either available prior to or separately from the target motion. For example, an independent measure may be determined by agreement, such as the length of a race, or it may measure another motion, such as the motion of a clock, which is then correlated with the target motion.

A standard clock measures time because it measures rotations around an axis as an angle. A length clock measures rotations about an axis as a length. With constant rates of rotation constant, there is a fixed ratio between the two kinds of clock.

A device that measures its own internal motion may be called an autometer. A clock is an example of an autometer. The internal motion of an autometer can be correlated with a target motion. For clocks this is called synchronization. For a length clock this is called symmacronization.

An odometer is a measurement device that depends on its target motion. The standard odometer measures length of travel. A time odometer, or trip-timer, measures time of travel. A trip-timer is a stopwatch that is on only while the target motion takes place. If there is a stop in the target motion, then the trip-timer also stops. So the trip-timer measures time of motion rather than elapsed time.

A device that measures a quantity of motion need not be attached to the moving body. The theory of relativity deals with the remote measurement of quantities of motion. A device that is attached to the moving body produces proper measures such as proper length or proper time.

Motion coordinates

As a thought experiment, consider a rifle bullet, conceived of as an inertial projectile, fired at a target. Let the bullet itself be a source of measurement units: there is the length of the bullet and the rotation of the bullet. The extent of the motion of the bullet to the target could then in principle be measured as a number of bullet lengths and a number of rotations.

Length is the number of bullet lengths. Time is the number of bullet rotations. Thus length is essentially a linear measure and time is essentially a rotational measure. Length is generalized as the correspondence of the motion to a linear object, a rigid rod or ruler, which forms the basis of space. Time is generalized as the correspondence of the motion to a rotational object, a clock, which forms the basis of (abstract) time.

A rifle bullet provides a way to conceive of motion coordinates. Consider individually labeled rifle bullets continually fired from a common origin toward three orthogonal directions. The coordinates of a particular motion are then the labels on the coordinates that correspond to the motion. This means there are three pairs of coordinates: two for each bullet. These axes are the six degrees of freedom.

Motion conceived as a length function of time means that each for each rotational coordinate there corresponds its paired length coordinate. Motion conceived as a time function of length means that for each length coordinate there corresponds one paired rotation coordinate.

In conclusion, there are three dimensions of mobility. There are three dimensions for each measure of the extent of motion, which totals six dimensions. For ordinary purposes, the three dimensions of motion are sufficient, with space and time kept separate. But for science, which seeks a unified treatment, space and time should be united into six dimensions.

Dual Lorentz Transformation

Victor Yakovenko has a derivation (see here) of the Lorentz Transformation (LT) in which he uses “only the equivalence of all inertial reference frames and the symmetries of space and time.” Because of the use of (spatial) reference frames and velocity, this is not completely symmetric. As we have seen, there is a dual Lorentz Transformation. Let us follow Yakovenko’s derivation but with reference timeframes and legerity (matrix forms omitted).

1) Let us consider two inertial reference timeframes P and P´. The reference timeframe P´ moves relative to P with legerity u along the t1t axis. We know that the coordinates t2 and t3 perpendicular to the legerity are the same in both reference timeframes: t2 = t2´ and t3 = t3´. So, it is sufficient to consider only transformation of the coordinates x and t from the reference timeframe P to = fx(x; t) and t´ = ft(x; t) in the reference timeframe P´.

From translational symmetry of space and time, we conclude that the functions fx(x, t) and ft(x, t) must be linear functions. Indeed, the relative distances between two events in one reference timeframe must depend only on the relative distances in another timeframe:

 t´1t´2 = ft(x1x2, t1t2),     x´12 = fx(x1x2, t1t2).          (1)

Read more →

Length clock

A time clock is a device that measures a constant rate of internal motion. Time clocks are synchronized to a common event and rate of internal motion. A time clock is used by correlating its internal measure with other motions and events. The unit of measure for a time clock is normally a unit of time but even if it is a unit of length, the constant rate means the length correlates to a time.

A length clock, also called an odologe, is a device that measures a constant rate of external motion. Length clocks are symmacronized to a common event and rate of external motion. A length clock is used by correlating its external measure with other motions and events. The unit of measure for a length clock is normally a unit of length but even if it is a unit of time, the constant rate means the time correlates to a length.

In general, a device to measure length need not run at a fixed rate, or “run” at all, such as a ruler. An orientation toward length rather than time is comparable to the Myers-Briggs-Jung perceptive rather than judging personality type (e.g., see here), in which “time” is perceived less by a time clock and more by something like the tasks remaining or the distance remaining on a trip (as measured by landmarks).

Modern cultures run on a time clock but ancient cultures ran on a different sense of time. I hypothesize that their sense of time is what the length clock measures. They measure what “time” it is by their length from a reference site, for example, how close they are to Jerusalem for the holy days. It is the same with any trip: one can measure the progress by either the elapsed time or the length of distance remaining to the destination.

Natural cyclical movements such as the positions of migrating birds could be used for an informal length clock. A consistent length clock requires a repeatable motion at a fixed rate. There is a constant relationship with such a device and a time clock, so in a sense they are interchangeable.

Symmetric relativity

Although there are many experimental methods available to measure the speed of light, the underlying principle behind all methods [is] the simple kinematic relationship between constant velocity, distance and time given below:

c = D / t                     (1)

In all forms of the experiment, the objective is to measure the time required for the light to travel a given distance. (Ref.)

From the perspective of the experimenter, light is an object whose speed is to be determined. Even though the distance traversed is fixed, it is placed in the numerator because this speed is to be compared with the speeds of other objects. For the same reason the quantity to be measured, time, is placed in the denominator.

But if we take the perspective of the experiment, of what is measured, then the fixed distance is the independent variable, which is placed in the denominator. The dependent variable is the time, which is placed in the numerator, so the pace of light is measured:

= t / D                     (2)

Read more →

Doppler effect in spacetime and timespace

We follow the presentation of Guy Moore, formerly of McGill University, online here.

The Doppler effect is the phenomenon we have all noticed, that a sound produced by a moving source, or which you hear while you are moving, has its perceived frequency shifted.

Spacetime (3+1)

If a source of sound makes a sudden bang (pressure pulse) at time 0, then the location in space of the pressure pulse in relation to time will look like successive concentric circles. For a source moving to the right, letting out a series of “bangs,” the location of the successive pressure peaks will be closer together on the right and further apart on the left.

Now remember that a sound is just a series of pressure peaks, which are tightly separated in time, which is the period of the wave. Therefore, instead of thinking of the sound waves as due to “bangs,” you can think of them as pressure peaks in a periodic sound wave. In front of the moving object the peaks are closer together. That means that the wave length is shorter, which means it is a higher frequency wave. Behind, the peaks are farther apart, meaning that it is a longer wavelength sound, at a lower frequency. This is the gist of the Doppler effect.

Let us now actually calculate the size of the effect. Suppose a sound source is moving right at you, at velocity v. At time 0, it emits a pressure peak. At time Δt, it emits a second pressure peak. If its distance from you at time 0 was x, its distance from you at time Δt was xvΔt (it is nearer, since it is moving towards you).

Read more →

Mean speed and pace

Speed of a motion is the time rate of length change, that is, the length interval with respect to a timeline interval without regard to direction. Pace of a motion is the space rate of time change, that is, the time interval with respect to a locusline interval without regard to direction.

The symbol for speed is v = Δst and for pace is u = Δts. Instantaneous speed is ds/dt. Punctaneous pace is dt/ds.

There are two kinds of mean speed or pace: the time mean and the space mean. The time mean is the arithmetic mean if the denominators are a common time interval. The space mean is the arithmetic mean if the denominators are a common space interval. The time mean is the harmonic mean if the denominators are a common space interval. If the denominators are a common time interval, the space mean is the harmonic mean.

The time mean speed (TMS) is the arithmetic mean of speeds with a common time interval. The time mean pace (TMP) is the harmonic mean of paces with a common time interval. For example, the travel distance for vehicles on a highway during a time period is measured. The time mean speed or pace may then be calculated.

The space mean pace (SMP) is the arithmetic mean of paces with a common space interval. The space mean speed (SMS) is the harmonic mean of speeds with a common space interval. For example, the travel time for vehicles over a length of highway is measured. The space mean speed or pace may then be calculated.

Read more →

Coordinate transformations

Coordinate Transformations with t

x = space coordinate, t = time coordinate, v = velocity, u = pace

 

Galileian transformation

speed: = xvt and t´ = t,         pace: = xt/u and t´ = t.

Co-Galileian transformation

speed: = tx/v and x´ = x,       pace: = tux and x´ = x.

 

Light:   c := speed of light,        := pace of light.

speed: x = ct or x/c = t and = ct´, or x´/c = ,

pace:  c´x = t or x = t/c´ and c´r′ = or = t´/c´.

 

Lorentz transformation

speed: γ = (1 – v2/c2)–1/2 with x´ = γ (x − vt) and = γ (txv/c²),

pace:  γ = (1 – 2/u2)–1/2 with γ (xt/u) and t´γ (txc´²/u),

which applies only if |v| < |c| or |u| > ||.

 

Co-Lorentz transformation

speed: λ = (1 − c2/v2)–1/2 with λ (t − x/v) and λ (xt (c2/v)),

pace:  λ = (1 – u2/2)–1/2 with λ (tux) and λ (xt (u/c´²)),

which applies only if |v| > |c| or |u| < ||.

Read more →

Past, present, and future

This continues the post on the Arrow of tense.

Past, present, and future are characteristics of time. But they are also characteristics of places, of things, or events, etc.

Yesterday was in the past, today is in the present, and tomorrow is in the future.

Past places are remembered, present places are experienced, and future places are imagined.

Some things were in the past, some things are in the present, and some things will be in the future.

Some events happened in the past, some events are happening in the present, and some events will be happening in the future.

So past, present, and future are not time itself. They are characteristics that apply to various things.

Past, present, and future are tenses, which refer to order, not time per se. One can order events, experiences, objects, places, and periods of time in various ways. One can study which order is the right physical order.

And time has order. But order is not time.

Time is duration.

New terms for 3D time

This post highlights several recent terms or definitions added to the glossary above.

The distance is the metric of space, the shortest length between two points in space. Similarly, the distime is the metric of time, the shortest duration between two points in time.

A timeline is a linear ordering of events by distime from or to a reference event. A locusline is a linear ordering of events by distance from or to a reference event.

A clock shows the present instant in the local timeline. An odologe (o′∙do∙loje) is an app or device that shows the present point in the current locusline.

Instantaneous events occur in an instant of time. Punctaneous events occur in a point of space.

Simultaneous events occur at the same time. Simulocus events occur at the same place.

Synchronous motions are parallel in time, as in having the same period. From Greek syn+chron+ous. Symmacronous motions are parallel in space, as in having the same orbit. From Greek sym+macron+ous.

Pseudo-length is measured by time and expressed as length, as with multiplying time by the free-flow speed. Pseudo-duration is measured by length and expressed as time, as with multiplying length by the free-flow pace.

Inertia (linear) is the resistance of an object to any change in its state of motion. Facilia (linear) is the nonresistance of a subject to a change in its state of movement.