Worldlines - no need for ref frames?

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Worldlines in spacetime diagrams allow for the relation of events without necessarily relying on reference frames. However, the discussion raises concerns about the necessity of a stationary reference frame to establish proper time and create other worldlines. It is argued that while worldlines can illustrate geometric relationships independent of the choice of axes, they still fundamentally depend on a reference frame for accurate measurements. The discussion emphasizes that while certain quantities, like intervals, can be frame-independent, this principle mainly holds in inertial frames within flat Minkowskian spacetime. Ultimately, the utility of worldlines is questioned without a defined point of reference in space and time.
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"In Principle, worldlines allow us to relate events on one another - to do sciecne without using reference frames at all".

This was in Wheeler and Taylor's Intro to SR book.

My question is, isn't this false? Because worldlines exist in a spacetime diagram. Vertical being time and horizontal is space. One reference frame is always needed, which normally is the one that does not move wrt space. Hence it registers the greatest proper time. All other worldlines are created wrt to this stationary reference frame (i.e. the speed and directions of the particles that translate to worldlines are calculated or measured wrt to the stationary frame). So one reference frame must be needed hence contradicting the statement?
 
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I think what they are trying to say is that
the physics involved relies only on the worldlines and their [Minkowski-]geometric relations to events and other figures... and not on the choice of axes (choice of reference frame) used to draw the picture. By direct analogy, the properties of Euclidean geometry rely on the figures themselves and not on the choice of axes used to draw the picture.
 
So they are trying to say that no matter which frame you are in, you will calculate the same major results such as the proper time for different moving objects moving wrt you. All reference frames are arbitary and there are quantities that are independent of all ref frames.

Correct?
 
pivoxa15 said:
So they are trying to say that no matter which frame you are in, you will calculate the same major results such as the proper time for different moving objects moving wrt you. All reference frames are arbitary and there are quantities that are independent of all ref frames.

Correct?
Interval ds is independent of ref. frame:

ds^2 = (ct)^2 - (dx^2 + dy^2 +dz^2).

If only one spatial dimension x is involved: ds^2 = (ct)^2 - dx^2.

But I think this is only valid with inertial ref. frames (or when you can ignore acceleration effects), that is in a Minkowskian space-time, that is, in a "flat" space-time. A lot of people here can correct me.
 
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pivoxa15 said:
"In Principle, worldlines allow us to relate events on one another - to do science without using reference frames at all".

This was in Wheeler and Taylor's Intro to SR book.

My question is, isn't this false?

Well, I'm not sure what the meaning was supposed to be wrt everything after the dash there? Doesn't sound right "as worded" here.

pivoxa15 said:
Because worldlines exist in a spacetime diagram. Vertical being time and horizontal is space. One reference frame is always needed, which normally is the one that does not move wrt space. Hence it registers the greatest proper time. All other worldlines are created wrt to this stationary reference frame (i.e. the speed and directions of the particles that translate to worldlines are calculated or measured wrt to the stationary frame). So one reference frame must be needed hence contradicting the statement?

Without a worldline, a Minkowski worldline diagram is pretty much useless. It's like defining the location of something with no point of reference anywhere anytime. Space & time w/o any observer.
 
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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