No problem, glad I could help! :smile:

In summary, Austin0 explained that d is an operator (a sort of function), and that when you perform the operation twice with respect to the same variable, you put dy2 on the bottom. He also said that if you want to see it in terms of ∆s, you can define ∆+x and ∆-x. Finally, he said that dx/dy = lim ∆+x/∆y and d2x/dy2 = lim ∆(dx/dy))/∆y.
  • #1
Austin0
1,160
1
I have been trying to learn the proper acceleration math , and don't understand d[tex]^{2}[/tex]x , or d[tex]^{2}[/tex]t as it appears , where d seems to have the normal meaning of delta.

Is this simply equivalent to dx[tex]^{2}[/tex] or dt[tex]^{2}[/tex] ?

Thanks
 
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  • #2
Hi Austin0! :smile:

(try using the X2 tag just above the Reply box :wink:)
Austin0 said:
I … don't understand d[tex]^{2}[/tex]x , or d[tex]^{2}[/tex]t as it appears , where d seems to have the normal meaning of delta.

Is this simply equivalent to dx[tex]^{2}[/tex] or dt[tex]^{2}[/tex] ?

No.

d is an operator (a sort of function), and d2 means that you perform the operation twice.

If you perform it both times with respect to the same variable, say y, you put dy2 on the bottom, so it's d2/dy2 (x), or d2x/dy2.

If you perform it once with respect to y and once with respect to z, you put dxdy on the bottom, so it's d2/dydz (x), or d2x/dydz. :smile:

If you want to see it in ∆s …

define ∆+x to be the increase in x if you increase y by ∆y, and ∆-x to be the decrease in x if you decrease y by ∆y.

Then dx/dy = lim ∆+x/∆y = lim ∆-x/∆y

and d2x/dy2 = lim ∆(dx/dy))/∆y

= lim (∆+x - ∆-x)/(∆y)2

(and, by comparison, (dx/dy)2 = dx/dy = lim (∆x)/(∆y)2, which is not the same :wink:)

For example, if x = yn,

then ∆+x = nyn-1∆y + (1/2)n(n-1)yn-2(∆y)2 + …,

and ∆-x = nyn-1∆y - (1/2)n(n-1)yn-2(∆y)2 + …,

so dx/dy = lim ∆+x/∆y = lim ∆-x/∆y = nyn-1,

and d2x/dy2 = lim (∆+x - ∆-x)/(∆y)2 = n(n-1)yn-2 :smile:
 
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  • #3
tiny-tim said:
Hi Austin0! :smile:

(try using the X2 tag just above the Reply box :wink:)


No.

d is an operator (a sort of function), and d2 means that you perform the operation twice.

If you perform it both times with respect to the same variable, say y, you put dy2 on the bottom, so it's d2/dy2 (x), or d2x/dy2.

If you perform it once with respect to y and once with respect to z, you put dxdy on the bottom, so it's d2/dydz (x), or d2x/dydz. :smile:

If you want to see it in ∆s …

define ∆+x to be the increase in x if you increase y by ∆y, and ∆-x to be the decrease in x if you decrease y by ∆y.

Then dx/dy = lim ∆+x/∆y = lim ∆-x/∆y

and d2x/dy2 = lim ∆(dx/dy))/∆y

= lim (∆+x - ∆-x)/(∆y)2

(and, by comparison, (dx/dy)2 = dx/dy = lim (∆x)/(∆y)2, which is not the same :wink:)

For example, if x = yn,

then ∆+x = nyn-1∆y + (1/2)n(n-1)yn-2(∆y)2 + …,

and ∆-x = nyn-1∆y - (1/2)n(n-1)yn-2(∆y)2 + …,

so dx/dy = lim ∆+x/∆y = lim ∆-x/∆y = nyn-1,

and d2x/dy2 = lim (∆+x - ∆-x)/(∆y)2 = n(n-1)yn-2 :smile:

Hi tiny-tim You have been very helpful. I didn't have the correct understanding of d at all.
I thought it was simply the total change in whatever it was applied to ,irrespective of whatever function it was used in. I.e. Simply the total interval. The distance represented by dx as the difference between two specific coordinate x's.
I think your explication has made it clear but I guess time will tell.
Thanks for your responce and friendly greeting :smile:
 

FAQ: No problem, glad I could help! :smile:

What is proper acceleration and how is it different from coordinate acceleration?

Proper acceleration is a measure of how rapidly an object's velocity changes with respect to its own proper time. It is different from coordinate acceleration, which measures the change in velocity with respect to a fixed frame of reference.

How is proper acceleration related to the curvature of spacetime?

Proper acceleration is directly related to the curvature of spacetime through Einstein's theory of general relativity. The presence of mass and energy curves the fabric of spacetime, causing objects to experience proper acceleration.

Can proper acceleration be negative?

No, proper acceleration cannot be negative. Since it is a measure of how rapidly an object's velocity is changing, it must always be positive or zero. Negative acceleration is a concept used in classical mechanics, but does not apply to proper acceleration in the context of relativity.

What are some real-world examples of proper acceleration?

Examples of proper acceleration include the acceleration experienced by a rocket as it launches, the acceleration experienced by an astronaut in orbit around Earth, and the acceleration experienced by objects falling towards a massive body like a planet or star.

How is proper acceleration measured and calculated?

Proper acceleration is typically measured using instruments such as accelerometers, which can detect changes in an object's velocity. It can also be calculated using mathematical equations that take into account an object's velocity and proper time.

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