Finding a solution for Relativistic Acceleration

In summary, Michio found an equation in Rindler coordinates that can be solved with a simple substitution.
  • #1
Michio Cuckoo
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I tried all my mathcad software such as Maple and I can't seem to find a solution to this time based differential equation.

m}\left%20(%201%20-%20\frac{\left%20[%20f(t)%20\right%20]^{2}}{c^{2}}%20\right%20)^{\frac{3}{2}}.gif
 
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  • #2
Michio Cuckoo said:
I tried all my mathcad software such as Maple and I can't seem to find a solution to this time based differential equation.

m}\left%20(%201%20-%20\frac{\left%20[%20f(t)%20\right%20]^{2}}{c^{2}}%20\right%20)^{\frac{3}{2}}.gif

Solving differential equations is often a matter of guessing and checking.
This equation comes up in Rindler coordinates, so I actually know the solution.

Let g = F/m.
Switch to a new independent variable T that is related to t through
t = c/g sinh(gT/c).

Then try the solution:

f = c tanh(gT/c)

In terms of the original t, we can rewrite f as

f = c (gt/c)/√(1 + (gt/c)2)

or

f = c (ct)/√((ct)2 + c2/g)
 
  • #3
Solving differential equations is often a matter of guessing and checking.
Michio, It's important part of everyone's physics education to pick up some standard techniques for solving DEs, so you don't have to depend entirely on the math software to do it for you, which often does an imperfect job. And this equation is a very easy one to solve. Setting the constant parameters to one to simplify the discussion,

df/dt = (1 - f2)3/2

Separate the variables (t on one side, f on the other) and integrate immediately:

t = ∫(1 - f2)-3/2 df

To do the integral, the factor 1 - f2 suggests making a trig substitution. Let f = sin θ.

t = ∫(cos θ)-3 cos θ dθ = ∫ sec2 θ dθ = tan θ

So we have f = sin θ, t = tan θ, giving us an algebraic relationship and the solution:

t = f/√(1 - f2) or f = t/√(1 + t2)
 
  • #4
Bill_K said:
t = ∫(1 - f2)-3/2 df

To do the integral, the factor 1 - f2 suggests making a trig substitution. Let f = sin θ.

Interestingly, it works to try the substitution f = sin(θ), then you get t = tan(θ), but it also works to try the substitution f = tanh(θ), then you get t = sinh(θ). I like the latter better, because that gets you to the Rindler coordinates.
 
  • #5
sin θ = tanh χ
cos θ = sech χ
tan θ = sinh χ

is known as the Gudermannian transformation and written θ = gd χ. See "Gudermannian Function" in Wikipedia.
 

FAQ: Finding a solution for Relativistic Acceleration

What is the concept of Relativistic Acceleration?

Relativistic Acceleration is a phenomenon in which an object's speed approaches the speed of light, causing its mass to increase and time to slow down according to the principles of Special Relativity.

Why is it important to find a solution for Relativistic Acceleration?

Understanding and finding a solution for Relativistic Acceleration is crucial in fields such as astrophysics and particle physics. It also has practical applications in technologies such as particle accelerators and GPS systems.

What are the challenges in finding a solution for Relativistic Acceleration?

One of the main challenges is the complex mathematical equations involved in describing and predicting Relativistic Acceleration. Additionally, the effects of Relativistic Acceleration become more significant as an object approaches the speed of light, making it difficult to observe and measure.

What are some current solutions for dealing with Relativistic Acceleration?

Some current solutions include using advanced mathematical models and simulations to predict the effects of Relativistic Acceleration. In practical applications, technologies such as particle accelerators use techniques such as magnetic fields to control and manipulate particles traveling at relativistic speeds.

What are some potential future solutions for Relativistic Acceleration?

There are ongoing research efforts to find ways to mitigate the effects of Relativistic Acceleration, such as developing materials that can withstand high speeds and energies without experiencing significant mass increase. Another approach is to continue exploring the principles of Special Relativity and finding new ways to manipulate space and time to overcome the limitations of Relativistic Acceleration.

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