Parabolic path at constant speed

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Discussion Overview

The discussion revolves around the mathematical analysis of an object moving along a parabolic path defined by the equation y = 1/2 x² at a constant speed. Participants explore the implications of this motion on velocity and acceleration, addressing challenges in deriving acceleration from the velocity components.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Exploratory

Main Points Raised

  • One participant describes the velocity components as functions of x, confirming that the speed remains constant at c.
  • Concerns are raised about calculating acceleration, particularly that the numerical method used yielded results that were not perpendicular to the velocity vector.
  • Another participant suggests using the chain rule to derive acceleration components, proposing that a_x = v_x (dv_x/dx) and a_y = v_x (dv_y/dx).
  • A later reply indicates that a revised numerical method for estimating acceleration improved accuracy, aligning with the expected relationship between acceleration and velocity.
  • One participant introduces the concept of radius of curvature for the parabolic path, providing a formula and applying it to confirm the magnitude of acceleration.

Areas of Agreement / Disagreement

Participants generally agree on the approach to derive acceleration using the chain rule and the importance of ensuring that acceleration is perpendicular to velocity. However, there are variations in the methods used to calculate these values, and some uncertainty remains regarding the initial numerical methods employed.

Contextual Notes

Some participants note limitations in their numerical methods and the need for careful consideration of derivatives when functions are expressed in terms of x rather than t. The discussion reflects ongoing refinement of mathematical approaches rather than a settled conclusion.

rcgldr
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parabolic path at constant speed? (having issues)

I found a brief mention of this problem at a few web sites. An object follows a parabolic path at constant speed. I'm having some issues with the math involved:

Assume the path is defined by y = 1/2 x2, and that the constant speed is c.

velocity vector can be defined in terms of x:

vx = dx/dt = c / sqrt(x2 + 1)
vy = dy/dt = c x / sqrt(x2 + 1)

speed = sqrt(vx2 + vy2)
... = sqrt( c2/(x2 + 1) + (c x)2/(x2 + 1) )
... = sqrt( c2 (1+x2)/(x2 + 1) )
... = sqrt( c2 )
... = c

so that checks.

Since y = 1/2 x2, dy = x dx, dy/dt = x dx/dt = c x / sqrt(x2 + 1) which matches vy as defined above.

time can be defined as a function of x:

dx/dt = c / sqrt(x2 + 1)

sqrt(x2 + 1) dx = c dt

(1/2)(x sqrt(x2+1) + ln(x + sqrt(x2+1)) = c t + C

assuming t=0 when x=0, the integration constant will be zero

(1/2)(x sqrt(x2+1) + ln(x + sqrt(x2+1)) = c t
t = ( x sqrt(x2+1) + ln(x + sqrt(x2+1)) ) / (2 c)

I then plugged this info into a spreadsheet, using a range of x values as input. I confirmed that speed was c and that the slope vy/vx = x as expected (since dy = x dx).

The issue I ran into was trying to determine acceleration. Using a crude numerical method (ax = Δvx / Δt, ay = Δvy / Δt) resulted in calculating acceleration that wasn't perpendicular to velocity, but that conflicts with the fact that the speed is constant. I'm not sure how to take the second derivative for dx/dt and dy/dt when they are funcions of x and not t. I can substitute x = sqrt(2 y) for dy/dt:

dx/dt = c / sqrt(x2 + 1)

dy/dt = c x / sqrt(x2 + 1) = c sqrt(2 y) / (sqrt(2 y + 1), for positive x
dy/dt = -c sqrt(2 y) / (sqrt(2 y + 1), for negative x

but I'm not sure how to take derivates to get accelerations for ax and ay.
 
Last edited:
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rcgldr said:
The issue I ran into was trying to determine acceleration. Using a crude numerical method (ax = Δvx / Δt, ay = Δvy / Δt) resulted in calculating acceleration that wasn't perpendicular to velocity, but that conflicts with the fact that the speed is constant. I'm not sure how to take the second derivative for dx/dt and dy/dt when they are funcions of x and not t. I can substitute x = sqrt(2 y) for dy/dt:

dx/dt = c / sqrt(x2 + 1)

dy/dt = c x / sqrt(x2 + 1) = c sqrt(2 y) / (sqrt(2 y + 1), for positive x
dy/dt = -c sqrt(2 y) / (sqrt(2 y + 1), for negative x

but I'm not sure how to take derivates to get accelerations for ax and ay.
Interesting problem. My initial thoughts are to use the chain rule to get dvx/dt:

\begin{align}<br /> a_x = \frac{dv_x}{dt} \\<br /> = \frac{dv_x}{dx} \frac{dx}{dt} \\<br /> = v_x \frac{dv_x}{dx}<br /> \end{align}

Similarly, a_y = v_x \frac{dv_y}{dx}

Hopefully that helps.
 


Redbelly98 said:
Interesting problem. My initial thoughts are to use the chain rule to get dvx/dt:
The orignial problem was due to my crude numerical derivative method. If acceleration is perpendicular to velocity, then inverting the slope for acceleration should match the slope for velocity: -ax/ay == vy/vx. My original estimated acceleration was based on

ai = (vi - vi-1) / (ti - ti-1).

but -ax/ay was low by a near constant value, ~(t1 - t0). I changed this to

ai = (vi+1 - vi-1) / (ti+1 - ti-1)

which solved the original problem.

Using the chain rule as suggested provided the actual solution:

ax = -c2 x / (x2+1)2
ay = c2 / (2y+1)2
ay = c2 / (x2+1)2

As expected, acceleration is perpendicular to velocity, -ax/ay = vy/vx = x.
 
Last edited:


Glad it worked out.
rcgldr said:
My original estimated acceleration was based on

ai = (vi - vi-1) / (ti - ti-1).

but -ax/ay was low by a near constant value, ~(t1 - t0). I changed this to

ai = (vi+1 - vi-1) / (ti+1 - ti-1)

which solved the original problem.
Yes. If you must evaluate a derivative numerically, your second method is just as simple and a much, much more accurate way than the first one.
 
I had actually tried chain method before, just messed up on the math and didn't follow up on checking for my mistake when comparing the chain method to my estimated accelerations on the spread sheet. Seeing you thought that chain method should also work, I did it again, this time paying more attention and getting the correct answer as posted above.

On a side note, I forgot to include radius of curvature for a general function {x, y(x)}:

radius(x) = (1 + (y'(x))2)3/2 / | y''(x) |

in this case, y = 1/2 x2, y' = x, y'' = 1, so

radius(x) = (1 + x2)3/2 / |1|

I could have used this to confirm the magnitude of acceleration, a = v2 / r, in this case:

a = c2 / (x2+1)3/2

checking

ax = -c2 x / (x2+1)2
ay = c2 / (x2+1)2

a = ( ax2 + ay2 )1/2
a = ( (-c2 x / (x2+1)2)2 + (c2 / (x2+1)2) )1/2
a = ( c4 (x2+1) / (x2+1)4) )1/2
a = ( c4 / (x2+1)3) )1/2
a = c2 / (x2+1)3/2
 

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