Solving for Acceleration on a Parabolic Path | Physics Tutorial

[Drill]

Hi everybody



we know that if we have an object sliding on a frictionless ramp,

the acceleration force will be constant, and it equals to

a=g * sin(theta)
where theta is the ramp angle w.r.t. the ground


so the path of motion in this problem can be written mathematically as a linear function
y(x)=bx
and hence the tangent tan(theta)= bx /x =b


The Question is
if the path of motion is parabolic and is of the form

y(x) = a x^2

how to solve for the acceleration with respect to time ??

be aware that ,in this case the acceleration is not constant , and it always equals to the tangent of the parabola at the current location of the object.
and the tangent in this case is the first derivative of y which is
y'=2ax

as we see the tangent and hence the acceleration is a function of x

so ,

how to calculate the time as the function of position ??

thanks

 

[rock.freak667]

Using n-t coordinates you'd get that the acceleration vector is

[tex]\vec{a}=\dot{v} \hat{e_t}+ \frac{v^2}{\rho} \hat{e_n}[/tex]

where

[tex]\rho =\frac{(1+(y')^2)^\frac{3}{2}}{y''}[/tex]


Not sure if I wrote down the formula for ρ correctly though.

then again, for a time parameter x=t.

 

[Drill]

Hi

and thanks for replying

but can you explaine how this equation came about

[tex]\vec{a}=\dot{v} \hat{e_t}+ \frac{v^2}{\rho} \hat{e_n}[/tex]

or at least show me the source link

 

[rock.freak667]

Hi

and thanks for replying

but can you explaine how this equation came about

[tex]\vec{a}=\dot{v} \hat{e_t}+ \frac{v^2}{\rho} \hat{e_n}[/tex]

or at least show me the source link

read http://web.mst.edu/~reflori/be150/FloriNotes/ntCoordLectureNotes1.htm"

 

[Drill]

thanks :)

read http://web.mst.edu/~reflori/be150/FloriNotes/ntCoordLectureNotes1.htm"