Force law for elliptical motion with constant parameters

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A body of mass m moves under the influence of a force F in two dimensions. It has an trajectory
r(t) = aCos(wt)x^ + bSin(wt)y^

a = alpha
b = beta
w = omega, they are not a, b, and w in alphabet
x^,y^: vector unit

a,b,w are constant. Find the force law F = F(r) which corresponds to this motion (This trajectory is an ellipse, but not Keplerian ellipse. Newton's Law of Gravitaion is not the force law you seek here).
 
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Hint: Newton's second law of motion.
 
Can you explain more in detail, it still confuses me. How do we derive the fomular of Newton's Second Law F=ma to this kind of fomular:confused:
 
Well we have;

[tex]\vec{F} = m\vec{a}[/tex]
[tex]\vec{F} = m\frac{d\vec{v}}{dt}[/tex]
[tex]\vec{F} = m\frac{d^2\vec{r}}{dt^2}[/tex]

Can you go from here?
 
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I have to admit that I'm stupid, I know the Newton's Second Law. But how to get to r(t) = aCos(wt)x^ + bSin(wt)y^
 
What does [tex]m\frac{d^2\vec{r}}{dt^2}[/tex] mean to you?
 
My god man! I've forgot my d's! Duly corrected ...