Respuesta :
The correct answer for this question is this one:Hope this helps answer your question and have a nice day ahead.
v( t)= sin( ωt) cos^2 ( ωt)
s(t) = ∫sin(ωt) cos^2 (ωt) dt
let cos(ωt) = u
-ωsin(ωt) dt = du
∫sin(ωt) cos^2 (ωt) dt = -(1/ω)∫u^2 du = -(1/ω)u^3 / 3 + const
s(t) = -(1/ω)cos^3(ωt) / 3 + const
s(0) = 0 => const = 1/(3ω)
s(t) = (1 - cos^3(ωt))/(3ω)
v( t)= sin( ωt) cos^2 ( ωt)
s(t) = ∫sin(ωt) cos^2 (ωt) dt
let cos(ωt) = u
-ωsin(ωt) dt = du
∫sin(ωt) cos^2 (ωt) dt = -(1/ω)∫u^2 du = -(1/ω)u^3 / 3 + const
s(t) = -(1/ω)cos^3(ωt) / 3 + const
s(0) = 0 => const = 1/(3ω)
s(t) = (1 - cos^3(ωt))/(3ω)
By integrating the velocity equation, we will see that the position equation is:
[tex]f(t) = \frac{cos^3(\omega t) - 1}{3}[/tex]
How to get the position equation of the particle?
Here we know that the velocity of the particle is:
[tex]v(t) = sin(\omega t)*cos^2(\omega t)[/tex]
To get the position equation we just need to integrate the above equation:
[tex]f(t) = \int\limits {sin(\omega t)*cos^2(\omega t)} \, dt[/tex]
If we take:
u = cos(ωt)
Then:
du = -sin(ωt)dt ⇒ dt = -du/sin(ωt)
Replacing that in our integral we get:
[tex]\int\limits {sin(\omega t)*cos^2(\omega t)} \, dt\\\\-\int\limits {\frac{sin(\omega t)*u^2 \, du}{sin(\omega t)}\\\\\\-\int\limits {u^2} \, dt = -\frac{u^3}{3} + c[/tex]
Where C is a constant of integration.
Now we remember that u = cos(ωt)
Then we have:
[tex]f(t) = \frac{cos^3(\omega t)}{3} + C[/tex]
To find the value of C, we use the fact that f(0) = 0.
[tex]f(t) = \frac{cos^3(\omega *0)}{3} + C = \frac{1}{3} + C = 0\\\\C = -1/3[/tex]
Then the position function is:
[tex]f(t) = \frac{cos^3(\omega t) - 1}{3}[/tex]
If you want to learn more about motion equations, you can read:
https://brainly.com/question/19365526