The tape is now wound back into the drum at angular rate omega(t). With what speed will the end of the tape move? (Note that our drawing specifies that a positive derivative of x(t)implies motion away from the drum. Be careful with your signs! The factthat the tape is being wound back into the drum implies that \omega(t) < 0, and for the end of the tape to move closer to the drum, it must be the case that v(t) < 0.
Answer in terms of omega(t) and other given quantities from the problem introduction.
v(t) =_____.


Respuesta :

Answer:

See description

Explanation:

Frist we need to know the longitude of tape which is unwinding. Such relationship can be obtained with arc length. An arc length is the distance bewteen two points in a curve.

The relationship is:

[tex]S = \theta r[/tex]

Where [tex]S[/tex] is the arc length or distance, theta is the angle that results from the initial point of the measure to the final point, and r is the radius of a circumference.

Now let [tex]x(t)[/tex] be length the unwinded tape. Change [tex]S[/tex] by [tex]x(t)[/tex] and you ge the relationship:

[tex]x(t) = \theta r[/tex]

if you unwind the tape by one revolution ([tex]\theta = 2 \pi[/tex]) you get the perimeter of a cricle [tex] x(t)= 2 \pi r[/tex], if you unwind it two times then [tex] x(t)= 4 \pi r[/tex] and so on.

Then we have that the derivative of [tex]x(t)[/tex] is [tex]v(t)[/tex]

so we replace:

[tex]\frac{dx}{dt} = v(t)\\ \frac{dx}{dt}=v(t)=\frac{d\theta}{dt}[/tex]

the derivative of theta with respect to t is ω(t) by definition:

[tex]\frac{d\theta}{dt}=\omega(t)\\ =>\frac{dx}{dt}=v(t)=\omega(t) r\\=>\frac{v(t)}{r}=\omega(t)[/tex]

The result is the relationship between angular velocity and the velocity and tangential velocity at the point r