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A block of mass 5kg slides down a surface inclined at 30 degrees to the horizontal. The coefficent of

kinetic friction is 0.3. A string attached to the block is wrapped around a flywheel on a fixed axis at O.

The flywheel has a mass 30kg and a moment of inertia 0.25kg·m2 with respect to the axis of rotation. The

string pulls without slipping at a perpendicular distance of 0.4m from the axis. (a) What is the acceleration

of the block down the plant? (b) What is the tension in the string?

A block of mass 5kg slides down a surface inclined at 30 degrees to the horizontal The coefficent ofkinetic friction is 03 A string attached to the block is wra class=

Respuesta :

Answer:

(a). The acceleration of the block is 1.793m/s.

(b). The string has a tension of 2.8N.

Explanation:

The forces acting on the block are the tension [tex]T[/tex] in the string, the frictional force [tex]F_k[/tex], and the gravitational force [tex]mg\: sin(\theta)[/tex], together they induce acceleration [tex]a[/tex] in the block; therefore,

[tex](1). \: \: ma= mg\:sin(\theta)- T-F_k[/tex].

Now, the frictional force [tex]F_k[/tex] is

[tex](2). \: \: F_k = \mu N =\mu \: mg\: cos(\theta)[/tex]

and the tension [tex]T[/tex] in the string is what causes the angular acceleration [tex]\alpha[/tex] in the flywheel; therefore,

[tex]I\alpha = TR[/tex]

[tex](3). \: \: \alpha = \dfrac{TR}{I},[/tex]

where [tex]R[/tex] is the distance from the axis of the flywheel and [tex]I[/tex] is its moment of inertia.

(a).

Since the linear acceleration of the flywheel is [tex]a = \alpha R[/tex], equation (3) gives

[tex]a = \dfrac{TR^2}{I}[/tex]

which when solved for [tex]T[/tex] gives

[tex](4).\: \: T = \dfrac{aI}{R^2}[/tex]

putting this and equation (2) into equation (1) gives

[tex]ma= mg\:sin(\theta)- \dfrac{aI}{R^2} -\mu mg\: cos(\theta)[/tex]

solving for [tex]a[/tex] we get:

[tex]ma+ \dfrac{aI}{R^2}= mg[\:sin(\theta)-\mu cos(\theta)][/tex]

[tex]a(m+ \dfrac{I}{R^2})= mg[\:sin(\theta)-\mu cos(\theta)][/tex]

[tex]\boxed{a = \dfrac{mg[\:sin(\theta)-\mu cos(\theta)]}{(m+ \dfrac{I}{R^2})}.}[/tex]

Putting in [tex]m=5kg[/tex], [tex]g= 9.8m/s^2[/tex], [tex]\theta = 30^o[/tex],[tex]\mu = 0.3[/tex], [tex]I = 0.25kg\:m^2[/tex], and [tex]R = 0.4m[/tex] we get:

[tex]a = \dfrac{(5kg)(9.8m/s^2)[\:sin(30^o)-(0.3) cos(30)]}{(5kg+ \dfrac{0.25kg\:m^2}{(0.4m)^2})}[/tex]

[tex]\boxed{a= 1.793m/s.}[/tex]

Thus, the acceleration of the block is 1.793m/s.

(b).

The tension [tex]T[/tex] in the string is given by the equation (4)

[tex]T = \dfrac{aI}{R^2}[/tex]

putting in  [tex]I = 0.25kg\:m^2[/tex], [tex]R = 0.4m[/tex], and [tex]a =1.793m/s[/tex] we get:

[tex]T = \dfrac{(1.793m/s^2)(0.25 kg\; m^2)}{(0.4m)^2}[/tex]

[tex]\boxed{T = 2.8N.}[/tex]

Thus, the string has a tension of 2.8N.