A uniform disk with mass 40.0 kg and radius 0.200 m is pivoted at its center about a horizontal, frictionless axle that is stationary. The disk is initially at rest, and then a constant force F = 30.0 N is applied tangent to the rim of the disk.
(a) What is the magnitude v of the tangential velocity of a point on the rim of the disk after the disk has turned through 0.200 revolution?
(b) What is the magnitude a of the resultant acceleration of a point on the rim of the disk after the disk has turned through 0.200 revolution?

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Answer:

Given that

r= 0.2 m

m= 40 kg

F= 30 N

We know that mass moment of inertia of disk given as

I = m r²/2

I= 40 x 0.2²/2

I= 0.8 kg.m²

The torque produce by force

T = F.r

T= 30 x 0.2 = 6 N.m

We also know that

T= I α

α = angular acceleration of disk

by putting the values

6 = 0.8 x α

α = 7.5 rad/s²

Given that initial speed is zero.

Lets speed is ω after 0.2 rev

ω ² = ωo+ 2 α θ

We know that

1 rev  = 2π

0.2 rev= 0.4π

θ = 0.4π

ω ² = 0+ 2 x 7.5 x 0.4 x π

ω = 4.34 rad/s

So the tangential velocity v

v= ω  r

v= 4.34 x 0.2 = 0.86 m/s

v= 0.86 m/s

Tangential acceleration (at)= α .r= 7.5 x 0.2 =1.5 m/s²

Radial acceleration(ar) = ω² r = 4.34² x 0.2 = 3.76 m/s²

resultant acceleration ,a

[tex]a=\sqrt{at^2+ar^2}[/tex]

[tex]a=\sqrt{1.5^2+3.76^2}[/tex]

a = 4.05 m/s²

The magnitude of the resultant acceleration of a point on the rim of the disk after the disk has turned through 0.200 revolutions is 4.05 m/s².

What is acceleration?

Acceleration is the rate of change of velocity with respect to time.

As it is given that the radius(r) of the disk is 0.2 m, while the mass of the disk is 40 kg, and the constant force applied is 30 N.

Now since we know that mass moment of inertia of disk is given as

[tex]I = \dfrac{m r^2}{2}\\\\\text{Substituting the values}\\\\I = \dfrac{40 \times 0.2^2}{2}\\\\I = 0.8\ kg\cdot m^2[/tex]

Thus, the mass moment of inertia of the disk is 0.8 kg·m².

The torque produced by force on the disk can be written as,

[tex]T = F\cdot r = I \times \alpha \\\\30 \times 0.2 = 0.8 \times \alpha \\\\ \alpha = 7.5\rm\ rad/sec^2[/tex]

Thus, the acceleration of the disk can be written as 7.5 rad/s².

The circular distance covered by the disk can be written as,

[tex]\rm 1\ rev = 2\pi \\\\0.2\ rev= 0.4\pi \\\\\theta = 0.4\pi[/tex]

As it is given that the initial speed is zero. therefore, according to the second equation of motion for the circular motion can be as

[tex]\omega^2 = \omega_o+ (2\alpha\ \theta) \\\\\omega^2 = 0+ (2 \times 7.5 \times 0.4 \times \pi)\\\\\omega = 4.34\ rad/s[/tex]

Now the tangential velocity v can be written as,

[tex]v=\omega \times r\\\\v= 4.34 \times 0.2 \\\\v= 0.86 m/s[/tex]

Further, the components of the acceleration can be written as,

Tangential acceleration

[tex]a_t= \alpha \times r\\\\a_t= 7.5 x 0.2 \\\\a_t=1.5\rm\ m/s^2[/tex]

Radial acceleration

[tex]a_r = \omega^2 r \\\\a_r= 4.34^2 \times 0.2 \\\\a_r= 3.76\rm\ m/s^2[/tex]

Resultant acceleration

[tex]a = \sqrt{a_t^2+a_r^2}\\\\a = \sqrt{1.5^2+3.76^2}\\\\a = 4.05\rm\ m/s^2[/tex]

Hence, the magnitude of the resultant acceleration of a point on the rim of the disk after the disk has turned through 0.200 revolutions is 4.05 m/s².

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