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klio [65]
3 years ago
14

A 0.50-kg object moves on a horizontal frictionless circular track with a radius of 2.5 m. An external force of 3.0 N, always ta

ngent to the track, causes the object to speed up as it goes around. If it starts from rest, then at the end of one revolution the radial component of the force of the track on it is ____________.
Physics
1 answer:
Allisa [31]3 years ago
3 0

Answer:

Radial force component of force = 37.68 N

Explanation:

By Newton's 2 nd law of motion,

F = ma

F = 3.0 N, m = 0.5 Kg, a (Linear Acceleration ) = ?

3 = 0.5 a

a = 6 m/sec^{2}

Now, a = 6 m/sec^{2} , r = 2.5 m ,α(angular acceleration )  = ?

a = r α

6= 2.5 α

hence α = 2.4 rad/sec^{2}

w= ?, w_0= 0, \alpha =2.4\ rad/sec^{2},\theta =2\ \pi (One\ Revolution)

we know that,

w^{2} =w_0^2 +2 \alpha\cdot s\\          =0 + 2\cdot 2.4\cdot 2\pi\\=30.14 \\w=\sqrt{30.144} = 5.49\ Rad/ sec

Radial force component of force  = m r w^{2}

since m =0.5 kg, r =2.5 m w =5.49 rad/sec

Radial force component of force =0.5\cdot\ 2.5\cdot\ 5.49^{2} = 37.68 N

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We need to separate the x- and y-components of the applied force. For simplicity, I will denote the direction along the inclined plane as x-direction, and the perpendicular direction as y-direction.

F_x = F\cos(30^\circ)\\F_y = F\sin(30^\circ)

Only the x-component of the applied horizontal force does work on the trunk.

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The work done by the weight of the trunk can be calculated similarly. Only the x-component of the weight does work on the trunk.

W_g = -mg\sin(30^\circ)d

Note that the direction of the weight force is opposite of the direction of the motion, so this force does negative work on the trunk.

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The energy dissipated by the frictional force can be found as follows:

W_f = -mg\cos(30^\circ)\mu d = -35(9.8)(0.86)(0.19)(4.8) = -269J

Additionally, the sum of work done by the friction and weight is equal in magnitude to the work done by the applied force. This shows that our calculations are consistent.

In the second part of the question, the applied force is on the x-direction. We will follow a similar procedure but a different force.

0 = F - mg\sin(30^\circ) - mg\cos(30^\circ)\mu\\0 = F - 35(9.8)(0.5) - 35(9.8)(0.86)(0.19)\\0 = F - 171.5 - 56\\F = 227.5N

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W_f = -mg\cos(30^\circ)\mu d = -35(9.8)(0.86)(0.19)(4.8) = -269J

Explanation:

As you can see above, the answers are the same, although the directions of the applied forces are different. The reason for this situation is that in the first part the y-component does no work.

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