Consider a motor that exerts a constant torque of 25.0 Nâ‹…m to a horizontal platform whose moment of inertia is 50.0 kgâ‹…m2 . Assume that the platform is initially at rest and the torque is applied for 12.0 rotations . Neglect friction.
Part A
How much work W does the motor do on the platform during this process?
Part B
What is the rotational kinetic energy of the platform Krot,f at the end of the process described above?

Respuesta :

To solve this exercise it is necessary to apply the concepts related to Work and Kinetic Energy. Work from the rotational movement is described as

[tex]W=\tau \Delta\theta[/tex]

In the case of rotational kinetic energy we know that

[tex]KE = \frac{1}{2}I\omega^2[/tex]

PART A) [tex]\theta[/tex] is given in revolutions and needs to be in radians therefore

[tex]\theta = 12rev(\frac{2\pi rad}{1rev})[/tex]

[tex]\theta = 24\pi rad[/tex]

Replacing in the work equation we have to

[tex]W=\tau \Delta\theta[/tex]

[tex]W= (25)(24\pi)[/tex]

[tex]W = 1884.95J[/tex]

PART B) From the torque and moment of inertia it is possible to calculate the angular acceleration and the final speed, with which the kinetic energy can be determined.

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

Rearrange for the angular acceleration,

[tex]\alpha = \frac{\tau}{I}[/tex]

[tex]\alpha = \frac{25}{50}[/tex]

[tex]\alpha = 0.5rad/s[/tex]

From the kinematic equations of angular motion we have,

[tex]\omega_f^2=\omega_i^2+2\alpha\theta[/tex]

[tex]\omega_f^2=0+2*0.5*24\pi[/tex]

[tex]\omega_f=\sqrt{0+2*0.5*24\pi}[/tex]

[tex]\omega_f = 8.68rad/s[/tex]

In this way the rotational kinetic energy would be given by

[tex]KE = \frac{1}{2}I\omega_f^2[/tex]

[tex]KE = \frac{1}{2}(50)(8.68)^2[/tex]

[tex]KE = 1883.56J[/tex]

A. The motors does work about 1880 J on the platform

B. The final rotational kinetic energy of the platform is about 1880 J

[tex]\texttt{ }[/tex]

Further explanation

Let's recall Moment of Force as follows:

[tex]\boxed{\tau = F d}[/tex]

where:

Ï„ = moment of force ( Nm )

F = magnitude of force ( N )

d = perpendicular distance between force and pivot ( m )

Let us now tackle the problem !

Given:

constant torque = Ï„ = 25.0 Nm

moment of inertia = I = 50.0 kg.m²

number of rotations = θ = 12.0 rotations = 24π rad

Asked:

A. work = W = ?

B. final rotational kinetic energy = Ek = ?

Solution:

Part A:

[tex]W = \tau \theta[/tex]

[tex]W = 25.0 \times 24\pi[/tex]

[tex]W = 600 \pi \texttt{ J}[/tex]

[tex]W \approx 1880 \texttt{ J}[/tex]

[tex]\texttt{ }[/tex]

Part B:

[tex]W = \Delta Ek[/tex]

[tex]W = Ek - Ek_o[/tex]

[tex]600 \pi = Ek - 0[/tex]

[tex]Ek = 600 \pi[/tex]

[tex]Ek \approx 1880 \texttt{ J}[/tex]

[tex]\texttt{ }[/tex]

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[tex]\texttt{ }[/tex]

Answer details

Grade: High School

Subject: Physics

Chapter: Moment of Force

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