The rate of rotation of a solid disk with a radius of #1 m# and mass of #5 kg# constantly changes from #16 Hz# to #27 Hz#. If the change in rotational frequency occurs over #12 s#, what torque was applied to the disk?

Answer 1

The torque was #=14.4Nm#

The torque is the rate of change of angular momentum

#tau=(dL)/dt=(d(Iomega))/dt=I(domega)/dt#
mass, #m=5kg#
radius, #r=1m#

The moment of inertia of a solid disc is

#I=1/2*mr^2#
#=1/2*5*1^2= 2.5 kgm^2#

The rate of change of angular velocity is

#(domega)/dt=((27-16))/12*2pi#
#=(11/6pi) rads^(-2)#
So the torque is #tau=2.5*(11/6pi) Nm=14.4Nm#
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Answer 2

To calculate the torque applied to the disk, we can use the formula:

Torque=I×α\text{Torque} = I \times \alpha

where I I is the moment of inertia of the disk and α \alpha is the angular acceleration.

The moment of inertia I I of a solid disk is given by the formula:

I=12mr2I = \frac{1}{2} m r^2

where m m is the mass of the disk and r r is the radius.

First, we calculate the initial and final angular velocities using the formula:

ω1=2πf1\omega_1 = 2\pi f_1 ω2=2πf2\omega_2 = 2\pi f_2

where f1=16Hz f_1 = 16 \, \text{Hz} and f2=27Hz f_2 = 27 \, \text{Hz} .

Then, we calculate the initial and final angular accelerations using the formula:

α=ω2ω1t\alpha = \frac{\omega_2 - \omega_1}{t}

where t=12s t = 12 \, \text{s} .

Now, we can plug in the values into the formulas to find the torque:

ω1=2π×16Hz=32πrad/s\omega_1 = 2\pi \times 16 \, \text{Hz} = 32\pi \, \text{rad/s} ω2=2π×27Hz=54πrad/s\omega_2 = 2\pi \times 27 \, \text{Hz} = 54\pi \, \text{rad/s}

α=54πrad/s32πrad/s12s=22πrad/s12s=116πrad/s2\alpha = \frac{54\pi \, \text{rad/s} - 32\pi \, \text{rad/s}}{12 \, \text{s}} = \frac{22\pi \, \text{rad/s}}{12 \, \text{s}} = \frac{11}{6} \pi \, \text{rad/s}^2

I=12×5kg×(1m)2=52kgm2I = \frac{1}{2} \times 5 \, \text{kg} \times (1 \, \text{m})^2 = \frac{5}{2} \, \text{kg} \cdot \text{m}^2

Torque=(52kgm2)×(116πrad/s2)=5512πNm\text{Torque} = \left(\frac{5}{2} \, \text{kg} \cdot \text{m}^2\right) \times \left(\frac{11}{6} \pi \, \text{rad/s}^2\right) = \frac{55}{12} \pi \, \text{N} \cdot \text{m}

Therefore, the torque applied to the disk is 5512πNm \frac{55}{12} \pi \, \text{N} \cdot \text{m} .

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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