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A physics student of mass 43.0 kg is standing at the edge of the flat roof of a building, 12.0 m above the sidewalk. An unfriendly dog is running across the roof toward her. Next to her is a large wheel mounted on a horizontal axle at its center. The wheel, used to lift objects from the ground to the roof, has a light crank attached to it and a light rope wrapped around it; the free end of the rope hangs over the edge of the roof. The student grabs the end of the rope and steps off the roof. If the wheel hasradius 0.300 m and a moment of inertia of \(9.60\,\,kg.{m^2}\) for rotation about the axle, how long does it take her to reach the sidewalk, and how fast will she be moving just before she lands? Ignore friction.

Short Answer

Expert verified

The time to reach the sidewalk is \(2.92\,\,{\rm{s}}\)

She is moving at the speed of just before she lands

Step by step solution

01

Identification of the given data.

Given in the question,

The Mass of the student,\({m_s} = 43.0\,\,{\rm{kg}}\)

The Height above the building\(h = \,12\,\,{\rm{m}}\)

The radius of the wheel\({r_w} = 0.300\,\,{\rm{m}}\)

The moment of inertia of the wheel, \(I = 9.60\,\,{\rm{kg}}{\rm{.}}{{\rm{m}}^{\rm{2}}}\)

02

Concept used to solve the question

Law of conservation of energy

According to the conservation of energy, the energy of a systemcan neither be created nor destroyed it can only be converted from one form of energy to another.

\({E_F} = {E_I}\)

03

Finding the time to reach the sidewalk.

From the conservation of energy,

Total initial energy = Total final energy

Initial potential energy +initial kinetic energy= final potential energy + final kinetic energy.

\({U_i} + K{E_i} = {U_f} + K{E_f}\)

Since the student is at height h.

The initial potential energy,\({U_i} = {m_s}gh\)

The system (student + wheel) is initially at the rest

The initial kinetic energy \(K{E_i} = 0\)

The final height is zero

Therefore,

Final potential energy \({U_f} = 0\)

The final kinetic energy will be the sum of the translational kinetic energy of the student and the rotational kinetic energy of the wheel.

Final kinetic energy

\(\begin{array}{}K{E_f} = K{E_{ts}} + K{E_{rw}}\\ = \frac{1}{2}{m_s}{v^2} + \frac{1}{2}I{\omega _w}^2\end{array}\)

Where v is linear speed, I is the moment of inertia and \(\omega \) is angular velocity.

Substituting all the values into the equation

\({m_s}gh + 0 = 0 + \frac{1}{2}{m_s}{v^2} + \frac{1}{2}{I_w}{\omega _w}^2\)

We know,

\(v = r\omega \)

\({m_s}gh = \frac{1}{2}{m_s}{\left( {{r_w}{\omega _w}} \right)^2} + \frac{1}{2}{I_w}{\omega _w}^2\)

Substituting the values

\(\begin{array}{}\left( {43.0\,\,{\rm{kg}}} \right)\left( {9.0\,\,{{\rm{m}} \mathord{\left/ {\vphantom {{\rm{m}} {{{\rm{s}}^{\rm{2}}}}}} \right.} {{{\rm{s}}^{\rm{2}}}}}} \right)\left( {\,12\,\,{\rm{m}}} \right) = \frac{1}{2}\left( {43.0\,\,{\rm{kg}}} \right){\left( {0.300\,\,{\rm{m}}} \right)^2}{\omega _w}^2 + \left( {9.60\,\,{\rm{kg}}{\rm{.}}{{\rm{m}}^{\rm{2}}}} \right){\omega _w}^2\\{\omega _w}^2 = 750.70\,\,\\{\omega _w} = 27.4\,\,{{{\rm{rad}}} \mathord{\left/{\vphantom {{{\rm{rad}}} {\rm{s}}}} \right.} {\rm{s}}}\end{array}\)

Therefore, the final angular velocity of the wheel is \({\omega _w} = 27.4\,\,{{{\rm{rad}}} \mathord{\left/ {\vphantom {{{\rm{rad}}} {\rm{s}}}} \right.} {\rm{s}}}\)

Therefore, the final angular displacement

\(\begin{array}{}\theta = \frac{h}{r}\\ = \frac{{12.00\,\,{\rm{m}}\,}}{{0.300\,{\rm{m}}}}\\ = 40\,\,{\rm{rad}}\end{array}\)

To find the time first we need to find the angular acceleration since, the force acting on the system is constant so we can use the equation

\(\omega = \omega _0^2 + 2\alpha \left( {\theta - {\theta _0}} \right)\)

Where, \(\omega \) is final angular velocity =\({\omega _w} = 27.4\,\,{{{\rm{rad}}} \mathord{\left/ {\vphantom {{{\rm{rad}}} {\rm{s}}}} \right.} {\rm{s}}}\)

Since the system is initially at rest initial angular velocity \({\omega _0} = 0\)

Initial angular displacement \({\theta _0} = 0\)

Final angular displacement \(\theta = 40\,\,{\rm{rad}}\)

Substituting into the equation.

\(\begin{array}{}{\left( {27.4\,\,{{{\rm{rad}}} \mathord{\left/{\vphantom {{{\rm{rad}}} {\rm{s}}}} \right.} {\rm{s}}}} \right)^2} = 0 + 2\alpha \left( {40\,\,{\rm{rad}} - 0} \right)\\\alpha = 9.39\,\,{{{{\rm{rad}}} \mathord{\left/ {\vphantom {{{\rm{rad}}} {\rm{s}}}} \right.}{\rm{s}}}^2}\end{array}\)

Therefore, angular acceleration is

Now for finding the time using the equation

\(\omega = {\omega _0} + \alpha t\)

Substituting the values

\(\begin{array}{}27.4\,\,{{{\rm{rad}}} \mathord{\left/ {\vphantom {{{\rm{rad}}} {\rm{s}}}} \right. } {\rm{s}}} = 0 + \left( {9.39\,\,{{{{{\rm{rad}}} \mathord{\left/ {\vphantom {{{\rm{rad}}} {\rm{s}}}} \right.} {\rm{s}}}}^2}} \right)t\\t = 2.92\,\,{\rm{s}}\end{array}\)

Therefore, the time to reach the sidewalk is \(2.92\,\,{\rm{s}}\)

Since both the wheel and the student is connecting, they will be same transitional speed

So, the speed of a student can be calculated using the equation

\(\begin{array}{}v = r{\omega _w}\\ = \left( {0.300\,\,{\rm{m}}} \right)\left( {27.4\,\,{{{\rm{rad}}} \mathord{\left/ {\vphantom {{{\rm{rad}}} {\rm{s}}}} \right.} {\rm{s}}}} \right)\\ = 8.22\,\,{{{\rm{m}} \mathord{\left/ {\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}^2}\end{array}\)

Hence, she is moving at the speed of \( = 8.22\,\,{{{\rm{m}} \mathord{\left/ {\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}^2}\)

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