The forearm in Fig. 8–46 accelerates a 3.6-kg ball at \({\bf{7}}{\bf{.0}}\;{\bf{m/}}{{\bf{s}}^{\bf{2}}}\) by means of the triceps muscle, as shown. Calculate (a) the torque needed and (b) the force that must be exerted by the triceps muscle. Ignore the mass of the arm.

FIGURE 8-46

Problems 35 and 36

Short Answer

Expert verified

(a) The required value of the torque is \(7.8\;{\rm{N}} \cdot {\rm{m}}\).

(b) The force exerted by the triceps muscle is \(310\;{\rm{N}}\).

Step by step solution

01

Concept

Torque is the product of the moment of inertia and the angular acceleration. For this problem, you have to find the relationship between linear acceleration and angular acceleration.

02

Given data

The mass of the ball is \(m = 3.6\;{\rm{kg}}\).

The length of the forearm is \(r = 31\;{\rm{cm}} = 0.31\;{\rm{m}}\).

The translational acceleration of the ball is \(a = 7.0\;{\rm{m/}}{{\rm{s}}^{\rm{2}}}\).

The perpendicular distance of the triceps from the axis of rotation is \({r_1} = 2.5\;{\rm{cm}} = 0.025\;{\rm{m}}\).

Let \(\tau \) torque be needed to produce such acceleration, and the force exerted by the triceps muscle is \(F\).

You can consider the joint as a point mass.

03

Calculation of part (a)

Part (a)

The moment of inertia of the ball relative to the axis of rotation is \(I = m{r^2}\).

Now, the angular acceleration of the ball is \(\alpha = \frac{a}{r}\).

Therefore, the torque on the ball is

\(\begin{align}\tau &= I\alpha \\ &= m{r^2} \times \frac{a}{r}\\ &= mra\end{align}\).

Now, substituting the values in the above equation, you get

\(\begin{align}\tau &= mra\\ &= \left( {3.6\;{\rm{kg}}} \right) \times \left( {0.31\;{\rm{m}}} \right) \times \left( {7.0\;{\rm{m/}}{{\rm{s}}^{\rm{2}}}} \right)\\ &= 7.8\;{\rm{N}} \cdot {\rm{m}}\end{align}\).

Hence, the required value of the torque is \(7.8\;{\rm{N}} \cdot {\rm{m}}\).

04

Calculation of part (b)

Part (b)

Now, to produce that amount of torque,

\(\begin{align}\tau &= F{r_1}\\7.8\;{\rm{N}} \cdot {\rm{m}} &= F \times 0.025\;{\rm{m}}\\F &= 312\;{\rm{N}}\\ \approx 310\;{\rm{N}}\end{align}\).

Hence, the force exerted by the triceps muscle is \(310\;{\rm{N}}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A spherical asteroid with radius\(r = 123\;{\rm{m}}\)and mass\(M = 2.25 \times {10^{10}}\;{\rm{kg}}\)rotates about an axis at four revolutions per day. A “tug” spaceship attaches itself to the asteroid’s south pole (as defined by the axis of rotation) and fires its engine, applying a force F tangentially to the asteroid’s surface as shown in Fig. 8–65. If\(F = 285\;{\rm{N}}\)how long will it take the tug to rotate the asteroid’s axis of rotation through an angle of 5.0° by this method?

A grinding wheel is a uniform cylinder with a radius of 8.50 cm and a mass of 0.380 kg. Calculate (a) its moment of inertia about its center and (b) the applied torque needed to accelerate it from rest to 1750 rpm in 5.00 s. Take into account a frictional torque that has been measured to slow down the wheel from 1500 rpm to rest in 55.0 s.

A large spool of rope rolls on the ground with the end of the rope lying on the top edge of the spool. A person grabs the end of the rope and walks a distance l, holding onto it, Fig. 8–64. The spool rolls behind the person without slipping. What length of rope unwinds from the spool? How far does the spool’s center of mass move?

Question:(II) A person stands, hands at his side, on a platform that is rotating at a rate of 0.90 rev/s. If he raises his arms to a horizontal position, Fig. 8–55, the speed of rotation decreases to 0.60 rev/s. (a) Why? (b) By what factor has his moment of inertia changed?

A small 350-gram ball on the end of a thin, light rod is rotated in a horizontal circle of a radius of 1.2 m. Calculate (a) the moment of inertia of the ball about the center of the circle and (b) the torque needed to keep the ball rotating at a constant angular velocity if the air resistance exerts a force of 0.020 N on the ball. Ignore the air resistance on the rod and its moment of inertia.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free