Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A crustacean (Hemisquilla ensigera) rotates its anterior limb to strike a mollusk, intending to break it open. The limb reaches an angular velocity of 175 rad/s in \(1.50 \mathrm{ms} .\) We can approximate the limb as a thin rod rotating about an axis perpendicular to one end (the joint where the limb attaches to the crustacean). (a) If the mass of the limb is \(28.0 \mathrm{g}\) and the length is \(3.80 \mathrm{cm}\) what is the rotational inertia of the limb about that axis? (b) If the ex-tensor muscle is 3.00 mm from the joint and acts perpendicular to the limb, what is the muscular force required to achieve the blow?

Short Answer

Expert verified
(b) What is the muscular force required to achieve the blow? (a) Based on the solution above, calculate the rotational inertia using the formula \(I = \frac{1}{3}mL^2\) with the given mass and length values. Plug in the values and find the rotational inertia. (b) By following the solution provided, first calculate the angular acceleration, torque, and finally muscular force using the specified formulas. Use the calculated values to determine the muscular force required to achieve the blow.

Step by step solution

01

(a) Calculate the rotational inertia of the limb

To find the rotational inertia of the limb, we need to use the formula used for a thin rod rotating about an axis perpendicular to one end. The formula for the rotational inertia for a thin rod is: \(I = \frac{1}{3}mL^2\) where \(I\) = rotational inertia \(m\) = mass of the limb = \(28.0 \mathrm{g} = 28.0 \times 10^{-3} \mathrm{kg}\) \(L\) = length of the limb = \(3.80 \mathrm{cm} = 3.80 \times 10^{-2} \mathrm{m}\) Plug in the values and find the rotational inertia.
02

(b) Calculate the angular acceleration

To find the angular acceleration, we will use the formula below: \(\alpha = \frac{\omega^2}{2\theta}\) where \(\alpha\) = angular acceleration \(\omega\) = angular velocity = \(175 \,\text{rad/s}\) \(\theta\) = angular displacement Since the limb reaches an angular velocity of \(175 \,\text{rad/s}\) in \(1.50 \,\text{ms}\), the angular displacement is: \(\theta = \omega t = 175 \,\text{rad/s} \times 1.50 \times 10^{-3} \,\text{s}\) Now, find the angular acceleration.
03

(c) Calculate the torque acting on the limb

To find the torque acting on the limb, we will use the formula below: \(\tau = I \alpha\) where \(\tau\) = torque \(I\) = rotational inertia \(\alpha\) = angular acceleration Find the torque by plugging in the values.
04

(d) Calculate the muscular force required to achieve the blow

Finally, to find the muscular force, we will use the relationship between torque and force: \(\tau = Fr\) where \(F\) = muscular force \(r\) = distance from the joint = \(3.00 \,\text{mm} = 3.00 \times 10^{-3} \,\text{m}\) Now, find the muscular force by rearranging the formula and substituting the values: \(F = \frac{\tau}{r}\)

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 solid sphere is rolling without slipping or sliding down a board that is tilted at an angle of \(35^{\circ}\) with respect to the horizontal. What is its acceleration?

Derive the rotational form of Newton's second law as follows. Consider a rigid object that consists of a large number \(N\) of particles. Let \(F_{i}, m_{i},\) and \(r_{i}\) represent the tangential component of the net force acting on the ith particle, the mass of that particle, and the particle's distance from the axis of rotation, respectively. (a) Use Newton's second law to find \(a_{i}\), the particle's tangential acceleration. (b) Find the torque acting on this particle. (c) Replace \(a_{i}\) with an equivalent expression in terms of the angular acceleration \(\alpha\) (d) Sum the torques due to all the particles and show that $$\sum_{i=1}^{N} \tau_{i}=I \alpha$$
A solid sphere of mass 0.600 kg rolls without slipping along a horizontal surface with a transnational speed of \(5.00 \mathrm{m} / \mathrm{s} .\) It comes to an incline that makes an angle of \(30^{\circ}\) with the horizontal surface. Ignoring energy losses due to friction, to what vertical height above the horizontal surface does the sphere rise on the incline?
A large clock has a second hand with a mass of \(0.10 \mathrm{kg}\) concentrated at the tip of the pointer. (a) If the length of the second hand is $30.0 \mathrm{cm},$ what is its angular momentum? (b) The same clock has an hour hand with a mass of \(0.20 \mathrm{kg}\) concentrated at the tip of the pointer. If the hour hand has a length of \(20.0 \mathrm{cm},\) what is its angular momentum?
In many problems in previous chapters, cars and other objects that roll on wheels were considered to act as if they were sliding without friction. (a) Can the same assumption be made for a wheel rolling by itself? Explain your answer. (b) If a moving car of total mass \(1300 \mathrm{kg}\) has four wheels, each with rotational inertia of \(0.705 \mathrm{kg} \cdot \mathrm{m}^{2}\) and radius of \(35 \mathrm{cm},\) what fraction of the total kinetic energy is rotational?
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