/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 99 A crustacean (Hemisquilla ensige... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

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 91Ó°ÊÓ!

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 skater is initially spinning at a rate of 10.0 rad/s with a rotational inertia of \(2.50 \mathrm{kg} \cdot \mathrm{m}^{2}\) when her arms are extended. What is her angular velocity after she pulls her arms in and reduces her rotational inertia to \(1.60 \mathrm{kg} \cdot \mathrm{m}^{2} ?\)
Two children standing on opposite sides of a merry-goround (see Fig. 8.5 ) are trying to rotate it. They each push in opposite directions with forces of magnitude \(10.0 \mathrm{N} .\) (a) If the merry-go-round has a mass of $180 \mathrm{kg}\( and a radius of \)2.0 \mathrm{m},$ what is the angular acceleration of the merry-go-round? (Assume the merry-go-round is a uniform disk.) (b) How fast is the merry-go-round rotating after \(4.0 \mathrm{s} ?\)
A 1.10 -kg bucket is tied to a rope that is wrapped around a pole mounted horizontally on friction-less bearings. The cylindrical pole has a diameter of \(0.340 \mathrm{m}\) and a mass of \(2.60 \mathrm{kg} .\) When the bucket is released from rest, how long will it take to fall to the bottom of the well, a distance of \(17.0 \mathrm{m} ?\)
A Ferris wheel rotates because a motor exerts a torque on the wheel. The radius of the London Eye, a huge observation wheel on the banks of the Thames, is \(67.5 \mathrm{m}\) and its mass is \(1.90 \times 10^{6} \mathrm{kg} .\) The cruising angular speed of the wheel is $3.50 \times 10^{-3} \mathrm{rad} / \mathrm{s} .$ (a) How much work does the motor need to do to bring the stationary wheel up to cruising speed? [Hint: Treat the wheel as a hoop.] (b) What is the torque (assumed constant) the motor needs to provide to the wheel if it takes 20.0 s to reach the cruising angular speed?
A uniform door weighs \(50.0 \mathrm{N}\) and is \(1.0 \mathrm{m}\) wide and 2.6 m high. What is the magnitude of the torque due to the door's own weight about a horizontal axis perpendicular to the door and passing through a corner?
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.