(III) A scallop force opens its shell with an elastic material called abductin, whose Young’s modulus is about \({\bf{2}}{\bf{.0 \times 1}}{{\bf{0}}^{\bf{6}}}\;{\bf{N/}}{{\bf{m}}^{\bf{2}}}\). If this piece of abductin is 3.0 mm thick and has a cross-sectional area of \({\bf{0}}{\bf{.50}}\;{\bf{c}}{{\bf{m}}^{\bf{2}}}\), how much potential energy does it store when compressed by 1.0 mm?

Short Answer

Expert verified

The stored potential energy is \(1.7 \times {10^{ - 2}}\;{\rm{J}}\).

Step by step solution

01

Concepts

The stored potential energy is \(U = \frac{1}{2}F\Delta l\).For this problem, first, find the force from the given values of the Young modulus, compression, areas, and initial length.

02

Explanation

The Young’s modulus is \(E = 2.0 \times {10^6}\;{\rm{N/}}{{\rm{m}}^{\rm{2}}}\).

The thickness of the material sample is \({l_ \circ } = 3.0\;{\rm{mm}} = 3.0 \times {10^{ - 3}}\;{\rm{m}}\).

The cross-sectional area of the material sample is \(A = 0.50\;{\rm{c}}{{\rm{m}}^{\rm{2}}} = 0.50 \times {10^{ - 4}}\;{{\rm{m}}^{\rm{2}}}\).

The compression of the sample metrical is \(\Delta l = 1.0\;{\rm{mm}} = 1.0 \times {10^{ - 3}}\;{\rm{m}}\).

Let F be the force on the material.

03

Calculation

Now, the force on the material can be written as

\(\begin{array}{c}E = \frac{{\frac{F}{A}}}{{\frac{{\Delta l}}{{{l_ \circ }}}}}\\\frac{F}{A} = E\frac{{\Delta l}}{{{l_ \circ }}}\\F = EA\frac{{\Delta l}}{{{l_ \circ }}}\end{array}\).

Now, the stored potential energy stored in the material due to compression is

\(\begin{array}{c}U = \frac{1}{2}F\Delta l\\ = \frac{1}{2}EA\frac{{\Delta l}}{{{l_ \circ }}}\Delta l\\ = \frac{1}{2}EA\frac{{{{\left( {\Delta l} \right)}^2}}}{{{l_ \circ }}}\end{array}\).

Now, substituting the values in the above equation,

\(\begin{array}{c}U = \frac{1}{2}EA\frac{{{{\left( {\Delta l} \right)}^2}}}{{{l_ \circ }}}\\ = \frac{1}{2} \times \left( {2.0 \times {{10}^6}\;{\rm{N/}}{{\rm{m}}^{\rm{2}}}} \right) \times \left( {0.50 \times {{10}^{ - 4}}\;{{\rm{m}}^{\rm{2}}}} \right) \times \frac{{{{\left( {1.0 \times {{10}^{ - 3}}\;{\rm{m}}} \right)}^2}}}{{3.0 \times {{10}^{ - 3}}\;{\rm{m}}}}\\ = 1.7 \times {10^{ - 2}}\;{\rm{J}}\end{array}\).

Hence, the stored potential energy is \(1.7 \times {10^{ - 2}}\;{\rm{J}}\).

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

As you increase the force that you apply while pulling on a rope, which of the following is not affected?

(a) The stress on the rope

(b) The strain on the rope

(c) The Young’s modulus of the rope

(d) All of the above

(e) None of the above

(II) If 25 kg is the maximum mass mthat a person can hold in a hand when the arm is positioned with a 105° angle at the elbow as shown in Fig. 9–74, what is the maximum force\({F_{{\bf{max}}}}\) that the biceps muscle exerts on the forearm? Assume the forearm and hand have a total mass of 2.0 kg with a CG that is 15 cm from the elbow, and that the biceps muscle attaches 5.0 cm from the elbow.

(III) A uniform ladder of mass mand length leans at an angle\(\theta \)against a frictionless wall, Fig. 9–70. If the coefficient of static friction between the ladder and the ground is\({\mu _s}\). Determine a formula for the minimum angle at which the ladder will not slip.

The roof over a \({\bf{9}}{\bf{.0}}\;{\bf{m \times 10}}{\bf{.0}}\;{\bf{m}}\) room in a school has a total mass of 13,600 kg. The roof is to be supported by vertical wooden (actually about \({\bf{4}}{\bf{.0}}\;{\bf{cm \times 9}}{\bf{.0}}\;{\bf{cm}}\)) equally spaced along the 10.0-m sides. How many supports are required on each side, and how far apart must they be? Consider only compression, and assume a safety factor of 12.

When you apply the torque equation \(\sum {\tau = 0} \) to an object in equilibrium, the axis about which the torques are calculated

(a) must be located at a pivot.

(b) must be located at the object’s center of gravity.

(c) should be located at the edge of the object.

(d) can be located anywhere.

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