/*! 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 114 A wire suspended vertically from... [FREE SOLUTION] | 91Ó°ÊÓ

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A wire suspended vertically from one of its ends is stretched by attaching a weight of \(200 \mathrm{~N}\) to the lower end. The weight stretches the wire by \(1 \mathrm{~mm}\). Then the elastic energy stored in the wire is \([\mathbf{2 0 0 3}]\) (A) \(0.2 \mathrm{~J}\) (B) \(10 \mathrm{~J}\) (C) \(20 \mathrm{~J}\) (D) \(0.1 \mathrm{~J}\)

Short Answer

Expert verified
The elastic potential energy stored in the wire is \(0.1 \mathrm{~J}\).

Step by step solution

01

Convert displacement unit

First, we need to convert the displacement from millimeters to meters: \[\Delta x = 1 \mathrm{~mm} = 0.001 \mathrm{~m}\]
02

Apply Hooke's Law

Now use Hooke's law to find the spring constant (\(k\)). We know the force (\(F\)) and displacement (\(\Delta x\)): \[F = 200 \mathrm{~N}\] \[\Delta x = 0.001 \mathrm{~m}\] \[F = k \cdot \Delta x\] Rearrange the equation to solve \(k\): \[k = \frac{F}{\Delta x}\]
03

Calculate spring constant

Now, using the known values to find the spring constant (\(k\)): \[k = \frac{200 \mathrm{~N}}{0.001 \mathrm{~m}}\] \[k = 200000 \mathrm{~N/m}\]
04

Calculate elastic potential energy

Finally, we can use the formula for elastic potential energy to find the energy stored in the wire: \[PE_{elastic} = \frac{1}{2} k \cdot \Delta x^2\] \[PE_{elastic} = \frac{1}{2} \cdot 200000 \mathrm{~N/m} \cdot (0.001 \mathrm{~m})^2\] \[PE_{elastic} = 0.1 \mathrm{~J}\] Since the calculated elastic potential energy is \(0.1 \mathrm{~J}\), the correct option is: (D) \(0.1 \mathrm{~J}\)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Hooke's Law
Hooke's Law is a principle of physics that relates the force needed to extend or compress a spring to the distance it extends or compresses. In simpler terms, it tells us that the displacement of the spring is directly proportional to the force applied. The law is named after the 17th-century British scientist Robert Hooke. He first stated the law in 1678 as a Latin anagram, and then translated it to the now-familiar form:
\[ F = k \cdot \Delta x \] where \(\text{F}\) is the force applied to the spring in Newtons (N), \(\text{k}\) is the spring constant that measures the stiffness of the spring in Newtons per meter (N/m), and \(\text{\Delta x}\) is the displacement of the spring from its equilibrium position in meters (m).
This law is the cornerstone for understanding elastic behavior in physics. For an object that can be modeled as a spring, such as a wire as in the above problem, Hooke's law is crucial for calculating how much it will stretch when a force is applied.
Spring Constant
The spring constant \(\text{k}\) is a measure of the stiffness of a spring or elastic material. It is a central concept in Hooke's law, indicating how resistant a spring is to being compressed or stretched. The higher the spring constant, the more force is required for the same amount of displacement. Mathematically, it's represented by the formula:
\[ k = \frac{F}{\Delta x} \] from the original Hooke's law equation. The unit of the spring constant is Newtons per meter (N/m).
In the context of the problem provided, knowing the force applied and the resulting displacement allowed for the calculation of the spring constant. It's essential to ensure that the units are consistent—forces in Newtons and displacement in meters—to avoid calculation errors.
Elastic Energy Calculation
Elastic potential energy is the energy stored in an object when it is stretched or compressed. To calculate this type of energy, one must understand that it directly depends on both the spring constant \(\text{k}\) and the displacement \(\text{\Delta x}\) squared. The formula used for the calculation of elastic potential energy is:
\[ PE_{elastic} = \frac{1}{2} k \cdot \Delta x^2 \] The result will give you the potential energy in Joules (J), which is the standard unit of energy. In the exercise under consideration, this formula was used after first determining the spring constant using Hooke's law. The calculated elastic potential energy was set equal to the work done by the force to stretch the spring, giving the amount of energy stored in the wire.
Physics Problem Solving
Solving physics problems like the one about the stretched wire involves a systematic approach. First, as with the problem given, understanding the question and identifying the relevant physics principles—namely Hooke's law in this case—is critical. Afterward, converting units for consistency is often necessary, as calculations must be in standard units like meters for displacement.
The next step involves algebraically manipulating the equations to find the desired quantities. For this problem, isolating \(\text{k}\) from Hooke's law led to the spring constant, which was then used to find the elastic potential energy. Lastly, substituting the correct values into the energy formula and solving the equation gives the final result. Careful and methodical work, checking units at each step, is key to successful physics problem solving.

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Most popular questions from this chapter

A cricket ball is hit for a six leaving the bat at an angle of \(45^{\circ}\) to the horizontal with kinetic energy \(K\). At the top position, the kinetic energy of the ball is (A) Zero (B) \(K\) (C) \(K / 2\) (D) \(K / \sqrt{2}\)

A body is moved along a straight line by a machine delivering a constant power. The distance moved by the body in time \(t\) is proportional to \([2003]\) (A) \(t^{3 / 4}\) (B) \(t^{3 / 2}\) (C) \(t^{1 / 4}\) (D) \(t^{1 / 2}\)

One end of a light spring of spring constant \(k\) is fixed to a wall and the other end is tied to a block placed on a smooth horizontal surface. In a displacement, the work done by the spring is \(\frac{1}{2} k x^{2}\). The possible cases are: (A) The spring was initially compressed by a distance \(x\) and was finally in its natural length. (B) It was initially stretched by a distance \(x\) and finally was in its natural length. (C) It was initially in its natural length and finally in a compressed position. (D) It was initially in its natural length and finally in a stretched position.

A block of mass \(m\) is released from rest when the extension in the spring is \(x_{0}\). The maximum downward displacement of the block is (A) \(\frac{m g}{2 k}-x_{0}\) (B) \(\frac{m g}{2 k}+x_{0}\) (C) \(\frac{2 m g}{k}-x_{0}\) (D) \(\frac{2 m g}{k}+x_{0}\)

A position-dependent force \(F=x^{2}-3\) Newton acts on a small body of mass \(2 \mathrm{~kg}\) and displaces it from \(x=0\) to \(x=5 \mathrm{~m}\). The work done is (A) \(110 \mathrm{~J}\) (B) \(\frac{80}{3} \mathrm{~J}\) (D) \(\frac{95}{2} \mathrm{~J}\) (D) Zero

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