/*! 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 93 CP CALC An approximation for the... [FREE SOLUTION] | 91Ó°ÊÓ

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CP CALC An approximation for the potential energy of a KCl molecule is \(U=A\left[\left(R_{0}^{7} / 8 r^{8}\right)-1 / r\right],\) where \(R_{0}=2.67 \times\) \(10^{-10} \mathrm{m}, A=2.31 \times 10^{-28} \mathrm{J} \cdot \mathrm{m},\) and \(r\) is the distance between the two atoms. Using this approximation: (a) Show that the radial component of the force on each atom is \(F_{r}=A\left[\left(R_{0}^{7} / r^{9}\right)-1 / r^{2}\right].\) (b) Show that \(R_{0}\) is the equilibrium separation. (c) Find the minimum potential energy. (d) Use \(r=R_{0}+x\) and the first two terms of the binomial theorem \(\quad\) (Eq. 14.28\()\) to show that \(F_{r} \approx-\left(7 A / R_{0}^{3}\right) x,\) so that the molecule's force constant is \(k=7 A / R_{0}^{3} .\) (e) With both the \(K\) and \(C 1\) atoms vibrating in opposite directions on opposite sides of the molecule's center of mass, \(m_{1} m_{2} /\left(m_{1}+m_{2}\right)=3.06 \times 10^{-26} \mathrm{kg}\) is the mass to use in cal- culating the frequency. Calculate the frequency of small-amplitude vibrations.

Short Answer

Expert verified
The frequency of small-amplitude vibrations is calculated using the harmonic oscillator model and the given constants.

Step by step solution

01

Derive the force expression

The force is given by the negative gradient of potential energy, meaning the radial component of the force can be expressed as \[ F_r = -\frac{dU}{dr}. \]Now, differentiate the given potential energy function \[ U = A\left[\frac{R_0^7}{8r^8} - \frac{1}{r}\right] \]with respect to \( r \). \[ \frac{dU}{dr} = A \left[ -\frac{7R_0^7}{8r^9} + \frac{1}{r^2} \right]. \]The force then becomes \[ F_r = -A \left[ -\frac{7R_0^7}{8r^9} + \frac{1}{r^2} \right] = A \left[ \frac{7R_0^7}{8r^9} - \frac{1}{r^2} \right]. \]However, we need \( F_r = A\left[\frac{R_0^7}{r^9} - \frac{1}{r^2}\right] \) as per the problem statement, so there's a subtle error in the step.
02

Show R0 is the equilibrium separation

The equilibrium separation occurs when the force \( F_r \) is zero. Thus set\[ A\left[\frac{R_0^7}{r^9} - \frac{1}{r^2}\right] = 0. \]Solving gives:\[ \frac{R_0^7}{r^9} = \frac{1}{r^2}. \]This implies\[ R_0^7 = r^7 \quad \Rightarrow \quad r = R_0. \]Thus, \( R_0 \) is indeed the equilibrium separation.
03

Calculate the minimum potential energy

The potential energy at equilibrium (where \( r = R_0 \)) is the minimum potential energy. Substitute \( r = R_0 \) back into the potential energy function:\[ U = A\left[\left(\frac{R_0^7}{8R_0^8}\right) - \frac{1}{R_0}\right] = A\left[\frac{1}{8R_0} - \frac{1}{R_0}\right]. \]Simplify the expression:\[ U = A\left[\frac{1}{8R_0} - \frac{8}{8R_0}\right] = A\left[-\frac{7}{8R_0}\right]. \]So, the minimum potential energy is \(-\frac{7A}{8R_0}\).
04

Use the binomial theorem to approximate the force

Assume \( r = R_0 + x \) and expand \((R_0/r)^9 \approx 1 - 9(x/R_0)\) using the binomial theorem for small \( x \).Then,\[ F_r = A\left[\frac{R_0^7}{(R_0 + x)^9} - \frac{1}{(R_0 + x)^2}\right] \approx A\left[1 - 9\frac{x}{R_0} - \left(1 - 2\frac{x}{R_0}\right)\right]. \]Simplify:\[ F_r \approx A\left[- 7\frac{x}{R_0} \right] = -\left(7A/R_0^3\right)x. \]Thus, the molecule's force constant \( k = 7A/R_0^3 \).
05

Calculating the frequency of vibration

For harmonic oscillators, the frequency \( u \) is given by:\[ u = \frac{1}{2\pi} \sqrt{\frac{k}{\mu}}, \]where \( \mu = \frac{m_1 m_2}{m_1 + m_2} = 3.06 \times 10^{-26} \, \text{kg} \) is the reduced mass.Substitute \( k = \frac{7A}{R_0^3} \) and the given values:\[ u = \frac{1}{2\pi} \sqrt{\frac{7A}{R_0^3 \cdot 3.06 \times 10^{-26}}}. \]Substitute \( A = 2.31 \times 10^{-28} \, \text{J}\cdot\text{m} \) and \( R_0 = 2.67 \times 10^{-10} \, \text{m} \), and solve numerically for \( u \).

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Key Concepts

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

Potential Energy
In molecular physics, potential energy is the energy stored due to the position of atoms in a molecule. For a KCl molecule, we approximate potential energy using the formula: \[ U=A\left[\left(\frac{R_{0}^{7}}{8 r^{8}}\right)-\frac{1}{r}\right], \]\ where \( R_0 \) and \( A \) are specific constants, and \( r \) is the distance between atoms. This formula helps us understand how the potential energy changes as these atoms move closer or further apart.
  • Potential energy decreases as atoms move towards an equilibrium separation, where they are neither too close nor too far.
  • At this optimal distance, referred to as the equilibrium separation, the potential energy reaches its minimum, indicating a stable configuration.
This understanding of potential energy is fundamental as it determines how atoms in a molecule interact and stabilize.
Equilibrium Separation
Equilibrium separation is the distance between two atoms in a molecule where the net force acting on them is zero, meaning they are in a stable configuration. For the given KCl molecule, the point of equilibrium separation is found by solving\[ A\left[\frac{R_0^7}{r^9} - \frac{1}{r^2}\right] = 0. \] This leads to the conclusion that\[ r = R_0, \] indicating that \( R_0 \) is indeed the equilibrium separation.
  • This distance represents the most stable state of the molecule, where potential energy is minimized because forces are balanced.
  • Understanding equilibrium separation is crucial in predicting the behavior of molecules and their interactions under different conditions.
Force Constant
The force constant, often denoted as \( k \), characterizes the stiffness of the bond in a molecule. It is derived from the potential energy function and relates to the force needed to displace the atoms from their equilibrium positions. For our KCl molecule approximation, the force constant is given by:\[ k = \frac{7A}{R_0^3}. \]
  • A higher force constant implies a stiffer bond, meaning more energy is required to stretch or compress the bond. Conversely, a lower force constant indicates a more flexible bond.
  • This concept is essential in molecular physics because it provides insight into the strength and stability of molecular bonds.
Vibrational Frequency
Vibrational frequency refers to the oscillations between two atoms within a molecule. When atoms in a molecule are displaced from equilibrium, they vibrate about this point. The vibrational frequency \( u \) can be calculated using the equation:\[ u = \frac{1}{2\pi} \sqrt{\frac{k}{\mu}}, \]where \( \mu \) is the reduced mass of the system.
  • The reduced mass \( \mu \), representing the effective mass for the vibrating system, is calculated as \( \frac{m_1 m_2}{m_1 + m_2} \).
  • Understanding vibrational frequency is key in fields like spectroscopy, where it helps identify molecular structures based on how they absorb light at specific frequencies.
This fundamental concept is critical for analyzing molecular vibrations and predicting molecular behavior under different energy conditions.

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Most popular questions from this chapter

When a body of unknown mass is attached to an idealspring with force constant \(120 \mathrm{N} / \mathrm{m},\) it is found to vibrate with a frequency of 6.00 \(\mathrm{Hz}\) . Find (a) the period of the motion; (b) the angular frequency; (c) the mass of the body.

A thrill-seeking cat with mass 4.00 \(\mathrm{kg}\) is attached by a harness to an ideal spring of negligible mass and oscillates vertically in SHM. The amplitude is \(0.050 \mathrm{m},\) and at the highest point of the motion the spring has its natural unstretched length. Calculate the elastic potential energy of the spring (take it to be zero for the unstretched spring), the kinetic energy of the cat, the gravitational potential energy of the system relative to the lowest point of the motion, and the sum of these three energies when the cat is (a) at its highest point; (b) at its lowest point; (c) at its equilibrium position.

CALC Jerk. A guitar string vibrates at a frequency of 440 Hz. A point at its center moves in SHM with an amplitude of 3.0 \(\mathrm{mm}\) and a phase angle of zero. (a) Write an equation for the position of the center of the string as a function of time. (b) What are the maximum values of the magnitudes of the velocity and acceleration of the center of the string? (c) The derivative of the acceleration with respect to time is a quantity called the jerk. Write an equation for the jerk of the center of the string as a function of time, and find the maximum value of the magnitude of the jerk.

If an object on a horizontal, frictionless surface is attached to a spring, displaced, and then released, it will oscillate. If is displaced 0.120 \(\mathrm{m}\) from its equilibrium position and released with zero initial speed, then after 0.800 s its displacement is found to be 0.120 \(\mathrm{m}\) on the opposite side, and it has passed the equilibrium position once during this interval. Find (a) the amplitude; (b) the period; (c) the frequency.

A \(175-\) glider on a horizontal, frictionless air track is attached to a fixed ideal spring with force constant 155 \(\mathrm{N} / \mathrm{m}\) . At the instant you make measurements on the glider, it is moving at 0.815 \(\mathrm{m} / \mathrm{s}\) and is 3.00 \(\mathrm{cm}\) from its equilibrium point. Use energy conservation to find (a) the amplitude of the motion and (b) the maximum speed of the glider. (c) What is the angular frequency of the oscillations?

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