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Ch 23: The Electric Field
Knight Calc - Physics for Scientists and Engineers 5th Edition
Knight Calc5th EditionPhysics for Scientists and EngineersISBN: 9780137344796Not the one you use?Change textbook
Chapter 23, Problem 61b

An electric field can induce an electric dipole in a neutral atom or molecule by pushing the positive and negative charges in opposite directions. The dipole moment of an induced dipole is directly proportional to the electric field. That is, p=αE\(\overrightarrow{p}\)=\(\alpha\]\overrightarrow{E}\), where α is called the polarizability of the molecule. A bigger field stretches the molecule farther and causes a larger dipole moment. An ion with charge q is distance r from a molecule with polarizability α. Find an expression for the force E\(\overrightarrow{E}\)ion on dipole.

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Step 1: Begin by understanding the relationship between the electric field created by the ion and the dipole moment induced in the molecule. The electric field due to a point charge q at a distance r is given by the formula: Eion=kqr2, where k is Coulomb's constant.
Step 2: Use the relationship between the dipole moment and the electric field. The dipole moment induced in the molecule is given by: p=αEion. Substitute the expression for Eion from Step 1 into this equation.
Step 3: Recognize that the force on a dipole in an electric field is given by the gradient of the potential energy. The potential energy of a dipole in an electric field is: U=-pEion. The force is then: F=-dUdr.
Step 4: Substitute the expression for U into the force equation. This involves differentiating the product of p and Eion with respect to r. Remember that p itself depends on Eion, which is a function of r.
Step 5: Simplify the resulting expression to find the force. After substituting and differentiating, the force on the dipole due to the ion will be expressed in terms of q, r, α, and k. Ensure the final expression is consistent with the physical principles of electrostatics and dipole interactions.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Electric Field

An electric field is a region around a charged particle where other charged particles experience a force. It is represented by the symbol E and is measured in volts per meter (V/m). The strength and direction of the electric field determine how charged particles, such as ions and dipoles, interact with each other. Understanding electric fields is crucial for analyzing how they induce dipoles in neutral atoms or molecules.
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Dipole Moment

The dipole moment is a vector quantity that represents the separation of positive and negative charges within a system. It is defined as the product of the charge and the distance between the charges, denoted as p = qd. In the context of induced dipoles, the dipole moment is proportional to the strength of the electric field, as expressed by the equation p = αE, where α is the polarizability. This concept is essential for understanding how external electric fields influence molecular behavior.
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Polarizability

Polarizability is a measure of how easily the electron cloud of a molecule can be distorted by an external electric field, resulting in an induced dipole moment. It is denoted by the symbol α and varies among different molecules based on their structure and electron distribution. A higher polarizability indicates that a molecule can develop a larger dipole moment in response to an electric field, which is critical for calculating the force exerted on the dipole by nearby charged particles.
Related Practice
Textbook Question

The two parallel plates in FIGURE P23.53 are 2.0 cm apart and the electric field strength between them is 1.0×104 N/C. An electron is launched at a 45° angle from the positive plate. What is the maximum initial speed v0 the electron can have without hitting the negative plate?

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Textbook Question

A rod of length L lies along the y-axis with its center at the origin. The rod has a nonuniform linear charge density λ=ay λ=a|y|, where a is a constant with the units C/m2. Find the electric field strength of the rod at distance x on the x-axis.

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Textbook Question

A problem of practical interest is to make a beam of electrons turn a 90° corner. This can be done with the parallel-plate capacitor shown in FIGURE P23.55. An electron with kinetic energy 3.0×10−17 J enters through a small hole in the bottom plate of the capacitor. Should the bottom plate be charged positive or negative relative to the top plate if you want the electron to turn to the right? Explain.

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Textbook Question

INT In a classical model of the hydrogen atom, the electron orbits the proton in a circular orbit of radius 0.053 nm. What is the orbital frequency in rev/s? The proton is so much more massive than the electron that you can assume the proton is at rest.

1958
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Textbook Question

A rod of length LL lies along the yy-axis with its center at the origin. The rod has a nonuniform linear charge density λ=ay λ=a|y|, where a is a constant with the units C/m2. Draw a graph of λλ versus yy over the length of the rod.

363
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Textbook Question

A rod of length LL lies along the yy-axis with its center at the origin. The rod has a nonuniform linear charge density λ=ay λ=a|y|, where a is a constant with the units C/m2. Determine the constant a in terms of LL and the rod's total charge QQ.

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