Ch 23: Electric Potential

Young & Freedman Calc - University Physics 15th Edition

Young & Freedman Calc15th EditionUniversity PhysicsISBN: 9780135159552Non è quello che usi tu?Cambia libro di testo

Young & Freedman Calc 15th Edition

Ch 23: Electric Potential

Problema 18a

Capitolo 23, Problema 18a

Two point charges of equal magnitude $Q$ are held a distance $d$ apart. Consider only points on the line passing through both charges. If the two charges have the same sign, find the location of all points (if there are any) at which (i) the potential (relative to infinity) is zero (is the electric field zero at these points?), and (ii) the electric field is zero (is the potential zero at these points?).

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Understand the concept of electric potential and electric field. The electric potential at a point due to a point charge is given by $ V = \frac{kQ}{r} $, where $ k $ is Coulomb's constant, $ Q $ is the charge, and $ r $ is the distance from the charge. The electric field due to a point charge is given by $ E = \frac{kQ}{r^2} $.

For part (a)(i), consider the potential due to two charges of the same sign. The potential at a point on the line is the algebraic sum of the potentials due to each charge. Set up the equation $ V = \frac{kQ}{r_1} + \frac{kQ}{r_2} = 0 $, where $ r_1 $ and $ r_2 $ are the distances from the point to each charge. Solve for the location where this condition is satisfied.

Determine if the electric field is zero at the points where the potential is zero. The electric field is the vector sum of the fields due to each charge. Set up the equation $ E = \frac{kQ}{r_1^2} - \frac{kQ}{r_2^2} = 0 $ (since the charges are of the same sign, the fields will oppose each other). Solve for the location where this condition is satisfied.

For part (a)(ii), find the location where the electric field is zero. Use the equation $ E = \frac{kQ}{r_1^2} - \frac{kQ}{r_2^2} = 0 $ and solve for the point where the fields cancel each other out. Check if the potential is zero at these points by substituting back into the potential equation.

Summarize the findings: Points where the potential is zero are not necessarily where the electric field is zero, and vice versa. Analyze the conditions under which these phenomena occur, considering the symmetry and properties of electric fields and potentials.

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Electric Potential

Electric potential at a point is the work done per unit charge in bringing a positive test charge from infinity to that point. For two like charges, the potential at a point is the algebraic sum of potentials due to each charge. Points where the potential is zero are equidistant from both charges, but the electric field may not be zero at these points.

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Electric Potential

Electric Field

The electric field is a vector field representing the force experienced by a unit positive charge at a point in space. For two like charges, the field is zero at a point where the forces due to each charge cancel each other out. At these points, the potential is not necessarily zero, as potential is a scalar quantity.

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Intro to Electric Fields

Superposition Principle

The superposition principle states that the net electric field or potential at a point is the vector or algebraic sum of fields or potentials due to individual charges. This principle is crucial for calculating the potential and field at any point on the line between two charges, allowing us to determine where these quantities are zero.

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Superposition of Sinusoidal Wave Functions

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