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Two charges \(A\) and \(B\) are fixed in place, at different distances from a certain spot. At this spot the potentials due to the two charges are equal. Charge \(A\) is 0.18 m from the spot, while charge \(B\) is 0.43 m from it. Find the ratio \(q_{B} / q_{A}\) of the charges.

Short Answer

Expert verified
The ratio \( \frac{q_B}{q_A} \) is approximately 2.39.

Step by step solution

01

Understanding Electric Potential

Electric potential, due to a point charge, is given by the equation \( V = \frac{kq}{r} \), where \( V \) is the potential, \( k \) is Coulomb's constant, \( q \) is the magnitude of the charge, and \( r \) is the distance from the charge to the point in question.
02

Equating Potentials of Both Charges

Since the potentials due to charges \( A \) and \( B \) are equal at the spot, we set their potential equations equal: \( \frac{kq_A}{0.18} = \frac{kq_B}{0.43} \). Here, \( r_A = 0.18 \) m and \( r_B = 0.43 \) m are the distances from the point to charges \( A \) and \( B \), respectively.
03

Simplifying the Equation

Cancel \( k \) from both sides of the equation \( \frac{q_A}{0.18} = \frac{q_B}{0.43} \) since it is common to both terms. This simplifies to \( \frac{q_B}{q_A} = \frac{0.43}{0.18} \).
04

Calculating the Ratio

Calculate the ratio \( \frac{q_B}{q_A} \) by evaluating the right-hand side: \( \frac{0.43}{0.18} \approx 2.39 \). Hence, the ratio of \( q_B \) to \( q_A \) is approximately \( 2.39 \).

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Key Concepts

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

Coulomb's constant
Coulomb's constant, often symbolized as \( k \), plays a crucial role in understanding electric forces and potentials. It is a proportionality constant used in calculations involving the forces or fields of electric charges. The value of Coulomb's constant is approximately \( 8.9875 \times 10^9 \, \text{N m}^2/\text{C}^2 \). This large number indicates that electric forces are potent over distances larger than atomic scales. In the formula for electric potential \( V = \frac{kq}{r} \), \( k \) helps convert the product of the charge \( q \) and its distance from the point \( r \) into a measure of electric potential, which is the energy per unit charge at a point in space. Without \( k \), understanding how individual charge effects translate to forces and potential fields would be much more complicated. Since \( k \) cancels out on both sides when equating equal potentials due to point charges \( A \) and \( B \), it makes determining other quantities, like charge ratios, more straightforward.
Point charge
A point charge is a simplified model representing an electric charge in an idealized form, as if it were concentrated at a single point in space. This abstraction is particularly useful when dealing with the behavior of charges at a distance.In physics problems, point charges allow us to simplify the electric potential and electric field calculations using precise equations such as \( V = \frac{kq}{r} \). The equations become much easier to handle analytically, especially in academic exercises.When solving problems with point charges, it's important to remember that actual charges are usually distributed over some volume. However, for many practical purposes, especially when far from the charge, treating them as point sources yields an accurate description. Point charges are prevalent in theoretical physics and help us dive into concepts of electrostatics without the complications that arise from charge distribution complexity.The solution of the exercise uses the idea of point charges to set up the equation for electric potential, simplifying both the expression and the solution by equating potentials.
Electric charge ratio
The concept of electric charge ratio involves comparing the magnitudes of two or more electric charges. It is particularly useful in determining how different charges influence an electric field or potential at a particular point.In the given problem, the electric charge ratio \( \frac{q_B}{q_A} \) depicts how charge \( B \) compares to charge \( A \) at the spot where their electric potentials are equal. By simplifying the equation: \( \frac{q_A}{0.18} = \frac{q_B}{0.43} \), we arrive at the ratio \( \frac{q_B}{q_A} = \frac{0.43}{0.18} \), which gives approximately \( 2.39 \).This ratio tells us that at this point, charge \( B \) is approximately 2.39 times larger than charge \( A \), assuming the same environment and constant conditions are applied. Understanding electric charge ratios is critical in real-world applications, such as designing electric components where distributed charges are often in play, allowing for the design and control of electric fields and potential differences through calculated charge distributions.

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Most popular questions from this chapter

Two particles each have a mass of \(6.0 \times 10^{-3}\) kg. One has a charge of \(+5.0 \times 10^{-6} \mathrm{C},\) and the other has a charge of \(-5.0 \times 10^{-6} \mathrm{C}\) . They are initially held at rest at a distance of 0.80 \(\mathrm{m}\) apart. Both are then released and accelerate toward each other. How fast is each particle moving when the separation between them is one-third its initial value?

A charge of \(+125 \mu \mathrm{C}\) is fixed at the center of a square that is 0.64 \(\mathrm{m}\) on a side. How much work is done by the electric force as a charge of \(+7.0 \mathrm{\muC}\) is moved from one corner of the square to any other empty corner? Explain.

If the electric field inside a capacitor exceeds the dielectric strength of the dielectric between its plates, the dielectric will break down, discharging and ruining the capacitor. Thus, the dielectric strength is the maximum magnitude that the electric field can have without breakdown occurring. The dielectric strength of air is \(3.0 \times 10^{6} \mathrm{V} / \mathrm{m},\) and that of neoprene rubber is \(1.2 \times 10^{7} \mathrm{V} / \mathrm{m} .\) A certain air-gap, parallel plate capacitor can store no more than 0.075 \(\mathrm{J}\) of electrical energy before breaking down. How much energy can this capacitor store with- out breaking down after the gap between its plates is filled with neoprene rubber?

Two identical point charges \(\left(q=+7.20 \times 10^{-6} \mathrm{C}\right)\) are fixed at diagonally opposite corners of a square with sides of length 0.480 \(\mathrm{m} .\) A test charge \(\left(q_{0}=-2.40 \times 10^{-8} \mathrm{C}\right)\) with a mass of \(6.60 \times 10^{-8} \mathrm{kg},\) is released from rest at one of the empty corners of the square. Determine the speed of the test charge when it reaches the center of the square.

A particle has a charge of \(+1.5 \mu \mathrm{C}\) and moves from point \(A\) to point \(B,\) a distance of 0.20 \(\mathrm{m}\) . The particle experiences a constant elec- tric force, and its motion is along the line of action of the force. The difference between the particle's electric potential energy at \(A\) and at \(B\) is EPE \(_{A}-\mathrm{EPE}_{B}=+9.0 \times 10^{-4} \mathrm{J}\) . (a) Find the magnitude and direction of the electric force that acts on the particle. (b) Find the magnitude and direction of the electric field that the particle experiences.

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