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Identical \(+1.8 \mu \mathrm{C}\) charges are fixed to adjacent corners of a square. What charge (magnitude and algebraic sign) should be fixed to one of the empty corners, so that the total electric potential at the remaining empty corner is \(0 \mathrm{V} ?\)

Short Answer

Expert verified
The charge needed is \(-3.6 \mu C\).

Step by step solution

01

Understand Electric Potential

Electric potential at a point due to a point charge \( q \) is given by the formula \( V = \frac{kq}{r} \), where \( k \) is the Coulomb's constant \( 8.99 \times 10^9 \text{ N m}^2/\text{C}^2 \), and \( r \) is the distance to the point from the charge. In this problem, we need to consider the contributions of potentials from multiple charges and determine the charge needed at the third corner to make their total zero.
02

Calculate Contribution from Existing Charges

Consider the square with charges at corners \( A \) and \( B \). The charge at \( A \) contributes a potential \( V_A = \frac{k (1.8 \times 10^{-6})}{d} \) at the empty corner \( C \), and similarly, charge at \( B \) contributes \( V_B = \frac{k (1.8 \times 10^{-6})}{d} \), where \( d \) is the side of the square. Summing these gives \( V_{AB} = \frac{2k (1.8 \times 10^{-6})}{d} \).
03

Set Total Potential to Zero

Let the charge at the empty corner \( D \) be \( q \). The potential due to this charge at the opposite empty corner \( C \) will be \( V_D = \frac{kq}{ ext{side}} \), as \( D \) is at a diagonal distance. To ensure the total electric potential at \( C \) is zero, we have \( V_{AB} + V_D = 0 \). Thus, \( \frac{2k (1.8 \times 10^{-6})}{d} + \frac{kq}{ ext{side}} = 0 \).
04

Solve for Unknown Charge \( q \)

Since the charges are identical and situated at a right angle, \( d \) serves as the diagonal as well. Hence, solve for \( q \) using \( 2 \times 1.8 \mu\text{C} + q = 0 \) which simplifies to \( q = -3.6 \mu\text{C} \). Therfore, the required charge has a magnitude of \( 3.6 \mu\text{C} \) and is negatively charged.

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Key Concepts

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

Point Charge
A point charge is a hypothetical charge located at a single point in space. This is a fundamental concept in electrostatics, used to simplify the analysis of electric fields and potentials. Instead of considering a charge distributed over a larger volume, a point charge is a highly concentrated form, allowing easier calculations of its influence. In most physics problems, point charges are assumed to be infinitesimally small, meaning their actual size is negligible compared to the distances involved. This allows us to focus solely on their charge and its effects.

The electric potential due to a point charge is a key element in calculating forces and interactions between charges. It helps us to understand how charged particles influence one another over a distance. This simplification is very useful in theoretical physics, enabling us to compute interactions between charges even in complex arrangements.
Coulomb's Law
Coulomb's Law is a central law in electrostatics that describes the force between two point charges. It shows that the electric force between two point charges is directly proportional to the product of their magnitudes and inversely proportional to the square of the distance between them. Mathematically, it is given by:
\[F = \frac{k |q_1 q_2|}{r^2}\]
where
  • \( F \) is the force between the charges,
  • \( k \) is the Coulomb's constant (\( 8.99 \times 10^9 \text{ N m}^2/ ext{C}^2 \)),
  • \( q_1 \) and \( q_2 \) are the magnitudes of the charges,
  • \( r \) is the distance between the charges.
This law is analogous to Newton's law of gravitation in that the electric force acts at a distance, and it can attract or repel depending on the signs of the charges. Like charges repel each other, while opposite charges attract.

When charges are part of a larger system, like in our square configuration, Coulomb's Law helps calculate the forces and potential at any given point, based on the sum of individual contributions from each point charge.
Electric Potential Zero
The concept of electric potential zero is crucial in understanding how different charges influence each other. Electric potential is the amount of work required to move a unit positive charge from a reference point to a specific point inside an electric field without producing any acceleration. When the total electric potential at a point is zero, it implies that there's no net gain or loss in potential energy for a test charge placed at that point.

In many electrostatic problems, like the one described in the exercise, the objective is to find a configuration where the electric potential at a certain point becomes zero. This involves carefully balancing the contributions from multiple charges, ensuring that their combined effect nullifies each other at the desired location. In essence, achieving zero electric potential at a point means the influences of all charges in question perfectly cancel out.
  • For the square with charges at two corners, we aim to find a charge at a third corner such that the total potential at the remaining corner is zero.
  • This typically involves introducing a charge of opposite sign and specific magnitude to counteract the effects of the existing charges.
Understanding how to achieve a zero potential is a fundamental skill in electrostatics, allowing one to predict and control electric field behavior effectively.

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Most popular questions from this chapter

'I'he membrane that surrounds a certain type of living cell has a surface area of \(5.0 \times 10^{-9} \mathrm{m}^{2}\) and a thickness of \(1.0 \times 10^{-8} \mathrm{m} .\) Assume that the membrane behaves like a parallel plate capacitor and has a dielectric constant of \(5.0 .\) (a) The potential on the outer surface of the membrane is \(+60.0 \mathrm{mV}\) greater than that on the inside surface. How much charge resides on the outer surface? (b) If the charge in part (a) is due to positive ions (charge \(+e\) ), how many such ions are present on the outer surface?

Four identical charges \((+2.0 \mu \mathrm{C}\) each \()\) are brought from infinity and fixed to a straight line. The charges are located \(0.40 \mathrm{m}\) apart. Determine the electric potential energy of this group.

A moving particle encounters an external electric field that decreases its kinetic energy from \(9520 \mathrm{eV}\) to \(7060 \mathrm{eV}\) as the particle moves from position \(A\) to position \(B .\) The electric potential at \(A\) is \(-55.0 \mathrm{V},\) and the electric potential at \(B\) is +27.0 V. Determine the charge of the particle. Include the algebraic sign \((+\) or \(-\) ) with your answer.

A spark plug in an automobile engine consists of two metal conductors that are separated by a distance of \(0.75 \mathrm{mm} .\) When an electric spark jumps between them, the magnitude of the electric field is \(4.7 \times\) \(10^{7} \mathrm{V} / \mathrm{m} .\) What is the magnitude of the potential difference \(\Delta V\) between the conductors?

What is the capacitance of a capacitor that stores \(4.3 \mu \mathrm{C}\) of charge on its plates when a voltage of \(1.5 \mathrm{V}\) is applied between them?

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