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Four identical charges \(Q\) are placed at the corners of a square of side \(L\). (a) In a free-body diagram, show all of the forces that act on one of the charges. (b) Find the magnitude and direction of the total force exerted on one charge by the other three charges.

Short Answer

Expert verified
The total force on one charge is \( \frac{kQ^2}{L^2} \sqrt{3} \), directed away from the charge towards the diagonal center of the opposite side.

Step by step solution

01

Understand the Setup of the Problem

We have a square with charges placed at each corner. Let's label the charges at the corners as 1, 2, 3, and 4, with charge 1 being the one we are focusing on for analysis. Each charge has a magnitude of \( Q \) and the side length of the square is \( L \). We need to find the forces acting on charge 1.
02

Draw the Free-Body Diagram

For charge 1, identify the other charges: charge 2 (neighbor along one side), charge 3 (diagonal), and charge 4 (neighbor along the other side). Charge 1 experiences repulsive forces away from each charge since like charges repel. Draw vectors on charge 1 showing force direction: \( F_{12} \), \( F_{13} \), \( F_{14} \). These vectors point directly away from charges 2, 3, and 4, respectively.
03

Calculate Each Force Magnitude

Use Coulomb’s Law to calculate the force between each pair: - For force from charge 2: \( F_{12} = \frac{kQ^2}{L^2} \).- For force from charge 4: \( F_{14} = \frac{kQ^2}{L^2} \).- For force from charge 3 (diagonal): \( F_{13} = \frac{kQ^2}{2L^2} \) because the diagonal distance \( d = \sqrt{L^2 + L^2} = \sqrt{2}L \).
04

Find the Resultant Force from Neighboring Charges

The forces from charges 2 and 4, \( F_{12} \) and \( F_{14} \), are perpendicular. Use vector addition: the resultant force from these charges combines as a vector of magnitude \( \sqrt{(F_{12})^2 + (F_{14})^2} = \sqrt{2} \frac{kQ^2}{L^2} \).
05

Combine Forces to Find Total Force on Charge 1

The force \( F_{13} \) acts along the diagonal direction of the square. Combine this force with the diagonal resultant from Step 4 using vector addition. The total force magnitude (\( F_{total} \)) can be found by:\[ F_{total} = \sqrt{(\sqrt{2} \frac{kQ^2}{L^2})^2 + \left( \frac{kQ^2}{2L^2} \right)^2} \]Upon calculation, \[ F_{total} = \frac{kQ^2}{L^2} \sqrt{3} \].
06

Direction of the Total Force

The resultant force from charges 2 and 4 is \( \sqrt{2} \frac{kQ^2}{L^2} \) in a vector direction of 45° relative to the horizontal and vertical (due to equal perpendicular vectors). The total force is resultant of this and the additional straight diagonal force from charge 3, effectively pulling charge 1 diagonally away from the center towards the midpoint of the opposite diagonal.

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Key Concepts

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

Coulomb's Law
Coulomb's Law is fundamental in understanding electric forces between stationary charges. It describes how the force between two point charges is proportional to the product of their charges and inversely proportional to the square of the distance between them. The formula for this law is expressed as: \[ F = \frac{k \cdot |q_1 \cdot q_2|}{r^2} \] where:
  • \( F \) is the magnitude of the force between the charges,
  • \( k \) is Coulomb's constant, approximately \( 8.98 \times 10^9 \, \text{N} \cdot \text{m}^2/\text{C}^2 \),
  • \( q_1 \) and \( q_2 \) are the magnitudes of the charges,
  • \( r \) is the distance between the charges.
In this specific exercise, each corner of a square holds a charge, exhibiting repulsive forces due to their identical nature. Coulomb's Law helps identify these magnitudes and directions. Applying this law allows us to calculate the magnitude of the forces acting between each pair of charges accurately, which is essential for understanding the overall electric interaction in the system.
Vector Addition
When multiple forces act on an object, like the charges in this system, we need to consider how these forces combine mathematically and geometrically. This is accomplished through vector addition. Electric forces are vectors, meaning they have both magnitude and direction. Vector addition allows us to find a single equivalent force, known as the resultant force, from combining several vectors.
In this exercise, charges at the corners influence each other, requiring vector addition to calculate the effect on a single charge. Imagine arrows pointing from one charge towards (or away) from another charge, representing their forces. Using the Pythagorean theorem and trigonometric concepts, we can translate these multi-directional forces into one resultant vector. This resultant vector simplifies our understanding of how the charges collectively interact, proving critical in solving many physics problems where multiple vectors are involved.
Free-Body Diagram
A free-body diagram is essential for visualizing the different forces acting upon an object. In our example, where charges are positioned at the corners of a square, a free-body diagram helps represent and simplify understanding of all forces involved. Each charge experiences a force from every other charge due to electric repulsion.
To make one:
  • Select the charge you are interested in, like charge 1 at the square's corner.
  • Draw a dot or small circle representing this charge.
  • From this charge, draw arrows (vectors) indicating the direction of repulsive forces from the other charges.
  • Label each arrow with its designated force like \( F_{12} \), \( F_{13} \), and \( F_{14} \).
This diagram simplifies complex problems by transforming the electric interactions into a clear visual map of forces at play, making it easier to apply concepts like vector addition and Coulomb's Law.
Resultant Force
The resultant force is the single force that results from the combination of all individual forces acting on an object. In our exercise, with charges located at the corners of a square, the resultant force on one specific charge is derived by combining all the forces exerted by the other three charges.
To find this, first apply vector addition to the perpendicular forces, typically those shared along the sides of the square. Then, incorporate diagonal forces acting across the longer distance of the square.
For example, if charges at two adjacent corners exert forces \( F_{12} \) and \( F_{14} \) on charge 1, these are added as vectors, often resulting in a direction of 45° along the diagonal due to similar magnitude and direction. Adding in a force from a charge directly across from you like \( F_{13} \), requires finding all components and solving using the Pythagorean theorem: \[ F_{total} = \sqrt{(\text{sum of all components})^2} \] Ultimately, understanding the resultant force is invaluable, as it provides a comprehensive picture of how all forces influence the charge in question, guiding expected physical behavior in electric fields.

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Most popular questions from this chapter

Two point charges are located on the \(y\)-axis as follows: charge \(q_1 = -1.50 \)nC at \(y = -\)0.600 m, and charge \(q_2 = +\)3.20 nC at the origin \((y = 0)\). What is the total force (magnitude and direction) exerted by these two charges on a third charge \(q_3 = +\)5.00 nC located at \(y = -\)0.400 m ?

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Three point charges are arranged on a line. Charge \(q_3 = +\)5.00 nC and is at the origin. Charge \(q_2 = -\)3.00 nC and is at \(x = +\)4.00 cm. Charge \(q_1\) is at \(x = +\)2.00 cm. What is \(q_1\) (magnitude and sign) if the net force on \(q_3\) is zero?

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