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A charge \(q_1 = +\)5.00 nC is placed at the origin of an \(xy\)-coordinate system, and a charge \(q_2 = -\)2.00 nC is placed on the positive \(x\)-axis at \(x = \)4.00 cm. (a) If a third charge \(q_3 = +\)6.00 nC is now placed at the point \(x =\) 4.00 cm, \(y =\) 3.00 cm, find the \(x\)- and \(y\)-components of the total force exerted on this charge by the other two. (b) Find the magnitude and direction of this force.

Short Answer

Expert verified
Total force on charge is \(7.29 \times 10^{-5}\) N, \(62.0^\circ\) above the negative x-axis.

Step by step solution

01

Determine Distances Between Charges

For the charge configurations, calculate the distances between each pair of charges. The distance between \(q_1\) and \(q_3\) is \( r_{13} = \sqrt{(4.00)^2 + (3.00)^2} = 5.00 \, \text{cm}\). The distance from \(q_2\) to \(q_3\) is \( r_{23} = 3.00 \, \text{cm}\), as both are on the line parallel to the y-axis.
02

Apply Coulomb's Law

Coulomb's Law gives the force between two charges, given by \( F = k \frac{|q_1 q_2|}{r^2}\). Calculate the force between \(q_1\) and \(q_3\): \( F_{13} = 8.99 \times 10^9 \frac{5.00 \times 10^{-9} \times 6.00 \times 10^{-9}}{(0.05)^2} \, \text{N}\approx 1.08 \times 10^{-4} \, \text{N}\). For \(q_2\) and \(q_3\), \( F_{23} = 8.99 \times 10^9 \frac{2.00 \times 10^{-9} \times 6.00 \times 10^{-9}}{(0.03)^2} \, \text{N}\approx 1.20 \times 10^{-4} \, \text{N}\).
03

Resolve Forces Into Components

The force \(F_{13}\) between \(q_1\) and \(q_3\) at an angle has components: \(F_{13,x} = F_{13} \times \cos(\theta) = 1.08 \times 10^{-4} \times \frac{4}{5} = 8.64 \times 10^{-5} \, \text{N}\) and \(F_{13,y} = F_{13} \times \sin(\theta) = 1.08 \times 10^{-4} \times \frac{3}{5} = 6.48 \times 10^{-5} \, \text{N}\). The force \(F_{23}\) acts along the x-axis, so \(F_{23,x} = -1.20 \times 10^{-4} \, \text{N}\), and \(F_{23,y} = 0\).
04

Calculate Total Force Components

Sum the force components to find the total force on \(q_3\). The components are: \((F_{total,x} = 8.64 \times 10^{-5} - 1.20 \times 10^{-4}) \, \text{N} = -3.36 \times 10^{-5} \, \text{N}\) and \(F_{total,y} = 6.48 \times 10^{-5} \, \text{N}\).
05

Find Magnitude and Direction of Total Force

The magnitude of the total force is \(F_{total} = \sqrt{(F_{total,x})^2 + (F_{total,y})^2} = \sqrt{(-3.36 \times 10^{-5})^2 + (6.48 \times 10^{-5})^2} \, \text{N} \approx 7.29 \times 10^{-5} \, \text{N}\). The direction is \( \theta = \tan^{-1}\left(\frac{F_{total,y}}{F_{total,x}}\right) \approx 62.0^\circ \) above the negative x-axis.

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Key Concepts

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

Electric Force
In the world of physics, the electric force is a fundamental concept that describes the interaction between electrically charged particles. It is what keeps electrons attracted to protons, allowing atoms to exist. This force can either pull charges together (attractive) or push them apart (repulsive) depending on their nature. Charges with the same sign repel each other, while opposite charges attract.
This concept is elegantly described by Coulomb's Law, where the electric force between two point charges is given by the formula: \[ F = k \frac{|q_1 q_2|}{r^2} \] Here, \(F\) is the electric force, \(q_1\) and \(q_2\) are the charges, \(r\) is the distance between them, and \(k\) is Coulomb's constant \( (8.99 \times 10^9 \, \text{N} \, \text{m}^2/\text{C}^2) \).
Coulomb's Law tells us that the strength of the force is directly proportional to the product of the charges and inversely proportional to the square of the distance between them. This relationship means that even small charges can exert significant forces on each other if they are very close.
Vector Components
In physics, dealing with forces like the electric force often requires breaking them down into components. This helps in understanding the net effect of multiple forces acting at angles. When dealing with vector components, we split a vector into parts that run parallel to the given axes, usually the \(x\)-axis and \(y\)-axis.
The process of finding vector components begins with the angle of the vector in relation to the axes. Using basic trigonometry:
  • The \(x\)-component of a vector \(F\) at angle \( \theta \) is given by \( F_x = F \cos(\theta) \).
  • The \(y\)-component is \( F_y = F \sin(\theta) \).
Once we have these components, it's much easier to analyze how each force influences the overall motion or position of an object.
Distance Between Charges
The distance between two charges is crucial for calculating the electric force between them using Coulomb’s Law. The force's intensity sharply decreases as the distance increases since it's inversely proportional to the square of the distance.
To calculate this distance, especially when charges are not on a straight line, we often resort to the Pythagorean theorem. For example, if one charge is located at \((x_1, y_1)\) and another at \((x_2, y_2)\), the distance \(r\) between them is:\[ r = \sqrt{(x_2 - x_1)^2 + (y_2 - y_1)^2} \]
Knowing how to find this distance helps accurately determine the electric force in exercises and real-life scenarios.
Magnitude and Direction
When multiple forces act on a charge, like in the given exercise, it’s important to find both the magnitude and the direction of the resultant force. The magnitude tells us how strong the total force is. The direction shows us the line along which the force acts.
To find the magnitude of a resultant force from its components \((F_x, F_y)\), use the Pythagorean theorem:\[ F_{total} = \sqrt{F_x^2 + F_y^2} \]
This step gives the complete strength of the force. To determine the direction, use the inverse tangent function:\[ \theta = \arctan\left(\frac{F_y}{F_x}\right) \]
This angle \( \theta \) will show you exactly where the force is heading, revealing the precise geometry of interactions between charges in any system. Understanding magnitude and direction is vital for predicting the behaviour of charged particles.

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Most popular questions from this chapter

What is the best explanation for the observation that the electric charge on the stem became positive as the charged bee approached (before it landed)? (a) Because air is a good conductor, the positive charge on the bee's surface flowed through the air from bee to plant. (b) Because the earth is a reservoir of large amounts of charge, positive ions were drawn up the stem from the ground toward the charged bee. (c) The plant became electrically polarized as the charged bee approached. (d) Bees that had visited the plant earlier deposited a positive charge on the stem.

A point charge is at the origin. With this point charge as the source point, what is the unit vector \(\hat{r}\) in the direction of the field point (a) at \(x = 0, \space y = -\)1.35 m; (b) at \(x =\) 12.0 cm, \(y =\) 12.0 cm; (c) at \(x = -\)1.10 m, \(y =\) 2.60 m ? Express your results in terms of the unit vectors \(\hat{\imath}\) and \(\hat{\jmath}\).

Two very large horizontal sheets are 4.25 cm apart and carry equal but opposite uniform surface charge densities of magnitude \(\sigma\). You want to use these sheets to hold stationary in the region between them an oil droplet of mass 486 \(\mu\)g that carries an excess of five electrons. Assuming that the drop is in vacuum, (a) which way should the electric field between the plates point, and (b) what should \(\sigma\) be?

Point charges \(q_1 = -\)4.5 nC and \(q_2 = +\)4.5 nC are separated by 3.1 mm, forming an electric dipole. (a) Find the electric dipole moment (magnitude and direction). (b) The charges are in a uniform electric field whose direction makes an angle of 36.9\(^\circ\) with the line connecting the charges. What is the magnitude of this field if the torque exerted on the dipole has magnitude \(7.2 \times 10^{-9}\) N \(\cdot\) m ?

Two identical spheres are each attached to silk threads of length \(L =\) 0.500 m and hung from a common point (Fig. P21.62). Each sphere has mass \(m =\) 8.00 g. The radius of each sphere is very small compared to the distance between the spheres, so they may be treated as point charges. One sphere is given positive charge \(q_1\) , and the other a different positive charge \(q_2\) ; this causes the spheres to separate so that when the spheres are in equilibrium, each thread makes an angle \(\theta = 20.0^\circ\) with the vertical. (a) Draw a free-body diagram for each sphere when in equilibrium, and label all the forces that act on each sphere. (b) Determine the magnitude of the electrostatic force that acts on each sphere, and determine the tension in each thread. (c) Based on the given information, what can you say about the magnitudes of \(q_1\) and \(q_2\)? Explain. (d) A small wire is now connected between the spheres, allowing charge to be transferred from one sphere to the other until the two spheres have equal charges; the wire is then removed. Each thread now makes an angle of 30.0\(^\circ\) with the vertical. Determine the original charges. (\(Hint\): The total charge on the pair of spheres is conserved.)

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