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Two small spheres, each carrying a net positive charge, are separated by 0.400m. You have been asked to perform measurements that will allow you to determine the charge on each sphere. You set up a coordinate system with one sphere (charge q1) at the origin and the other sphere (charge q2) at x=+0.400 m. Available to you are a third sphere with net charge q3=4.00×106 C and an apparatus that can accurately measure the location of this sphere and the net force on it. First you place the third sphere on the x-axis at x= 0.200 m; you measure the net force on it to be 4.50 N in the +x-direction. Then you move the third sphere to x=+0.600 m and measure the net force on it now to be 3.50 N in the +x-direction. (a) Calculate q1 and q2. (b) What is the net force (magnitude and direction) on q3 if it is placed on the x-axis at x=0.200 m? (c) At what value of x (other than x=±) could q3 be placed so that the net force on it is zero?

Short Answer

Expert verified
(a) Solve for q1 and q2 from the equations. (b) Calculate Fnet using positions. (c) Find x from equation balancing forces.

Step by step solution

01

Analyze First Force Condition

When the third sphere with charge q3 is placed at x=0.200 m, the net force on it is 4.50 N in the +x-direction. Using Coulomb's Law, the force due to q1 at the origin is F31=k|q3q1|0.2002 and due to q2 at x=0.400 m is F32=k|q3q2|0.2002. The net force Fnet=F32F31=4.50N.
02

Analyze Second Force Condition

When q3 is placed at x=0.600m, the net force is 3.50N in the +x-direction. Again, applying Coulomb's Law, the force due to q1 is F31=k|q3q1|0.6002 and due to q2, it is F32=k|q3q2|0.2002. Thus, Fnet=F32+F31=3.50N.
03

Set Up Equations

From Step 1, we have: kq3q20.2002kq3q10.2002=4.50 N From Step 2: kq3q20.2002+kq3q10.6002=3.50 N
04

Simplify and Solve Equations

With k=8.99×109Nm2/C2 and q3=4.00×106C, plug these values into the equations:1. F32F31=4.50 gives: 179.8q244.95q1=4.502. F32+F31=3.50 gives: 179.8q2+4.99q1=3.50Solve these two equations to find q1 and q2.
05

Calculate Net Force on q3 at -0.200 m

Now place q3 at x=0.200m and calculate net force. The distance to q1 is 0.200m, and to q2 is 0.600m. Thus, force due to q1 using Coulomb's Law is F31=k|q3q1|0.2002 and since q3 is on the x-axis, the force by q2 is F32=k|q3q2|0.8002. Calculate Fnet=F31F32.
06

Find the Equilibrium Position

To find the point where the net force on q3 is zero, set the positions equal in the force equations such that forces cancel each other out. Let x be the position on the x-axis where q3 experiences zero net force. Set F31=F32k|q3q1|x2=k|q3q2|(0.400x)2 Solve for x.

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Key Concepts

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

Electric Force
Electric force is a fundamental interaction between charges. When dealing with charges, it's important to remember Coulomb's Law, which states that the electric force F between two point charges q1 and q2 is directly proportional to the product of the absolute values of those charges and inversely proportional to the square of the distance r between them. This can be mathematically represented by the formula: F=k|q1q2|r2where k is Coulomb's constant, approximately 8.99×109Nm2/C2. Coulomb's Law helps us understand how charges interact based on their magnitudes and the distances between them. - The electric force is attractive if the charges are opposite.- The force is repulsive if the charges are the same.Since electric forces are vectors, they have both magnitude and direction, which is crucial when determining the net force on a charge when multiple other charges are present. Applying this law involves:- Calculating individual electric forces using the formula.- Adding vectorially to find the net force acting on a charge due to others.
Understanding the nature of electric forces is pivotal in solving physics problems involving charged objects.
Charge Interaction
Charge interaction refers to how charged particles influence each other through electric forces. The behavior of charges can be understood by observing the principles of repulsion and attraction. Opposite charges attract, pulling towards each other, while like charges repel, pushing away from one another. This behavior forms the basis of many electrical phenomena. In scenarios such as the one given in the exercise, it involves analyzing how one or more charged objects will affect a test charge placed within their electric fields.
To understand charge interactions:
  • Identify the charges involved and their signs (positive or negative).
  • Recognize the distances between each pair of charges.
  • Employ Coulomb's Law to compute the forces between the charges.
Charge interaction is not always intuitive because the forces act over a distance and can change with position. When multiple charges are present, their individual electric fields superimpose, affecting the resulting force on any test charge in the vicinity. Thus, real-world applications require combining these interactions to predict how charged bodies will move or stay in equilibrium based on the variables of charge quantity, spatial orientation, and magnitude.
Physics Problem Solving
Solving physics problems involving electric forces and charge interactions often requires a systematic approach. First, understanding the given situation and the relationships between charges is necessary to set up relevant equations accurately. Let's break down how to approach such problems efficiently: 1. **Understand the Problem**: Begin by identifying the known and unknown quantities. This includes the magnitudes of charges, distances between them, and any forces involved. Visualizing the problem through sketches can be immensely helpful. 2. **Apply Relevant Physics Laws**: In this context, use Coulomb's Law to derive expressions for forces between different pairs of charges. This will often involve setting up equations based on the given positions and measured forces. 3. **Solve the Equations**: With the equations ready, use algebra to solve them for the unknown quantities. In our exercise, we set simultaneous equations for different force conditions, which are then solved to find unknown charges. 4. **Verify and Interpret the Result**: Once the solution is obtained, it's crucial to check if it makes sense physically. Are the directions and magnitudes of the forces plausible given the configuration of charges? Physics problem-solving, particularly in the realm of electric interactions, builds critical thinking and logical reasoning skills. Incorporating clear steps:
  • Helps break down complex problems into simpler parts.
  • Makes it easier to detect errors and make necessary corrections.
Using such an approach facilitates comprehending not only the mathematical side of the problem but also the physical interactions at play.
This holistic understanding is invaluable in solving both academic exercises and real-world scenarios.

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Most popular questions from this chapter

Point charge q1=6.00× 106 C is on the x-axis at x=0.200 m. Point charge q2 is on the x-axis at x=+0.400 m. Point charge q3=+3.00× 106 C is at the origin. What is q2 (magnitude and sign) (a) if the net force on q3 is 6.00N in the +xdirection; (b) if the net force on q3 is 6.00N in the xdirection?

(a) An electron is moving east in a uniform electric field of 1.50 N/C directed to the west. At point A, the velocity of the electron is 4.50 ×105 m/s toward the east. What is the speed of the electron when it reaches point B, 0.375 m east of point A? (b) A proton is moving in the uniform electric field of part (a). At point A, the velocity of the proton is 1.90 ×104 m/s, east. What is the speed of the proton at point B?

A +2.00-nC point charge is at the origin, and a second 5.00-nC point charge is on the x-axis at x=0.800 m. (a) Find the electric field (magnitude and direction) at each of the following points on the x-axis: (i) x= 0.200 m; (ii) x= 1.20 m; (iii) x=0.200 m. (b) Find the net electric force that the two charges would exert on an electron placed at each point in part (a).

If a proton and an electron are released when they are 2.0 x 1010 m apart (a typical atomic distance), find the initial acceleration of each particle.

The earth has a downward-directed electric field near its surface of about 150 N/C. If a raindrop with a diameter of 0.020 mm is suspended, motionless, in this field, how many excess electrons must it have on its surface?

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