Four infinitely long parallel wires carrying equal current I are arranged in such a way that when looking at the cross section, they are at the corners of a square, as shown in the right figure below. Currents in A and D point out of the page, and into the page at Band C. What is the magnetic field at the center of the square? [Hint: set a 2-dimensional reference system with origin in P; Use the formula for the magnetic field of an infinite wire and the superposition principle to find vector B] • P a B (× a
Four infinitely long parallel wires carrying equal current I are arranged in such a way that when looking at the cross section, they are at the corners of a square, as shown in the right figure below. Currents in A and D point out of the page, and into the page at Band C. What is the magnetic field at the center of the square? [Hint: set a 2-dimensional reference system with origin in P; Use the formula for the magnetic field of an infinite wire and the superposition principle to find vector B] • P a B (× a
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![### Problem Statement
Four infinitely long parallel wires carrying equal current \( I \) are arranged in such a way that, when looking at the cross-section, they are at the corners of a square, as shown in the figure below. Currents in wires at points \( A \) and \( D \) point out of the page, and currents at \( B \) and \( C \) point into the page. What is the magnetic field at the center \( P \) of the square?
**Hint**: Set a 2-dimensional reference system with origin at \( P \). Use the formula for the magnetic field of an infinite wire and the superposition principle to find vector \( \mathbf{B} \).
### Diagram Explanation
The diagram depicts four points, labeled \( A \), \( B \), \( C \), and \( D \), located at the four corners of a square. Each side of the square is marked with length \( a \).
- Points \( A \) and \( D \) have currents directed out of the page, represented by dots within circles.
- Points \( B \) and \( C \) have currents directed into the page, represented by crosses within circles.
At the center of the square is point \( P \), which is where the magnetic field is to be calculated. Each wire contributes to the magnetic field at the center based on their direction and magnitude of the current.
### Approach
1. **Set up a coordinate plane**: Place the center \( P \) of the square at the origin.
2. **Calculate magnetic effect**: Use the Biot-Savart Law or Ampere's Law for each wire to calculate the magnetic field contribution.
3. **Apply the superposition principle**: Add the vector contributions of each wire to find the net magnetic field at the center \( P \).
This setup and calculation method will allow you to determine the overall magnetic field at point \( P \).](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F21383fc6-537b-4c15-bc94-620c670c55a7%2F75491a18-89ab-4196-9e9f-8885af718de2%2Fajijmil_processed.png&w=3840&q=75)
Transcribed Image Text:### Problem Statement
Four infinitely long parallel wires carrying equal current \( I \) are arranged in such a way that, when looking at the cross-section, they are at the corners of a square, as shown in the figure below. Currents in wires at points \( A \) and \( D \) point out of the page, and currents at \( B \) and \( C \) point into the page. What is the magnetic field at the center \( P \) of the square?
**Hint**: Set a 2-dimensional reference system with origin at \( P \). Use the formula for the magnetic field of an infinite wire and the superposition principle to find vector \( \mathbf{B} \).
### Diagram Explanation
The diagram depicts four points, labeled \( A \), \( B \), \( C \), and \( D \), located at the four corners of a square. Each side of the square is marked with length \( a \).
- Points \( A \) and \( D \) have currents directed out of the page, represented by dots within circles.
- Points \( B \) and \( C \) have currents directed into the page, represented by crosses within circles.
At the center of the square is point \( P \), which is where the magnetic field is to be calculated. Each wire contributes to the magnetic field at the center based on their direction and magnitude of the current.
### Approach
1. **Set up a coordinate plane**: Place the center \( P \) of the square at the origin.
2. **Calculate magnetic effect**: Use the Biot-Savart Law or Ampere's Law for each wire to calculate the magnetic field contribution.
3. **Apply the superposition principle**: Add the vector contributions of each wire to find the net magnetic field at the center \( P \).
This setup and calculation method will allow you to determine the overall magnetic field at point \( P \).
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