Question #74425

Two long, straight, parallel wires A and B, separated by a distance of 30 cm, carry currents IA = 10A and IB = 30A. The currents in both the wires flow in the same direction. Calculate the net magnetic field at the midpoint of the line joining the two wires and perpendicular to them
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Expert's answer

2018-03-12T16:47:07-0400

Answer on Question #74425 - Physics - Electromagnetism

Question:

Two long, straight, parallel wires A and B, separated by a distance of 30 cm30~\mathrm{cm} , carry currents IA = 10A and IB = 30A. The currents in both the wires flow in the same direction. Calculate the net magnetic field at the midpoint of the line joining the two wires and perpendicular to them

Solution:

1. At first we can find the magnetic field of one wire. Ampère's circuit law


μ0I=(B,dl)=2πRB,\mu_ {0} I = \oint (\vec {B}, \vec {d l}) = 2 \pi R B,


if we integrate the magnetic field along the circle with radius RR . Therefore the magnitude of magnetic field for one wire is


B=μ0I2πRB = \frac {\mu_ {0} I}{2 \pi R}


where μ01.2566×106(N/A2)\mu_0\approx 1.2566\times 10^{-6}(\mathrm{N / A^2}) -- magnetic constant in vacuum. The distance from the axis of the wire to the midpoint, for both wires is


R=d2R = \frac {d}{2}


where d=30(cm)=0.3(m)d = 30(\mathrm{cm}) = 0.3(\mathrm{m}) is the distance between wires A and B.

2. The vector of the net magnetic field Bnet\vec{B}_{net} will be the sum of the vectors BA\vec{B}_A and BB\vec{B}_B of parallel wires A and B. We can find directions of the vectors BA\vec{B}_A and BB\vec{B}_B with the help of "Right-hand rule". Therefore at the midpoint of the line joining the two wires, the vectors BA\vec{B}_A and BB\vec{B}_B will have the opposite direction, and the magnitude of the net magnetic field will be


Bnet=BBBA=μ0IB2πRμ0IA2πR=μ0(IBIA)πdB _ {n e t} = B _ {B} - B _ {A} = \frac {\mu_ {0} I _ {B}}{2 \pi R} - \frac {\mu_ {0} I _ {A}}{2 \pi R} = \frac {\mu_ {0} (I _ {B} - I _ {A})}{\pi d}Bnet1.2566×106×(3010)3.14×0.32.67×105(T)B _ {n e t} \approx \frac {1 . 2 5 6 6 \times 1 0 ^ {- 6} \times (3 0 - 1 0)}{3 . 1 4 \times 0 . 3} \approx 2. 6 7 \times 1 0 ^ {- 5} (T)


Fig. The magnetic field of one wire with the current IAI_A (green) and IBI_B (red); the net magnetic field (blue) at the midpoint of the line joining the two wires.

Answer:

The net magnetic field at the midpoint of the line joining the two wires: Bnet2.67×105(T)B_{net} \approx 2.67 \times 10^{-5}(T)

Comments:

1. we use standard SI units:

T—Tesla, m—metre, N—Newton, A -- Ampere

https://en.wikipedia.org/wiki/International_System_of_Units

2. Ampère's circuital law – for example:

https://en.wikipedia.org/wiki/Amp%C3%A8re%27s_circuital_law

(the table -- "Forms of the original circuital law written in SI units")

3. "Right-hand rule"– for example:

https://en.wikipedia.org/wiki/Right-hand_rule

4. the magnetic field of the wire is well-known classical problem. For example, the next:

http://farside.ph.utexas.edu/teaching/3021/lectures/node75.

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