Calculating Magnetic Flux: Plane with Rotated Wire and Current of 2.5 A

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SUMMARY

The magnetic flux crossing the portion of the plane defined by 0.01 m < r < 0.05 m and 0 m < z < 2 m, with a current of 2.5 A flowing along the z-axis, is calculated to be 0.00000785 Wb. The magnetic field around a long wire is given by B(r) = (μ0 I)/(2π r), where μ0 is the permeability constant. The area of the circular portion of the plane is determined using A = πr^2, resulting in an area of 0.00785 m². The angle between the normal to the plane and the magnetic field is π/4, leading to the final flux calculation using Φ = BAcos(θ).

PREREQUISITES
  • Understanding of magnetic flux and its calculation
  • Familiarity with the Biot-Savart Law and magnetic fields around current-carrying wires
  • Knowledge of calculus for integration and area calculations
  • Basic understanding of trigonometry, particularly cosine functions
NEXT STEPS
  • Study the Biot-Savart Law for detailed understanding of magnetic fields
  • Learn about the permeability constant (μ0) and its significance in electromagnetism
  • Explore advanced applications of magnetic flux in electromagnetic theory
  • Investigate the effects of varying current on magnetic field strength and flux
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Physics students, electrical engineers, and professionals involved in electromagnetism and magnetic field analysis will benefit from this discussion.

hd28cw
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Find the magnetic flux crossing the portion of the plane
theta = x/4 defined by 0.01 m < r <0.05 m and 0 m < z < 2 m. A current of 2.50 A is flowing along z-axis along a very long wire.

in drawing the picture i know that there is a long thin wire with a current of 2.5 amps flowing positively on the z-axis and the plane is lying rotated at an angle of pi/4 with the magnetic field flowing in a counter clockwise direction.

How do I go about finding the magnetic flux.
Please help.
 
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hd28cw said:
Find the magnetic flux crossing the portion of the plane
theta = x/4 defined by 0.01 m < r <0.05 m and 0 m < z < 2 m.
Should that be theta=pi/4?


[tex]\Phi_B=\int_P \vec B \cdot d\vec a[/tex]

Since the plane lies parallel with the z-axis, its normal points in the same direction as the magnetic field everywhere in the plane, so you can drop the dot in the integrand

[tex]\Phi_B=\int_P B da[/tex]

Recall that the magnitude of the magnetic field of a long wire is:

[tex]B(r)=\frac{\mu_0 I}{2\pi r}[/tex]
where r is the distance from the wire.
 


To calculate the magnetic flux, we can use the formula Φ = BAcosθ, where Φ is the magnetic flux, B is the magnetic field, A is the area, and θ is the angle between the normal to the area and the magnetic field. In this case, we have a wire with a current of 2.5 A flowing along the z-axis, which creates a magnetic field around it. The plane is rotated at an angle of π/4, so the angle between the normal to the plane and the magnetic field is also π/4.

First, we need to find the magnetic field at the given point on the plane. Using the right-hand rule, we can determine that the direction of the magnetic field is out of the page. The magnitude of the magnetic field can be calculated using the formula B = μ0I/2πr, where μ0 is the permeability constant, I is the current, and r is the distance from the wire. In this case, r = 0.05 m. Plugging in the values, we get B = (4π×10^-7 T⋅m/A)(2.5 A)/(2π×0.05 m) = 0.001 T.

Next, we need to calculate the area of the portion of the plane defined by the given values of r and z. Since the plane is a circle, the area can be calculated using the formula A = πr^2. In this case, r = 0.05 m, so A = π(0.05 m)^2 = 0.00785 m^2.

Finally, we can plug in the values into the formula Φ = BAcosθ. Since θ = π/4, we get Φ = (0.001 T)(0.00785 m^2)cos(π/4) = 0.00000785 Wb. Therefore, the magnetic flux crossing the portion of the plane is 0.00000785 Wb.
 

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