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Magnetic Flux


Magnetic flux measures how many magnetic field lines pass through a surface. It is key to understanding electromagnetic induction.

  • Consider a constant magnetic field B⃗\vec{ B}passing through a flat area A⃗\vec{A}.
Image illustrating Magnetic Flux
  • The magnetic flux through the surface is given by the following equation, where θ\theta is the angle between the magnetic field and area vectors:
Φm=B⃗⋅A⃗=∣B∣⃗∣A∣⃗cos⁡(θ)\boxed{\Phi_m=\vec{B}\cdot\vec{A}=\vec{\left|B\right|}\vec{\left|A\right|}\cos(\theta)}
  • The SI unit for magnetic flux is the Weber. 1 Wb=1 Tm2\boxed{1~Wb=1~Tm^2}



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Example: Magnetic Flux


A box is oriented as shown in the diagram below. There is a uniform magnetic field of B=0.3 TB=0.3\ Tpointing parallel to the positive z-axis.

Image illustrating Example: Magnetic Flux

a) Find the magnetic flux across the surface ABDC.

b) Find the magnetic flux across the surface BDEF.

c) Find the total magnetic flux through the box.

Part a)


The surface ABDC has an area vector that points in the positive z-direction, which is the same direction as the magnetic field. Therefore, the dot product reduces to a simple multiplication.

Φm=BAcos⁡θΦm=(0.3 T)(5m×2m)cos⁡(0o)Φm=3.0 Wb\begin{aligned} \Phi_m&=BA\cos\theta \\ \Phi_m&=(0.3~T)(5m\times2m)\cos(0^o) \\ \Phi_m&= 3.0 ~Wb\\ \end{aligned}

Part b)


The surface BDEF has an area vector that points in the positive y-direction, which is perpendicular to the magnetic field. Therefore, the magnetic flux is zero (cos⁡90o=0\cos90^o=0).


Part c)


For all closed surfaces (such as this box!), the total magnetic flux passing through it is zero!


If we wanted to be more detailed, we could see that the flux through four of the surfaces is zero (the area vector is perpendicular to the field direction), and the flux passing through the top surface would be equal and opposite to our result from Part (a) (cos⁡180o=−1\cos180^o=-1). So the flux would be given as: +3 + 0 + 0 + 0 + 0 - 3 = 0 Wb.


Practice: Spinning Ring


A circular loop of wire of radius rr is mounted on a vertical shaft in a region of uniform magnetic field of strengthBB.


Initially, the magnetic field is perpendicular to the plane of the ring. At this moment, the ring is set to rotate about its vertical axis with an angular frequency of ω\omega.

Illustration for practice question: Magnetic Flux

a) Find an expression for the flux through the ring as a function of time.

b) How does your answer change if the field was initially parallel to the plane of the ring, instead of perpendicular?


Illustration for practice question: Magnetic Flux


Part a)

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Magnetic Flux (with calculus)


A bit more effort is required to find the magnetic flux in some scenarios.

  • The full equation for magnetic flux is given by the following equation:

Φm=∫B⃗⋅dA⃗\boxed{\Phi_m=\displaystyle \int\vec{{B}}\cdot d\vec{A}}

  • For example, this integral must be used if the magnetic field B⃗\vec B is not uniform, or if the surface A⃗\vec A is curved.


Practice: Magnetic Flux from a Non-Uniform Field


Consider a non-uniform magnetic field given by the expression B⃗(x,y)=10x2y3 T\vec B\left(x,y\right)=10x^2y^3~T. The field is perpendicular to the x-y plane.


a) If you place a 2cm-by-2cm square in this field, with the square centered on the origin of the coordinate system, what is the magnetic flux through the surface?

b) What if the square is moved 1-cm in the +y direction (that is, the square is now fully in the positive-y region, and its bottom edge is at y=0)?

Part a)

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