The relationship between **permeability (μ)** and **magnetic flux density (B)** is fundamental to understanding how magnetic fields interact with materials.
1. **Magnetic Flux Density (B)**: This represents the strength and direction of the magnetic field in a given area. It is often called the **magnetic field** and is measured in **Tesla (T)**.
2. **Permeability (μ)**: This is a material property that indicates how easily a magnetic field can pass through a material. It is a measure of how well a material can become magnetized when exposed to a magnetic field. Permeability is typically measured in **Henries per meter (H/m)**.
The relationship between **B** (magnetic flux density) and **H** (magnetic field intensity) in a material is given by:
\[
B = \mu H
\]
Where:
- \(B\) is the **magnetic flux density** (in Tesla),
- \(\mu\) is the **permeability** of the material (in Henries per meter, H/m),
- \(H\) is the **magnetic field intensity** (in Ampere-turns per meter, A/m).
In simpler terms, permeability (\(\mu\)) tells us how easily a material allows the magnetic field to pass through, and **flux density (B)** tells us how much magnetic field is present in that material.
- For **vacuum or air**, the permeability is constant and denoted as \(\mu_0\) (vacuum permeability), and the relationship is straightforward.
- In **materials** like iron, the permeability (\(\mu\)) is much higher, allowing more magnetic flux density (B) for the same magnetic field intensity (H).
So, if the permeability of a material increases, the magnetic flux density (B) will also increase for the same applied magnetic field intensity (H).