Magnetic Flux Density
CSCA Magnetic Flux Density study guide organized around the publicly available CSCA syllabus. Practice Physics questions on aicsca.com.
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This study guide is organized around the publicly available CSCA syllabus for international undergraduate applicants.
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International students preparing for CSCA Math, Physics, Chemistry, or Chinese exams.
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Related formulas, concepts, and glossary terms
Physics Formula & Concept Reference
- Definition of Magnetic Induction (Magnetic Flux Density)
- Magnetic Field on the Axis of a Current - Carrying Circular Loop
- Ampere's Circuital Law (for Magnetic Fields)
- Magnetic Field of an Infinite Straight Wire
- Magnetic Field of an Infinite Straight Current - Carrying Wire
- Biot - Savart Law (Magnetic Field from a Current Element)
- Biot - Savart Law
- Definition of Magnetic Induction Intensity
Physics Exam Glossary
Tutorial Content
Topic: Electromagnetism > Magnetic Field > Magnetic Flux Density
1. Core Concept: Magnetic Flux Density ($B$)
**Magnetic Flux Density** describes the strength and direction of a magnetic field (Vector).
* **Physical Meaning**: Analogous to Electric Field Strength $E$, it describes the **force nature** of the magnetic field.
* **Direction Rule**: The direction the **North Pole of a compass** points when at rest.
* **Unit**: **Tesla (T)**.
* $1 T = 1 \frac{N}{A \cdot m} = 1 \frac{Wb}{m^2}$.
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2. Definition vs. Determination Formula
For the CSCA exam, distinguish clearly between "How to define B" and "What determines B".
(1) Definition Formula
$$B = \frac{F}{IL}$$
* **Condition**: The wire must be placed **perpendicular** to the magnetic field.
* **Understanding**:
* This is a **Ratio Definition**.
* The magnitude of $B$ is determined by the field itself, **independent of $I, L$ or $F$**.
* If the wire is parallel to the field, $F=0$, but $B \neq 0$ at that point.
(2) Determination Formula
For magnetic fields produced by specific current geometries:
| Source | Formula (Vacuum $\mu_0$) | Notes |
| :--- | :--- | :--- |
| **Long Straight Wire** | $$B = \frac{\mu_0 I}{2\pi r}$$ | $r$: Perpendicular distance.<br>Closer to wire $\to$ Stronger B. |
| **Solenoid** | $$B = \mu_0 n I$$ | $n = N/L$: Turns per unit length.<br>Interior field is approx. **Uniform**. |
| **Center of Loop** | $$B = \frac{\mu_0 I}{2R}$$ | $R$: Radius of loop. |
**Constant**: Permeability of vacuum $\mu_0 = 4\pi \times 10^{-7} T\cdot m/A$.
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3. Magnetic Field Lines
Imaginary curves to visualize the magnetic field.

**Three Key Features**:
1. **Closed Loops**: No start or end points.
* **External**: N Pole $\to$ S Pole.
* **Internal**: S Pole $\to$ N Pole (Major difference from Electric Field Lines).
2. **No Intersection**: The field direction at any point is unique.
3. **Density = Strength**: Denser lines mean larger $B$.
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4. Superposition of Magnetic Fields
$B$ is a **Vector**. If multiple fields exist, use **Vector Addition**.

**Steps**:
1. **Direction**: Use **Ampere's Right-Hand Grip Rule** to draw the direction of each $B$ component.
2. **Magnitude**: Calculate each magnitude using formulas.
3. **Resultant**: Use geometry (Pythagoras, components) to find the total vector.
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5. Typical Examples
**Example 1: Applying Definition**
**Problem**: A $0.2m$ wire is perpendicular to a field. Current $I=2A$, Force $F=0.4N$. Find:
(1) $B$;
(2) If $I$ becomes $4A$, what are the Force and $B$?
**Solution**:
(1) $$B = \frac{F}{IL} = \frac{0.4}{2 \times 0.2} = 1 T$$
(2) $B$ is a field property, **unchanged** at $1T$.
$$F' = B I' L = 1 \times 4 \times 0.2 = 0.8 N$$
**Example 2: Superposition (Parallel Wires)**
**Problem**: Two parallel long wires, distance $2d$, carry opposite currents $I$. Find $B$ at the midpoint $O$.
**Solution**:
1. **Direction**:
* Left Wire (Up current): $B_1$ at $O$ is **Into Page**.
* Right Wire (Down current): $B_2$ at $O$ is **Into Page**.
2. **Magnitude**:
$$B_1 = B_2 = \frac{\mu_0 I}{2\pi d}$$
3. **Total**:
$$B_{total} = B_1 + B_2 = \frac{\mu_0 I}{\pi d}$$ (Direction: Into Page)
**Example 3: 3D Superposition**
**Problem**: Two perpendicular non-touching wires. Find total B direction at equidistant points.
**Solution**: Draw a 3D or top-down view, determine component vectors using Right-Hand Rule, and add them.