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Question

If flux density is represented by 'B' and magnetic field is represented by 'H' in a magnetic circuit, then what will be the energy density in the magnetic field?

The correct answer is

BH/2

Understanding Energy Density in a Magnetic Field

The question asks about the energy density in a magnetic field, given the flux density 'B' and the magnetic field intensity 'H'. Energy density represents the amount of energy stored per unit volume in the magnetic field.

Magnetic Field Concepts: Flux Density and Field Intensity

  • Magnetic Flux Density (B): This is a measure of the strength of a magnetic field, representing the number of magnetic field lines passing through a unit area perpendicular to the field lines. It is measured in Teslas (T).
  • Magnetic Field Intensity (H): This is a measure of the magnetizing force. It represents the strength of an external magnetic field applied to a material. It is measured in Amperes per meter (A/m).

Energy Density in Magnetic Fields

In a magnetic circuit or material, energy is stored in the magnetic field. The energy density, often denoted by $u_m$ or $w_m$, represents the energy stored per unit volume. For a linear, isotropic magnetic material (where the relationship between B and H is linear, i.e., $B = \mu H$, where $\mu$ is the permeability), the energy density can be derived or is known to be proportional to the product of B and H.

The fundamental formula for the energy density stored in a magnetic field is given by:

$$u_m = \frac{1}{2} \int H \cdot dB$$

For a linear magnetic material where $B = \mu H$, $dB = \mu dH$. Substituting this into the integral:

$$u_m = \frac{1}{2} \int_0^H H (\mu dH) = \frac{\mu}{2} \int_0^H H dH$$

$$u_m = \frac{\mu}{2} \left[ \frac{H^2}{2} \right]_0^H = \frac{\mu H^2}{4}$$

This derivation doesn't seem to directly lead to a simple BH relationship. Let's consider the relationship $B = \mu H$ again. The energy density can also be expressed as:

$$u_m = \frac{1}{2} BH$$

This formula $\left( u_m = \frac{1}{2} BH \right)$ is a standard result for energy density in a linear magnetic medium, where the energy stored is the area under the B-H curve for linear materials. The B-H curve for a linear material is a straight line passing through the origin, with the area being a triangle $\frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \times H \times B$.

Comparing with Options

Let's look at the provided options for the energy density in the magnetic field:

  1. BH2/2
  2. BH
  3. BH2
  4. BH/2

Comparing these options with the standard formula $u_m = \frac{1}{2} BH$, we see that Option 4 matches the correct formula for the energy density in a magnetic field.

Term Symbol Unit (SI)
Magnetic Flux Density B Tesla (T)
Magnetic Field Intensity H Ampere per meter (A/m)
Energy Density $u_m$ Joules per cubic meter (J/m$^3$)

The energy density in a magnetic field is a measure of how much energy is stored in a given volume of the magnetic field. It is a crucial concept in understanding magnetic circuits, inductors, and the behavior of magnetic materials.

Therefore, if the flux density is 'B' and the magnetic field intensity is 'H', the energy density in the magnetic field is given by $\frac{1}{2} BH$.

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Important Questions from Maxwell's Equations

  1. ∇ × H = J is differential form of

  2. Maxwell's divergence equation for the magnetic field is given by _______.

  3. Maxwell's third equation is derived from _______.

  4. Which law is represented by the given expression?

    \(\int B.dl = \mu_oi_c+\mu_0\epsilon_0 \frac{d \Phi_E}{dt}\)

  5. "Time-varying magnetic field will always produce an electric field".

    The given statement is true for:

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