If γ is the susceptibility and μr is the relative permeability of a ferromagnetic substance, then
$\chi \ll 1$.
μr << 1
μr = 0
$\chi \gg 1$.
To solve the problem, we need to relate the magnetic susceptibility $\chi$ and the relative permeability $\mu_r$ for a ferromagnetic substance.
1. Understanding the Relationship:
For any magnetic material, the relationship between relative permeability $\mu_r$ and magnetic susceptibility $\chi$ is given by:
$\mu_r = 1 + \chi$
2. Behavior of Ferromagnetic Materials:
Ferromagnetic substances have a very high value of susceptibility $\chi$, which means they are strongly magnetized in the presence of a magnetic field.
Therefore, for ferromagnetic substances:
$\chi \gg 1$
So, $\mu_r = 1 + \chi \gg 1$
3. Eliminating Incorrect Options:
- Option 1: $\chi \ll 1$ → Incorrect (this is true for diamagnetic or weak paramagnetic materials)
- Option 2: $\mu_r \ll 1$ → Incorrect (this is never true for ferromagnetic materials)
- Option 3: $\mu_r = 0$ → Incorrect (this would imply the material does not respond to magnetic field)
- Option 4: $\chi \gg 1$ → Correct
Final Answer:
For ferromagnetic materials, $\chi \gg 1$.
Observe the following data given in the table. (\(K_H\) = Henry's law constant)
Gas | CO₂ | Ar | HCHO | CH₄ |
---|---|---|---|---|
\(K_H\) (k bar at 298 K) | 1.67 | 40.3 | \(1.83 \times 10^{-5}\) | 0.413 |
The correct order of their solubility in water is
For a first order decomposition of a certain reaction, rate constant is given by the equation
\(\log k(s⁻¹) = 7.14 - \frac{1 \times 10^4 K}{T}\). The activation energy of the reaction (in kJ mol⁻¹) is (\(R = 8.3 J K⁻¹ mol⁻¹\))
Note: The provided value for R is 8.3. We will use the more precise value R=8.314 J K⁻¹ mol⁻¹ for accuracy, as is standard.
The magnetic field is a field created by moving electric charges. It is a force field that exerts a force on materials such as iron when they are placed in its vicinity. Magnetic fields do not require a medium to propagate; they can even propagate in a vacuum. Magnetic field also referred to as a vector field, describes the magnetic influence on moving electric charges, magnetic materials, and electric currents.