Q.What are the dimensions of χ, the magnetic susceptibility? Consider an H-atom. Guess an expression for χ, upto a constant by constructing a quantity of dimensions of χ, out of parameters of the atom: e, m, v, R and μ0. Here, m is the electronic mass, v is electronic velocity, R is Bohr radius. Estimate the number so obtained and compare with the value of χ∼10−5 for many solid materials.
🔒You're viewing a preview — the full solution, concept, methods & PYQ mapping are locked.
🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Magnetic Materials Magnetization
From a Paperclip to a Magnet: The Intuition
You already know that a magnet can pick up iron nails. But what is actually happening inside that nail when it gets near the magnet? And why does a plastic comb, rubbed on hair, pick up tiny bits of paper — but never iron filings?
The answer lies in magnetization — the process by which a material becomes magnetic.
Think of a piece of iron as a chaotic crowd of tiny compass needles. Each needle is an atomic magnetic moment (a tiny magnet, arising from the spin of electrons). In unmagnetized iron, these needles point in random directions. Their magnetic effects cancel out, so the iron as a whole shows no net magnetism.
Now bring a strong magnet close. Its magnetic field acts like a command: "Line up!" The tiny compass needles inside the iron start rotating, aligning themselves with the external field. The more they align, the stronger the iron's own magnetic field becomes. This alignment is magnetization.
Magnetization is not the same as inducing a current. It is a purely magnetic reorientation of atomic dipoles inside a material.
The Precise Definition
Magnetization (M) is the net magnetic dipole moment per unit volume of a material. It tells you how strongly a material is magnetized — how many tiny atomic magnets are aligned, and in which direction.
If a material has N atoms per unit volume, each with an average magnetic moment μavg, then:
M=Nμavg
The SI unit of M is amperes per metre (A/m). Why? Because a magnetic dipole moment has units of A·m², and dividing by volume (m³) gives A/m.
M=volumetotal magnetic dipole moment
How Magnetization Connects to the Magnetic Field
When a material gets magnetized, it produces its own magnetic field. The total magnetic field B inside the material is the sum of:
- The external applied field H (caused by free currents, like the current in a solenoid)
- The material's response — the magnetization M
The fundamental relation is:
B=μ0(H+M)
where μ0=4π×10−7T⋅m/A is the permeability of free space.
Do not confuse H (magnetic field intensity, or "magnetizing field") with B (magnetic flux density). H is what you apply; M is what the material does; B is the total field you measure.
The Three Kinds of Magnetic Materials
Not all materials respond the same way to an external field. The magnetization M is proportional to H for most materials (at least for small fields):
M=χmH
where χm is the magnetic susceptibility — a dimensionless number that tells you how easily a material magnetizes.
| Material Type | χm | Behaviour | Example |
|---|---|---|---|
| Diamagnetic | Small and negative (≈−10−5) | Weakly repelled by a magnet; M opposes H | Water, copper, bismuth |
| Paramagnetic | Small and positive (≈10−5 to 10−3) | Weakly attracted; M aligns with H | Aluminium, oxygen gas |
| Ferromagnetic | Large and positive (≫1) | Strongly attracted; M can be huge and persists even after H is removed | Iron, nickel, cobalt |
Why this formula?
Magnetic Materials & Magnetization: Why the Key Formulas Hold
Let's build this from the ground up — starting with what magnetization physically means, then deriving the formulas step by step.
1. What is Magnetization (M)?
Magnetization is the net magnetic dipole moment per unit volume of a material.
- Inside a material, atoms act like tiny magnetic dipoles (due to electron spin and orbital motion).
- Without an external field, these dipoles point randomly → net M=0.
- When an external field H is applied, dipoles align partially → net M=0.
Definition:
M=volumenet magnetic dipole moment
Units: A/m (same as H).
2. The Fundamental Relation: B=μ0(H+M)
This is the master equation linking the three magnetic fields:
- B = magnetic flux density (the total field inside the material)
- H = applied magnetic field (due to free currents)
- M = magnetization (response of the material)
- μ0 = permeability of free space (4π×10−7 H/m)
Why this form?
Step 1: In vacuum, there is no material, so M=0. Then:
B=μ0H
Step 2: Inside a material, the dipoles themselves produce an additional field. The total B is the sum of:
- The field due to free currents (μ0H)
- The field due to bound currents (from aligned dipoles), which is μ0M
Hence:
B=μ0H+μ0M=μ0(H+M)
Key insight: M is not an independent field — it's the material's response to H.
3. Magnetic Susceptibility (χm) and Permeability (μ)
For linear, isotropic, homogeneous materials (most common in exams), magnetization is proportional to the applied field:
M=χmH
- χm = magnetic susceptibility (dimensionless)
- χm>0 for paramagnetic materials
- χm<0 for diamagnetic materials
- χm≫1 for ferromagnetic materials (but not linear!)
Derivation of relative permeability μr:
Substitute M=χmH into the master equation:
B=μ0(H+χmH)=μ0(1+χm)H
Define:
μr=1+χm(relative permeability)
μ=μ0μr(absolute permeability)
Thus:
B=μH
Why this matters: It shows that the material simply scales the applied field by a factor μr.
4. Why χm Has Different Signs (Physical Reasoning)
| Material Type | χm | Why? |
|---|---|---|
| Diamagnetic | χm<0 (small, ~10−5) | Applied field induces opposing dipole moments (Lenz's law at atomic level). M opposes H. |
| Paramagnetic | χm>0 (small, ~10−3) | Permanent atomic dipoles align partially with H. Thermal agitation fights alignment. |
Dimensions of χ. Since M=χH and both M and H are measured in A/m, the susceptibility χ is dimensionless.
Building χ from atomic parameters. Seek χ∼μ0aebmcvdRf that is dimensionless. Using [μ0]=MLT−2I−2, [e]=IT, [m]=M, [v]=LT−1, [R]=L and demanding all four dimensions cancel gives b=2a, c=−a, d=0, f=−a. The velocity power is zero, so v drops out and
χ∼mRμ0e2.
Estimate (Bohr atom): with μ0=4π×10−7, e=1.6×10−19C, m=9.1×10−31kg, R=5.3×10−11m, …
χ is dimensionless. The only dimensionless combination of {e,m,v,R,μ0} is χ∼μ0e2/(mR) (the velocity v drops out); numerically ≈6.7×10−4∼10−4, about an order of magnitude larger than the observed ∼10−5.
Dimensions of χ
Susceptibility is defined by M=χH. Magnetisation and magnetising field are both in A/m, so their ratio is a pure number:
[χ]=[H][M]=A⋅m−1A⋅m−1=1(dimensionless).
Constructing χ from atomic parameters
Look for χ∼μ0aebmcvdRf. In terms of M,L,T,I:
[μ0]=MLT−2I−2, [e]=IT, [m]=M, [v]=LT−1, [R]=L.
Requiring the product to be dimensionless gives
M:I:T:L:a+c=0−2a+b=0−2a+b−d=0a+d+f=0
From the I-equation b=2a; substituting into the T-equation gives d=0; then c=−a and f=−a. The combination is therefore (mRμ0e2)a, and the fundamental dimensionless quantity is
χ∼mRμ0e2.
The velocity power came out d=0: v drops out entirely. The estimate depends only on the orbit size R and the charge-to-mass ratio, not on how fast the electron moves.
Dimension check: (M)(L)(MLT−2I−2)(I2T2)=1.
Numerical estimate
For the hydrogen atom (Bohr radius R=a0):
mRμ0e2=(9.1×10−31)(5.3×10−11)(4π×10−7)(1.6×10−19)2.
- Numerator: 4π×10−7×2.56×10−38≈3.22×10−44.
- Denominator: 9.1×10−31×5.3×10−11≈4.82×10−41. …
Method: Dimensional Analysis to Guess an Unknown Physical Quantity from a Set of Parameters
Use this whenever you're asked to "construct" or "estimate" a quantity (up to a constant) from a given list of physical parameters, without deriving it from first principles.
Steps
Step 1: Find the target quantity's own dimensions first
Before guessing a formula, work out the dimensions of the quantity you're building directly from its definition. Here, susceptibility is defined by M=χH; since magnetisation M and magnetising field H are both measured in the same unit (A/m), their ratio χ is dimensionless:
[χ]=[H][M]=1.
Knowing the target dimension in advance tells you exactly what condition the guessed combination must satisfy.
Step 2: Propose a general power-law combination of the given parameters
Write the unknown quantity as a product of the given parameters, each raised to an unknown power:
χ∼μ0aebmcvdRf.
Step 3: Express every parameter's dimensions in the base set M,L,T,I
Look up (or derive from a known formula) the dimensions of each quantity — e.g. [μ0]=MLT−2I−2, [e]=IT, [m]=M, [v]=LT−1, [R]=L — and substitute into Step 2's combination.
Step 4: Set up and solve the simultaneous equations
Collect the total power of each base dimension (M, L, T, I) in the combined expression, and set each equal to the target dimension's corresponding power found in Step 1 (all zero here, since χ is dimensionless). This gives one linear equation per base dimension; solve them together for the exponents a,b,c,d,f. …
- GUJCET 2026Set x1 markMCQQ.A closely wound solenoid of 800 turns and area of cross section 2.5×10−4 m2 can carry a current of 3.0 A. The magnetic moment associated with it is ______. (A) 60 JT−1 (B) 0.60 JT−1 (C) 6 JT−1 (D) 0.06 JT−1
›Reveal solutionSolution
m=NIA=0.60 J T−1.
Magnetic moment of a solenoid: …
- GUJCET 2024Set 131 markMCQQ.AmVs is the unit of which physical quantity? (A) χm (B) μ0 (C) χc (D) ε0
›Reveal solutionSolution
A⋅mV⋅s equals AT⋅m, which is the SI unit of the permeability of free space μ0 (H/m).
Concept. μ0 has units of henry per metre; 1H=1V⋅s/A, so μ0 is measured in A⋅mV⋅s.
Steps. …
- GUJCET 2024Set 131 markMCQQ.A solenoid has a core of a material with relative permeability 400. The windings of the solenoid are insulated from the core and carry a current of 2 A. If the number of turns is 1000 per meter then the value of magnetic intensity will be ________. (A) 8×10−5 Am−1 (B) 2×103 Am−1 (C) 2×10−3 Am−1 (D) 8×105 Am−1
›Reveal solutionSolution
H=nI — it depends only on the current and turns per metre, not on the core.
Concept. Magnetic intensity (magnetising field) in a solenoid is H=nI, independent of the core material's permeability. …
- GUJCET 2023Set 091 markMCQQ.A solenoid of length 0.5 m has a radius of 1 cm and is made up of 250 turns. It carries a current of 5 A. What is the magnitude of the magnetic field inside the solenoid? (A) 3.14×10−3 T (B) 6.28×10−3 T (C) 62.8×10−3 T (D) Zero
›Reveal solutionSolution
Field inside a long solenoid is B=μ0nI; the radius is irrelevant.
Concept: For a solenoid, B=μ0nI where n is turns per unit length.
n=LN=0.5250=500 m−1. …
- GUJCET 2023Set 091 markMCQQ.A solenoid has a core of a material with relative permeability 400. The windings of solenoid are insulated from the core and carry a current of 2 A. If the number of turns is 1000 per metre, the magnetic field B inside the solenoid is ______ T. (A) 1.5 (B) 1.0 (C) 1.8 (D) 2.0
›Reveal solutionSolution
A magnetic core multiplies the solenoid field by relative permeability: B=μ0μrnI.
Concept: With a core, B=μ0μrnI. …
- GUJCET 2022Set 171 markMCQQ.A solenoid of length 0.25 m has a radius of 1 cm and is made up of 500 turns. It carries a current of 2.5 A. What is the magnitude of the magnetic field inside the solenoid? (μ0=4π×10−7 SI) (A) 6.28×10−3 T (B) 6.28×10−2 T (C) 6.28×10−4 T (D) 6.28×10−1 T
›Reveal solutionSolution
n=N/l=2000 turns/m, so B=μ0nI=6.28×10−3 T (radius irrelevant).
Concept: n=0.25500=2000 turns/m. …
- GUJCET 2022Set 171 markMCQQ.A solenoid has a core of a material with relative permeability 400. The windings of the solenoid are insulated from the core and carry a current of 1 A. If the number of turns is 1000 per metre, find magnetic field (B) ________ T. (μ0=4π×10−7 SI) (A) 1.6π×10+2 (B) 16π×102 (C) 16π×10−2 (D) 0.16π×10−2
›Reveal solutionSolution
With a magnetic core, B=μ0μrnI=16π×10−2 T. …
- GUJCET 2021Set 151 markMCQQ.A solenoid of length 0.5 m has a radius of 1 cm and is made up of 1000 turns. It carries a current of 10A. What is the magnitude of the magnetic field inside the solenoid? (A) 6.28×10−3 T (B) 2.51×10−2 T (C) 1.71×10−2 T (D) 7.23×10−3 T
›Reveal solutionSolution
B=μ0nI; radius is irrelevant for a long solenoid.
Concept: …
- GUJCET 2020Set 071 markMCQQ.The relative permeability in a core of a solenoid is 400. The windings of a solenoid are insulated from the core and carry a current of 2A. If the number of turns is 1000 per meter. Then magnetic Intensity inside the core of solenoid is ______ A/m. (A) 2.5×103 (B) 2×103 (C) 2.5×10−3 (D) 2×10−3
›Reveal solutionSolution
H=nI, independent of the core; H=1000×2=2×103 A/m. …
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.A toroid wound with 100 turns/m of wire carries a current of 3A. The core of toroid is made of iron having relative magnetic permeability of mu_r = 5000 under given conditions. The magnetic field inside the iron is ___.(a) 0.15 T(b) 0.47 T(c) 1.5 x 10^-2 T(d) 1.88 T
›Reveal solutionSolution
The field in the toroid core is B = mu_0 mu_r n I; substituting gives about 1.88 T.
Field inside a toroid with a magnetic core: B = mu_0 mu_r n I, where n = 100 turns/m, I = 3 A, mu_r = 5000.
B = (4*pi x 10^-7)(5000)(100)(3) …
🎓Unlock everything free for 14 days
- ✓Full step-by-step solutions
- ✓Concept-first explanations
- ✓Methods, shortcuts & mistakes
- ✓PYQ mapping + timed mock tests
Full access for 14 days. No credit card required.