Magnetic fields and field lines
Earth's field at the surface is about 25 to 65 microtesla; the field inside a hospital MRI solenoid is tens of thousands of times stronger.
A map of forces
A magnet pushes or pulls on another magnet without touching it. To keep track of that action at a distance, physicists describe the space around a magnet with a magnetic field, the B field. At every point the field has a direction and a strength. The direction is defined by a small compass: the field points the way the compass needle's north end points. A compass is small enough not to disturb the field it measures.
Put compasses all around a bar magnet and join up the directions they show, and you get field lines. OpenStax sums up four rules for them. First, the field at a point is along the line there, so a compass lines up with it. Second, the strength is shown by how close the lines are: crowded lines mean a strong field. Third, field lines never cross, because the field has only one direction at each point. Fourth, they form closed loops with no start or end: outside the magnet they run from the north pole to the south pole, and inside they carry on from south back to north.
Field lines are a drawing tool, not threads in space. You can see their pattern, though, by shaking iron filings onto paper over a magnet. Each filing becomes a tiny magnet and turns along the field, so the filings settle into curves that match the lines.
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Measuring field strength: the tesla
The SI unit of magnetic field strength is the tesla (T). One tesla is a strong field: a wire 1 m long carrying 1 A across a 1 T field feels a force of 1 N, so 1 T = 1 N/(A·m). Everyday fields are much smaller, so you often see microtesla (μT, millionths of a tesla) and nanotesla (nT, billionths). An older unit, the gauss, is still common in geology and on magnet labels: 1 gauss = 10⁻⁴ T = 100,000 nT.
Some reference values help. NOAA's National Centers for Environmental Information give Earth's field at the surface as roughly 25,000 to 65,000 nT, which is 25 to 65 μT or 0.25 to 0.65 gauss. OpenStax often rounds it to 5.0 × 10⁻⁵ T, 50 μT. Its worked examples use 1.50 T for a strong laboratory magnet and 2.01 T inside a large solenoid of the kind used in MRI scanners. That is about 40,000 times Earth's field.
| Field | Strength |
|---|---|
| Earth's surface (NOAA range) | 25 to 65 μT |
| Earth, round value used in OpenStax | 50 μT = 5.0 × 10⁻⁵ T |
| Strong lab magnet (OpenStax example) | 1.50 T |
| Large solenoid as in MRI (OpenStax example) | 2.01 T |
Two magnets: the fields add
When two magnets are near each other, the field at any point is the sum of the two fields, added as arrows. Put a north pole facing a south pole and the lines run straight across the gap from one magnet into the other; the field in the gap is strong, and the magnets pull together. Put two north poles face to face and the lines from each are turned aside. They squeeze sideways out of the gap, and halfway between the poles there is a spot where the two fields cancel. A compass placed exactly there has no preferred direction and only Earth's weak field steers it.
The same adding explains why a compass on a desk can mislead you. A steel desk frame, a speaker magnet or a current in nearby wiring makes its own field, and near it that field can be stronger than Earth's 25 to 65 μT. The needle then points along the total, not toward the north. Hold a compass away from metal objects and electrical equipment when you want a true reading.
| Direction of B | The way a compass needle's north end points |
| Crowded field lines | A strong field |
| Outside a magnet, lines run… | From N to S |
| Tesla (T) | 1 T = 1 N/(A·m) |
| 1 gauss | 10⁻⁴ T = 100,000 nT |
- A compass shows the field direction: its north end points along B.
- Field lines: tangent to B, closer means stronger, never cross, closed loops N to S outside.
- The SI unit is the tesla; 1 gauss = 10⁻⁴ T.
- Earth's field is about 25 to 65 μT at the surface.
- Outside a bar magnet, field lines run:
- From N to S
- From S to N
- In straight lines away from both poles
- Round in circles about the middle
- Where are field lines closest together around a bar magnet?
- Near the poles
- Far from the magnet
- At the middle of the side
- They are equally spaced everywhere
- Why can two field lines never cross?
- The field has one direction at each point
- Lines repel each other
- They are made of iron
- They only exist inside magnets
- How many nanotesla are in 1 gauss?
- Earth's field at a place is 50,000 nT. What is that in gauss?
- Express 50 μT in tesla, in units of 10⁻⁵ T (so 5.0 means 5.0 × 10⁻⁵ T).
- How many times stronger than 50 μT is a 2.01 T field? (nearest whole number)
- What does the compass needle's north end point along?
- The direction of the magnetic field
- Always the geographic North Pole
- The nearest piece of iron
- The direction of the electric field
- Iron filings sprinkled over a magnet line up because:
- Each filing becomes a tiny magnet and turns along the field
- They are charged
- Air currents push them
- Gravity pulls them to the poles
- Inside a bar magnet, the field lines run:
- From S to N
- From N to S
- Nowhere; they stop at the poles
- In circles
Sources for this course (16)
- OpenStax College Physics 2e (openstax.org/books/college-physics-2e): 22.1 Magnets (all magnets have N and S poles, north-seeking and south-seeking, like poles repel and unlike attract, poles cannot be separated, the magnetic pole near the geographic North Pole is a south magnetic pole, sunspots come in N/S pairs)
- 22.2 Ferromagnets and electromagnets (iron, cobalt, nickel, gadolinium; neodymium alloys; domains grow to millimetre size; Curie temperature of iron 1043 K (770 °C); Oersted saw a compass needle deflected by a current; electromagnets in scrapyard cranes, particle accelerators and MRI; electric current is the source of all magnetism; no monopoles observed)
- 22.3 Magnetic fields and field lines (direction = where a compass north end points; four rules: tangent, density = strength, never cross, closed loops from N to S outside)
- 22.7 Magnetic force on a current-carrying conductor (F = I l B sin θ, 1 T = 1 N/(A·m), example 20.0 A, 5.00 cm, 1.50 T gives 1.50 N; motors)
- 22.9 Magnetic fields produced by currents (Oersted 1820, right hand rule 2, B = μ0 I ÷ (2π r), μ0 = 4π × 10⁻⁷ T·m/A, Earth's field about 5.0 × 10⁻⁵ T, 25 A at 5.0 cm gives twice that; loop centre B = N μ0 I ÷ 2R; solenoid B = μ0 n I, 2000 loops over 2.00 m with 1600 A gives 2.01 T, MRI; ferromagnetic cores)
- 23.1 Induced emf and magnetic flux (Faraday's iron-ring apparatus, emf only while the field changes, magnet pushed into a coil, faster motion gives more emf, generators, Φ = B A cos θ)
- NIST CODATA 2022 vacuum magnetic permeability μ0 = 1.25663706127(20) × 10⁻⁶ N/A² (physics.nist.gov/cgi-bin/cuu/Value?mu0)
- NOAA NCEI Geomagnetism Frequently Asked Questions (ncei.noaa.gov/products/geomagnetism-frequently-asked-questions): field like a dipole at Earth's centre, over 90% from the outer core, intensity roughly 25,000 to 65,000 nT (0.25 to 0.65 gauss)
- 1 gauss = 100,000 nT, declination = angle between magnetic north and true north (east positive)
- inclination, dip poles, dipole axis 9.41° from the rotation axis (WMM2020, 2020.0)
- north magnetic pole moving about 55 km per year north-northwest (2001 and 2007 surveys)
- last reversal about 750,000 to 780,000 years ago, reversals spaced 5 thousand to 50 million years, a reversal would take several thousand years, models renewed every five years, blackout zones where H < 2000 nT, compass balance weights differ by hemisphere, true bearing = magnetic bearing + declination
- NOAA NCEI news "World Magnetic Model 2025 Released" (17 December 2024)
- NOAA NCEI "December 2025 State of the Geomagnetic Field" (north dip pole 36 km/yr and south dip pole 9 km/yr since 1 January 2025)
- USGS, "Pre-gilbertian conceptions of terrestrial magnetism" (pubs.usgs.gov/publication/70009843): Gilbert's De Magnete (1600) first suggested that Earth behaves as a great magnet. Royal Institution, Michael Faraday's ring-coil apparatus (rigb.org): made August 1831, success on 29 August 1831, the first electric transformer
- APS News "This Month in Physics History" (Aug 2001): Faraday's electromagnetic rotation experiments of September 1821, the principle behind the electric motor.
Checked: 2026-10-17