Vary number of turns, current, length, and relative permeability to calculate internal magnetic field, axial field distribution, and inductance in real time.
Coil Parameters
Central magnetic flux density B₀
—
mT
While paused, moving a slider updates the results immediately.
Results
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Internal magnetic field B [mT]
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Turn density n [/m]
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Current I [A]
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Inductance L
Current (around the coil)Uniform internal magnetic fieldExternal magnetic field linesN poleS pole
Changing the number of turns N, current I, coil length L, or relative permeability μr changes the coil current and the density (∝ n·I) of the uniform internal field and looping external field lines in real time.
Axial
Magnetic field intensity H
—
Turn density n
—
Inductance L
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End field B_end
—
On-axis magnetic-field distribution
Current and turn-count comparison
Magnetic-field map
Compare
On-axis magnetic-field distribution. It is uniform at the center and falls to approximately half at the ends.
Field
The magnetic field is proportional to both current and the number of turns (proportional to nI).
Theory & Key Formulas
Magnetic-field strength map inside and outside the solenoid (cross section), showing the uniform field inside.
Theory & Key Formulas
$B_0 = \mu_0 \mu_r n I = \mu_0 \mu_r \dfrac{N}{L} I$
Inductance
$L = \mu_0 \mu_r \dfrac{N^2 A}{l}$ (A is the cross-sectional area)
On-axis magnetic field (finite-length effect)
$B(x) = \dfrac{\mu_0 \mu_r n I}{2}(\cos\theta_1 + \cos\theta_2)$
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Earth's magnetic field is about 0.05 mT, while a refrigerator magnet is around 10 mT. A 1.5 T MRI field is about 30,000 times Earth's field, and a 3 T MRI is about 60,000 times stronger. Research high-field magnets can reach roughly 45 T. Producing 3 T with ordinary copper windings would create enormous Joule heating, so superconducting coils with near-zero resistance are essential. This is why MRI magnets are cooled with liquid helium.
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What kind of CAE analyses use solenoid magnetic field calculations?
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This is a typical application of electromagnetic CAE and FEM-EM analysis in tools such as ANSYS Maxwell, COMSOL, and Abaqus EM. Examples include heating-pattern prediction for induction heating, torque optimization in motors and generators, pull-force design for solenoid valves, and uniform-field shimming for MRI and NMR equipment. Eddy-current loss calculations are also important for reducing transformer core losses.
Frequently Asked Questions
The horizontal axis of the graph represents the axial position from the center of the solenoid, and the vertical axis represents the magnetic flux density. Increasing the number of turns or the current proportionally increases the value on the vertical axis. Additionally, changing the length alters the extent of the uniform magnetic field region, so pay attention to the shape of the distribution.
This simulator assumes the insertion of a magnetic material such as an iron core, but the effect of relative permeability is directly reflected in the calculation formula for the internal magnetic field. If the value does not change, please check whether the input field has been correctly updated with the numerical value or whether the browser has properly recalculated.
Inductance indicates the energy storage capability of the coil and is important for circuit design and transient response analysis. For example, it can be used as a parameter that determines the speed of current change in switching power supplies or motor drive circuits.
Increasing the radius narrows the uniform magnetic field region inside and makes the magnetic field decay more gradual at the ends. Additionally, even with the same number of turns and current, the central magnetic field decreases slightly. When designing, choose the radius by considering the balance between the desired uniform region and magnetic field strength.
What is Solenoid Magnetic Field?
Solenoid Magnetic Field is a fundamental topic in engineering and applied physics. This interactive simulator lets you explore the key behaviors and relationships by directly manipulating parameters and observing real-time results.
By combining numerical computation with visual feedback, the simulator bridges the gap between abstract theory and physical intuition — making it an effective learning tool for students and a rapid-verification tool for practicing engineers.
Physical Model & Key Equations
The simulator is based on the governing equations behind Solenoid Magnetic Field Calculator. Understanding these equations is key to interpreting the results correctly.
Each parameter in the equations corresponds to a slider in the control panel. Moving a slider changes the equation's solution in real time, helping you build a direct connection between mathematical expressions and physical behavior.
Real-World Applications
Engineering Design: The concepts behind Solenoid Magnetic Field Calculator are applied across mechanical, structural, electrical, and fluid engineering disciplines. This tool provides a quick way to estimate design parameters and sensitivity before committing to full CAE analysis.
Education & Research: Widely used in engineering curricula to connect theory with numerical computation. Also serves as a first-pass validation tool in research settings.
CAE Workflow Integration: Before running finite element (FEM) or computational fluid dynamics (CFD) simulations, engineers use simplified models like this to establish physical scale, identify dominant parameters, and define realistic boundary conditions.
Common Misconceptions and Points of Caution
Model assumptions: The mathematical model used here relies on simplifying assumptions such as linearity, homogeneity, and isotropy. Always verify that your real system satisfies these assumptions before applying results directly to design decisions.
Units and scale: Many calculation errors arise from unit conversion mistakes or order-of-magnitude errors. Pay close attention to the units shown next to each parameter input.
Validating results: Always sanity-check simulator output against physical intuition or hand calculations. If a result seems unexpected, review your input parameters or verify with an independent method.
Set coil turns (N) using nSlider: typical range 100–10,000 for industrial solenoids
Adjust current (I) in amperes via iSlider: 0.5–20A covers most actuator applications
Define solenoid length (L) in millimeters using lSlider: 10–200mm for compact designs
Configure coil radius (R) in millimeters via rSlider: 5–50mm for standard core diameters
Observe real-time field magnitude updates for axial, internal, and external field regions
Worked Example
A relay solenoid with N=500 turns, I=2.5A, L=25mm, R=8mm generates internal axial field B = μ₀nI = (1.257×10⁻⁶ H/m)(20,000 turns/m)(2.5A) ≈ 62.8 mT at coil center. External field drops to ~8 mT at radial distance 15mm from axis. Ampère's law confirms field concentration within bore versus rapid decay outside winding.
Practical Notes
Solenoid actuators for industrial pneumatic valves operate 12–24V DC; use iSlider to match coil resistance and verify pull-in field threshold (typically 30–50 mT minimum)
Ferromagnetic core insertion increases internal field 200–400× depending on permeability; this calculator shows air-core baseline
Axial field homogeneity degrades near coil ends; account for fringe effects when positioning sensors or armature travel limits
Eddy current losses scale with frequency; for DC holding coils, static field dominates; for AC switching (50/60 Hz), laminated cores reduce heating
🎬 Watch it in motion
Cyclotron Motion | fast or slow, the same orbit time #Shorts
Lenz's Law | A Magnet Falls in Slow Motion #Shorts
Magnetic Field Lines | closed loops, no loose ends #Shorts
Cyclotron Motion | fast or slow, the same orbit time #Shorts
