Physics and engineering

Magnetic Force Trajectory Calculator

Solve a nonrelativistic charged particle's helical radius, period, phase, pitch, position, and velocity in a uniform magnetic field.

CURRENT MODEL

Define one particle and elapsed uniform-field flight

Physics students, beamline learners, and laboratory teams estimating ideal particle paths before numerical field-map tracking.

Decision supportedEstimate whether a charged particle's ideal radius, pitch, and elapsed-time position fit a uniform-field region.
Gyroradius--
Cyclotron period--
Signed revolutions--
Axial advance--
Final transverse position--
Path state--

PHYSICAL CONTEXT

The modeled decision in context

This static editorial scene clarifies the apparatus and evidence boundary; all current numeric detail remains in the exact ledger below.

A beamline physicist follows a charged particle spiralling through a cylindrical uniform magnetic-field chamber.
A uniform-field chamber illustrates the ideal helical path, while real beamline fringe fields and material interactions remain outside the model.
Charged-particle trajectory ledgerCurrent values; full precision retained before display rounding
Charged-particle trajectory ledger for current inputs
QuantitySymbol or equationCurrent valueUnit

How to use

Set a nonrelativistic particle trajectory

  1. Enter signed charge in elementary-charge multiples.
  2. Enter particle mass in unified atomic mass units.
  3. Use initial speed below the stated nonrelativistic limit.
  4. Measure velocity angle from the +B direction.
  5. Enter positive uniform field and elapsed time.
  6. Review radius, pitch, signed turns, position, and speed check together.

Trajectory fundamentals

Six facts behind a magnetic helix

Perpendicular component
Creates circular gyromotion.
Parallel component
Advances uniformly along field.
Charge sign
Reverses rotation handedness.
Gyroradius
Scales with momentum perpendicular to field.
Cyclotron period
Is independent of speed in the nonrelativistic uniform model.
No magnetic work
Ideal magnetic force preserves speed.

Calculation method

Decompose velocity before integrating position

The page converts charge, mass, field, speed, and time to SI, splits velocity by pitch angle, then uses signed angular frequency to integrate transverse coordinates and parallel drift.

Handedness evidence

Signed turns and coordinates preserve charge sign; taking absolute charge too early would erase a measurable trajectory distinction.

Relativistic boundary

Above the page limit, momentum gains a gamma factor and both radius and frequency need a relativistic treatment.

Field-map departure

Real fringe fields can change pitch and guiding centre, requiring stepwise Lorentz integration rather than a closed helix.

Detailed calculation process

Symbols, conversions, substitution, intermediate results, and reconciliation

v_perp=v sin(alpha); omega=qB/m; r=m v_perp/(|q|B); T=2pi/|omega|SI constants, phase, and coordinates retain full precision; nonrelativistic validity and aligned-path state are evaluated before formatting.
Trajectory symbols and defaults
SymbolMeaningDefaultUnit
qSigned particle charge+1e
mParticle mass1.007276466621u
vInitial speed100km/s
alphaAngle from +B60deg
BUniform field50mT
tElapsed time2microseconds

    Waiting for valid inputs.

    Interpretation

    Read radius, pitch, and phase as one path

    Radius describes transverse confinement, pitch gives axial distance per turn, and signed phase locates the particle at the entered time. A zero radius can mean a valid field-aligned path.

    Evidence and measurement

    Preserve initial conditions and field definition

    Record particle species and charge state, mass source, velocity distribution, pitch-angle datum, field-map region, entry coordinates, timing reference, vacuum quality, detector resolution, uncertainty, and relativistic screening.

    Scope and limitations

    What the ideal helix excludes

    • Electric fields and E cross B drift
    • Field gradients and magnetic mirrors
    • Collisions and material energy loss
    • Radiation loss and space charge
    • Relativistic momentum
    • Beamline safety and acceptance

    Uniform magnetic field along +z, no electric field, no collisions or radiation loss, and speed below 0.1c. Charge sign controls handedness.

    Key terminology

    Trajectory glossary

    Pitch angle
    Angle between velocity and magnetic field.
    Gyroradius
    Radius of transverse circular motion.
    Cyclotron period
    Time for one ideal revolution.
    Helix pitch
    Axial advance per turn.
    Guiding centre
    Centre around which transverse motion circles.
    Charge state
    Signed number of elementary charges.

    Practical cases

    Two distinct path regimes

    Proton-like helical flight

    The default case completes about 1.525 signed turns while advancing 100 mm along +z.

    Field-aligned injection

    At zero pitch angle radius collapses to zero and the particle travels straight, a valid boundary rather than an error.

    Important note

    Uniform-field tracking is a screening model

    Use a verified field map and relativistic numerical integrator for real beam transport or exposure decisions.

    Frequently asked questions

    Why does the magnetic field not change particle speed?

    The Lorentz magnetic force is perpendicular to velocity, so it changes direction while doing no work in this ideal model.

    What does negative charge change?

    It reverses the sign of angular frequency and therefore the helix handedness, while radius and period magnitudes remain unchanged.

    Why is there a helical pitch?

    The perpendicular velocity circles around the field while the parallel component continues uniformly along it.

    What happens at zero pitch angle?

    Perpendicular speed and radius are zero, so the particle travels straight along the field without gyromotion.

    Why reject speeds at 0.1c?

    The formulas use nonrelativistic momentum. At higher speed, relativistic gamma changes radius and angular frequency materially.

    Can this track a particle through a real magnet fringe?

    No. Field gradients, fringe regions, electric fields, scattering, and material interactions require numerical integration through a field map.

    Authority and follow-on work

    Reliable sources and related calculators