dB = (mu_0 / 4 pi) (I dl cross r_hat) / r^2
The field contribution d B equals mu nought over four pi, times I d l cross r hat, over r squared.
Field contribution from a current element.
- B
- magnetic field (T)
- I
- current (A)
- dl
- current-element length vector (m)
- r
- distance from element to field point (m)
Use when — Steady current element in free space, source-field problems without enough symmetry for Ampere's law.
Common trap — Dropping the vector direction or geometry of the cross product.
closed integral(B dot dl) = mu_0 I_enclosed
The closed-path integral of B dot d l equals mu nought times the enclosed current.
Ampere circuital law relating field circulation to enclosed current.
- B
- magnetic field (T)
- dl
- path-length element (m)
- I_enclosed
- net current enclosed by the path (A)
Use when — Magnetostatics; useful as a field-solving shortcut only with strong symmetry.
Common trap — Assuming B is constant on an arbitrary loop without justifying it from symmetry.
B = mu_0 I / (2 pi r)
B equals mu nought I over two pi r.
Field of an infinite straight current-carrying wire at perpendicular distance r.
- r
- perpendicular distance from the wire (m)
Use when — Ideal infinitely long straight wire.
Common trap — Applying near a finite end without correction.
B = mu_0 N I / (2 R)
B equals mu nought N I over two R.
Field at the centre of N circular turns.
- N
- number of turns
- R
- loop radius (m)
Use when — Closely wound coplanar circular turns, field at the centre.
Common trap — Using this centre-only result at any axial point.
B = mu_0 n I
B equals mu nought n I.
Field inside an ideal long solenoid.
- n
- turn density (turns per metre)
Use when — Long solenoid, away from ends.
Common trap — Using total turns where turn density is required.
F = q v cross B
Force equals q times v cross B.
Magnetic force on a moving charge.
- F
- force (N)
- q
- charge (C)
- v
- velocity (m/s)
- B
- magnetic field (T)
Use when — Point charge in a magnetic field.
Common trap — Forgetting that charge sign reverses direction.
r = m v_perp / (|q| B)
r equals m v perpendicular over the magnitude of q times B.
Radius of the circular component of a charged particle's path.
- r
- radius (m)
- m
- mass (kg)
- v_perp
- velocity component perpendicular to B (m/s)
Use when — Uniform B, non-relativistic particle.
Common trap — Using total speed when a parallel component also exists.
F = I L cross B
Force equals I times L cross B.
Force on a straight current-carrying segment.
- L
- length vector along current direction (m)
Use when — Uniform field over the segment.
Common trap — Losing current direction when forming the cross product.
mu = N I A ; tau = mu cross B
Magnetic moment equals N I A; torque equals mu cross B.
Magnetic moment of a current loop and the torque it experiences in a uniform field.
- mu
- magnetic moment (A m^2)
- A
- oriented area vector (m^2)
- tau
- torque (N m)
Use when — Planar loop in a uniform field.
Common trap — Using the geometric plane instead of the oriented area vector.
S = I_g G / (I - I_g)
Shunt resistance equals I g G over the quantity I minus I g.
Shunt resistance needed to convert a galvanometer to an ammeter of range I.
- S
- shunt resistance (ohm)
- G
- galvanometer resistance (ohm)
- I_g
- full-scale galvanometer current (A)
- I
- desired ammeter range (A)
Use when — Converting a galvanometer to an ammeter.
Common trap — Placing the shunt in series instead of in parallel.
R = V / I_g - G
Added series resistance equals V over I g, minus G.
Series resistance needed to convert a galvanometer to a voltmeter of range V.
- R
- added series resistance (ohm)
- V
- desired voltmeter range (V)
Use when — Converting a galvanometer to a voltmeter.
Common trap — Using a low parallel resistance instead of a high series resistance.