Section 4.2 · Worked examples · 3 of 3
Worked example 4.2.3: Loudspeaker voice coil
About the worked examples of Section 4.2
Three short calculations tied to the applications. They use only , and the Lorentz force , and no new physics. Numerical constants: , . A good way to use them: read the given quantities, produce the formula from the corresponding application or problem yourself, and only then put the numbers in.
Loudspeaker voice coil
#cf. Application 4.2.3
Given. A loudspeaker gap with a radial field . The voice coil has turns of radius , all inside the gap, and carries . The moving mass (coil, former and cone) is .
Find. (a) the length of wire in the field and the force factor , (b) the force on the coil, (c) the acceleration of the moving mass, in m/s and in units of , (d) the force when the current reverses.
Each element sits in , so : axial, and of the same sign all round the coil. The total force is times the total wire length, with , Eq. (4.2.41).
.
With ,
changes sign with : , the cone is pulled inwards. An alternating current of amplitude drives the cone with a force of amplitude at the signal frequency.
Units: TmA (Vs/m)(m)(A) (VAs)/m J/m N. Only , yet , because the moving mass is tiny. is the same wherever the coil sits in the gap, since is radial everywhere there: a linear motor. It is the spider and the surround, not the field, that bring the cone back (Application 4.2.3).