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The Transient Magnetic Behaviour of Loudspeaker Motors' Mark Dodd

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Constant current density in conductive region. Total Flux in gap ... stranded conductor' constant current density. ... Power density at 20Hz 40vrms input with ... – PowerPoint PPT presentation

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Title: The Transient Magnetic Behaviour of Loudspeaker Motors' Mark Dodd


1
The Transient Magnetic Behaviour of Loudspeaker
Motors.Mark Dodd
2
Loudspeaker Basics
  • Loudspeakers convert an electrical signal to a
    mechanical signal and then to an acoustic signal.

  • Moving coil linear actuator voltage -gt motion.
  • Diaphragm motion -gt sound pressure.

3
Loudspeaker Basics.
  • Rigid body motion assumed.
  • Mechanically loudspeaker is equivalent to a mass,
    m mechanical resistance rmc and spring stiffness
    k.
  • Equating forces gives Drive force F
  • For a small current i

4
Loudspeaker Basics.
  • The acoustic pressure P produced, at distance r
    by a sinusoidal point source with volume velocity
    U at angular frequency w is given by
  • Where volume velocity U is produced by a
    diaphragm with area S moving at velocity, dx/dt
    is given by

5
Pass Band Response.
  • Motion mass-limited, decreasing amplitude with
    frequency.

m
0.28m
0.21m
0.14m
70u
0
20
50
100
100
200
500
1k
1k
2k
5k
10k
10k
20k
20
20k
Frequency
Hz
6
Pass Band Response.
  • Velocity amplitude decreases above resonance
    frequency.

-40
dB
-54
-68
-82
-96
-110
20
50
100
100
200
500
1k
1k
2k
5k
10k
10k
20k
20
20k
Frequency
Hz
7
Pass Band Response.
  • Radiation efficiency increases with increasing
    frequency.

ohm
4.3k
3.3k
2.2k
1.2k
100
20
50
100
100
200
500
1k
1k
2k
5k
10k
10k
20
20k
Frequency
Hz
8
Pass Band Response.
  • Motional impedance is reflected in electrical
    domain.
  • Net result is an SPL response with a flat pass
    band.

dB
110
80
dB
Uin2.83Vrms, Distance1m
100
64
90
48
80
32
70
16
60
0
20
50
100
100
200
500
1k
1k
2k
5k
10k
10k
20k
20
20k
Frequency
Hz
9
Previous Approach
  • Consider the static flux from permanent magnet
    separately from flux produced by current flowing
    through the coil.
  • Use FEM to calculate static field calculate
    Bl(x) for different coil displacements x.
  • Calculate Flux through coil for an arbitrary
    current.

10
Polynomial method
  • Assume that Lvc is a function of x but not i.
  • Express force variation with current in terms of
    coil inductance

FBl(x)I-Lvc(x)i2.
11
Polynomial method
  • Eddy Currents.
  • AC signal through coil results in alternating
    magnetic field.
  • EMF induced in any conductive loops round field.
  • Current flow in skin depth.

12
Polynomial method
  • Eddy currents
  • assumed to be confined to a cylindrical region
    equal to skin depth adjacent to coil.
  • Permeability fixed at average static value.
  • Constant current density in conductive region.
  • Total Flux in gap now given by
  • Flux from eddy currents used to derive Lvc as a
    function of frequency and coil position Lvc(x,f).

13
Polynomial method
  • Equating forces.
  • Equating voltages.
  • Runge Kutta method used to numerically solve
    equations.
  • Spectrum of distorted sinusoidal waveform
    produced is analysed with FFT.

14
New Magnet Topology
15
Flux2D Magneto-static FEM.
  • Magneto-static solver uses static version of
    Maxwell's equation.
  • Force on a coil is calculated using

16
Flux2D Magneto-static FEM Results.
  • The force versus displacement may be calculated
    for a range of coil displacements.

17
Flux 2D Magneto-static FEM Results.
  • Voice coil self Inductance may be calculated for
    different coil positions and currents.

18
Flux2D Magneto-dynamic FEM
  • Linear steady state sinusoidal solution.
  • No static magnetic field.
  • Sinusoidal input to coil induces eddy-currents in
    conductive regions.
  • Use of permeability from static solution would
    give quick calculation of small signal dynamic
    fields.
  • Could be used to generate Lvc(x,f) for parametric
    model.

19
Flux2D Transient Magnetic FEM
  • Allows solution of stationary voice coil
    permanent magnet with poles of non-linear steel
    for time-varying currents fields.
  • Based on dynamic Maxwell's equation.
  • Solution is made for 40-120 time-steps per period.

20
Flux2D Transient Magnetic FEM
  • Mesh uses quadrilateral elements to mesh skin
    and give a fast solution time.
  • Mesh has frequency dependant spacing
    perpendicular to metal surface.


21
Flux2D Transient Magnetic FEM
  • Sinusoidal voltage source input allows
    calculation of blocked impedance of coil.
  • Voice coil is stranded conductor constant
    current density.
  • Iron NdFeB are solid conductors with eddy
    currents.
  • Hysteresis is neglected.
  • Calculation may be for different coil positions
    and voltage inputs.

22
Flux2D Transient Magnetic FEM
  • Flux at 80Hz.

23
Flux2D Transient Magnetic FEM
  • Permeability at 80Hz.

24
Flux2D Transient Magnetic FEM
  • Power density currents at 80Hz various coil
    displacements.

25
Flux2D Transient Magnetic FEM
  • Power density currents at 20Hz, 80Hz 240Hz.

26
Flux2D Transient Magnetic FEM With Kinematics
  • Mass, compliance and mechanical resistance
    included in the model.
  • Acceleration is derived from driving force.
  • Displacement mesh allows solution with coil
    displaced axially.
  • Rigid body motion assumed.
  • Compliance assumed to be linear.
  • Iron BH curve and compliance force stiffness
    curves do not include hysteresis.

27
Kinematic Validation.
28
Flux2D Transient Magnetic FEM with Kinematics
Results.
  • Power density at 20Hz 40vrms input with coil
    motion.

29
Flux2D Transient Magnetic FEM with Kinematics
Results.
  • magnetic field in gap plotted along contour, at
    20Hz 40vrms input as a function of time.

30
Flux2D Transient Magnetic FEM With Kinematics
Results.
  • waveform and spectra of eddy currents in pole

31
Flux2D Transient Magnetic FEM with Kinematics
Results.
  • Acceleration waveform and spectra at 20Hz for
    40vrms input.

32
Flux2D Transient Magnetic FEM With Kinematics
Results.
  • Relative Harmonic distortion of cone acceleration.

33
Flux2D Transient Magnetic FEM With Kinematics
Results.
  • Measured Versus FEM of SPL Magnitude of
    impedance.

34
Conclusion.
  • Flux2D is able to predict loudspeaker motor
    distortion from geometry and material properties.
  • FEM results contain a wealth of data including
    some which cannot be readily measured.
  • Possible improvements are
  • Include FEM derived Force versus Displacement
    data for suspension.
  • Include magnetic Hysteresis of iron.
  • Include mechanical Hysteresis of suspension.
  • Better material property data required!
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