mi.lib

//############################# mi.lib #########################################
// This ongoing work is the fruit of a collaboration between GRAME-CNCM and
// the ANIS (Arts Numériques et Immersions Sensorielles) research group from
// GIPSA-Lab (Université Grenoble Alpes).
//
// This library implements basic 1-DoF mass-interaction physics algorithms,
// allowing to declare and connect physical elements (masses, springs, non
// linear interactions, etc.) together to form topological networks.
// Models can be assembled by hand, however in more complex scenarios it is
// recommended to use a scripting tool (such as MIMS) to generate the FAUST
// signal routing for a given physical network. Its official prefix is `mi`.
//
// [Video introduction to Mass Interaction](https://faust.grame.fr/community/events/#an-introduction-to-mass-interaction-modelling-in-faust-james-leonard-and-jerome-villeneuve)
//
// [LAC 2019 Paper](https://hal.science/hal-02270654)
//
// ## Sources
//
// The core mass-interaction algorithms implemented in this library are in the public
// domain and are disclosed in the following scientific publications:
//
// * Claude Cadoz, Annie Luciani, Jean-Loup Florens, Curtis Roads and Françoise
// Chabade. Responsive Input Devices and Sound Synthesis by Stimulation of
// Instrumental Mechanisms: The Cordis System. Computer Music Journal, Vol 8.
// No. 3, 1984.
// * Claude Cadoz, Annie Luciani and Jean Loup Florens. CORDIS-ANIMA: A Modeling
// and Simulation System for Sound and Image Synthesis: The General Formalism.
// Computer Music Journal. Vol. 17, No. 1, 1993.
// * Alexandros Kontogeorgakopoulos and Claude Cadoz. Cordis Anima Physical
// Modeling and Simulation System Analysis. In Proceedings of the Sound and Music
// Computing Conference (SMC-07), Lefkada, Greece, 2007.
// * Nicolas Castagne, Claude Cadoz, Ali Allaoui and Olivier Tache. G3: Genesis
// Software Environment Update. In Proceedings of the International Computer
// Music Conference (ICMC-09), Montreal, Canada, 2009.
// * Nicolas Castagné and Claude Cadoz. Genesis 3: Plate-forme pour la création
// musicale à l'aide des modèles physiques Cordis-Anima. In Proceedings of the
// Journée de l'Informatique Musicale, Grenoble, France, 2009.
// * Edgar Berdahl and Julius O. Smith. An Introduction to the Synth-A-Modeler
// Compiler: Modular and Open-Source Sound Synthesis using Physical Models. In
// Proceedings of the Linux Audio Conference (LAC-12), Stanford, USA, 2012.
// * James Leonard and Claude Cadoz. Physical Modelling Concepts for a Collection
// of Multisensory Virtual Musical Instruments. In Proceedings of the New
// Interfaces for Musical Expression (NIME-15) Conference, Baton Rouge, USA, 2015.
//
// #### References
// * <https://github.com/grame-cncm/faustlibraries/blob/master/mi.lib>
//##############################################################################

ma = library("maths.lib");
ba = library("basics.lib");

declare name "Faust mass-interaction physical modelling library";
declare version "1.1.0";
declare author "James Leonard";
declare author "Romain Michon";
declare copyright "2018-2020 GRAME / GIPSA-Lab";

//===============================Utility Functions========================================
// These utility functions are used to help certain operations (e.g. define initial
// positions and velocities for physical elements).
//========================================================================================


//------------------------`(mi.)initState`----------------------
// Used to set initial delayed position values that must be initialised
// at step 0 of the physics simulation.
//
// If you develop any of your own modules, you will need to use this (see
// `mass` and `springDamper` algorithm codes for examples).
//
// #### Usage
//
// ```
// x : initState(x0) : _
// ```
//
// Where:
//
// * `x`: position value signal
// * `x0`: initial value for position
//---------------------------------------------------------
initState(init) = R(0,init)
with{
  R(n,(initn,init)) = +(1: ba.impulsify@n * initn) : R(n+1,init);
  R(n,initn) = +(1 : ba.impulsify@n * initn);
};


//=================================Mass Algorithms========================================
// All mass-type physical element functions are declared here. They all expect to receive
// a force input signal and produce a position signal.
// All physical parameters are expressed in sample-rate dependant values.
//========================================================================================


//------------------------`(mi.)mass`----------------------
// Implementation of a punctual mass element.
// Takes an input force and produces output position.
//
// #### Usage
//
// ```
// mass(m, grav, x0, xr0),_ : _
// ```
//
// Where:
//
// * `m`: mass value
// * `grav`: gravity force value
// * `x0`: initial position
// * `xr0`: initial delayed position (inferred from initial velocity)
//---------------------------------------------------------
mass(m, grav, x0, x1) = equation
with{
  A = 2;
  B = -1;
  C = 1/m;
  equation = x 
	letrec{
    'x = A*(x : initState(x0)) + B*(x' : initState((x1,x0))) + (_-grav)*(C);
	};
};


//------------------------`(mi.)oscil`----------------------
// Implementation of a simple linear harmonic oscillator.
// Takes an input force and produces output position.
//
// #### Usage
//
// ```
// oscil(m, k, z, grav, x0, xr0),_ : _
// ```
//
// Where:
//
// * `m`: mass value
// * `k`: stiffness value
// * `z`: damping value
// * `grav`: gravity force value
// * `x0`: initial position
// * `xr0`: initial delayed position (inferred from initial velocity)
//---------------------------------------------------------
oscil(m, k, z, grav, x0, x1) = equation
with{
  A = 2 - (k + z)/m;
  B = z/m - 1;
  C = 1/m;
  equation = x
	letrec{
    'x = A*(x : initState(x0)) + B*(x' : initState((x1, x0))) + (_-grav)*(C);
	};
};


//------------------------`(mi.)ground`----------------------
// Implementation of a fixed point element.
// The position output produced by this module never changes, however
// it still expects a force input signal (for compliance with connection
// rules).
//
// #### Usage
//
// ```
// ground(x0),_ : _
// ```
//
// Where:
//
// * `x0`: initial position
//---------------------------------------------------------
ground(x0) = equation
with{
  // could this term be removed or simlified? Need "unused" input force signal for the routing scheme to work
  C = 0;
  equation = x 
	letrec{
		'x = (x : initState(x0)) + *(C);
	};
};


//------------------------`(mi.)posInput`----------------------
// Implementation of a position input module (driven by an outside
// signal). Takes two signal inputs: incoming force (which doesn't
// affect position) and the driving position signal.
//
// #### Usage
//
// ```
// posInput(x0),_,_ : _
// ```
//
// Where:
//
// * `x0`: initial position
//---------------------------------------------------------
posInput(init) = _,_ : !,_ : initState(init);


//===============================Interaction Algorithms====================================
// All interaction-type physical element functions are declared here. They each expect to
// receive two position signals (coming from the two mass-elements that they connect) and
// produce two equal and opposite force signals that must be routed back to the mass
// elements' inputs.
// All physical parameters are expressed in sample-rate dependant values.
//=========================================================================================


//------------------------`(mi.)spring`----------------------
// Implementation of a linear elastic spring interaction.
//
// #### Usage
//
// ```
// spring(k, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `k`: stiffness value
// * `x1r`: initial delayed position of mass 1 (unused here)
// * `x2r`: initial delayed position of mass 2 (unused here)
//---------------------------------------------------------
spring(k, x1r0, x2r0, x1, x2) = 
  k*deltapos <: *(-1),_
with{
    deltapos = x1-x2;
};


//------------------------`(mi.)damper`----------------------
// Implementation of a linear damper interaction.
// Beware: in 32bit precision mode, damping forces can become
// truncated if position values are not centered around zero!
//
// #### Usage
//
// ```
// damper(z, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `z`: damping value
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
damper(z, x1r0, x2r0, x1, x2) = 
  z*deltavel <: *(-1),_
with{
    deltavel = (x1 - x1' : initState(x1r0)) - (x2 - x2' : initState(x2r0));
};


//------------------------`(mi.)springDamper`----------------------
// Implementation of a linear viscoelastic spring-damper interaction
// (a combination of the spring and damper modules).
//
// #### Usage
//
// ```
// springDamper(k, z, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `k`: stiffness value
// * `z`: damping value
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
springDamper(k, z, x1r0, x2r0, x1, x2) = 
  k*deltapos + 
  z*deltavel <: *(-1),_
with{
    deltapos = x1-x2;
    deltavel = (x1 - x1' : initState(x1r0)) - (x2 - x2' : initState(x2r0));
};


//------------------------`(mi.)nlSpringDamper2`----------------------
// Implementation of a non-linear viscoelastic spring-damper interaction
// containing a quadratic term (function of squared distance).
// Beware: at high displacements, this interaction will break numerical
// stability conditions ! The `nlSpringDamperClipped` is a safer option.
//
// #### Usage
//
// ```
// nlSpringDamper2(k, q, z, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `k`: linear stiffness value
// * `q`: quadratic stiffness value
// * `z`: damping value
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
nlSpringDamper2(k, q, z, x1r0, x2r0, x1, x2) =
  k*deltapos + q * ma.signum(deltapos) * pow(deltapos, 2) +
  z*deltavel <: *(-1),_
with{
    deltapos = x1-x2;
    deltavel = (x1 - x1' : initState(x1r0)) - (x2 - x2' : initState(x2r0));
};


//------------------------`(mi.)nlSpringDamper3`----------------------
// Implementation of a non-linear viscoelastic spring-damper interaction
// containing a cubic term (function of distance^3).
// Beware: at high displacements, this interaction will break numerical
// stability conditions ! The `nlSpringDamperClipped` is a safer option.
//
// #### Usage
//
// ```
// nlSpringDamper3(k, q, z, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `k`: linear stiffness value
// * `q`: cubic stiffness value
// * `z`: damping value
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
nlSpringDamper3(k, q, z, x1r0, x2r0, x1, x2) =
  k*deltapos + q * pow(deltapos, 3) +
  z*deltavel <: *(-1),_
with{
    deltapos = x1-x2;
    deltavel = (x1 - x1' : initState(x1r0)) - (x2 - x2' : initState(x2r0));
};


//------------------------`(mi.)nlSpringDamperClipped`----------------------
// Implementation of a non-linear viscoelastic spring-damper interaction
// containing a cubic term (function of distance^3), bound by an
// upper linear stiffness (hard-clipping).
//
// This bounding means that when faced with strong displacements, the
// interaction profile will "clip" at a given point and never produce
// forces higher than the bounding equivalent linear spring, stopping models
// from becoming unstable.
//
// So far the interaction clips "hard" (with no soft-knee spline
// interpolation, etc.)
//
// #### Usage
//
// ```
// nlSpringDamperClipped(s, c, k, z, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `s`: linear stiffness value
// * `c`: cubic stiffness value
// * `k`: upper-bound linear stiffness value
// * `z`: (linear) damping value
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
nlSpringDamperClipped(s, c, k, z, x1r0, x2r0, x1, x2) =
    select2(c == 0,
        select2(s >= k,
            select2(absdeltapos <= b,
                // Overdamping induced here to prevent "locked" states...
                k * deltapos + (z+0.3*k)*deltavel,
                s * deltapos + c * pow(deltapos, 3) + z*deltavel
            ),
            k * deltapos + z*deltavel
        ),
        s * deltapos + z*deltavel
    )<: *(-1),_
with{
    b = sqrt(k-s)/c;
    deltapos = x1-x2;
    deltavel = (x1 - x1' : initState(x1r0)) - (x2 - x2' : initState(x2r0));
    absdeltapos = abs(deltapos);

};


//------------------------`(mi.)nlPluck`----------------------
// Implementation of a piecewise linear plucking interaction.
// The symmetric function provides a repulsive viscoelastic interaction
// upon contact, until a tipping point is reached (when the plucking occurs).
// The tipping point depends both on the stiffness and the distance scaling
// of the interaction.
//
//
// #### Usage
//
// ```
// nlPluck(knl, scale, z, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `knl`: stiffness scaling parameter (vertical stretch of the NL function)
// * `scale`: distance scaling parameter (horizontal stretch of the NL function)
// * `z`: (linear) damping value
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
nlPluck(k, scale, z, x1r0, x2r0, x1, x2) = 
  select2(absdeltapos < tipdist,
    select2(absdeltapos < scale,
	  		0,
	  		ma.signum(deltapos)* -tipdist * k + Kend * deltapos + 
              z* deltavel
	  		),
	(k - Kend) * -deltapos + z* deltavel
	) <:  *(-1),_
with{
  deltapos = x1 - x2;
  deltavel = (x1 - x1' : initState(x1r0)) - (x2 - x2' : initState(x2r0));

  absdeltapos = abs(deltapos);
  sharpness = 10;
  tipdist = scale / sharpness;
  Kend = k / sharpness;
};


//------------------------`(mi.)nlBow`----------------------
// Implementation of a non-linear friction based interaction
// that allows for stick-slip bowing behaviour.
// Two versions are proposed : a piecewise linear function (very
// similar to the `nlPluck`) or a mathematical approximation (see
// Stefan Bilbao's book, Numerical Sound Synthesis).
//
//
// #### Usage
//
// ```
// nlBow(znl, scale, type, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `znl`: friction scaling parameter (vertical stretch of the NL function)
// * `scale`: velocity scaling parameter (horizontal stretch of the NL function)
// * `type`: interaction profile (0 = piecewise linear, 1 = smooth function)
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
nlBow(z, scale, type, x1r0, x2r0, x1, x2) =
  select2(type > 0,
    select2(absdeltavel < tipvel,
        select2(absdeltavel < scale,
	  		0,
	  		ma.signum(deltavel)* tipvel * z - Zend * deltavel
	  		),
	    (z - Zend) * deltavel
	),
    0.63 * z * deltavel *exp(-4*pow(deltavel/scale, 2) + 1/2)
  )
   <:  *(-1),_
with{
  deltavel = (x1 - x1' : initState(x1r0)) - (x2 - x2' : initState(x2r0));
  absdeltavel = abs(deltavel);
  sharpness = 3;
  tipvel = scale / sharpness;
  Zend = z / sharpness;
};


//------------------------`(mi.)collision`----------------------
// Implementation of a collision interaction, producing linear visco-elastic
// repulsion forces when two mass elements are interpenetrating.
//
//
// #### Usage
//
// ```
// collision(k, z, thres, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `k`: collision stiffness parameter
// * `z`: collision damping parameter
// * `thres`: threshold distance for the contact between elements
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
collision(k,z,thres,x1r0,x2r0,x1,x2) = 
  springDamper(k,z,x1r0,x2r0,x1+thres,x2) : (select2(comp,0,_),select2(comp,0,_))
with{
  comp = (x2-x1) < thres;
};


//------------------------`(mi.)nlCollisionClipped`----------------------
// Implementation of a collision interaction, producing non-linear
// visco-elastic repulsion forces when two mass elements are interpenetrating.
// Bound by an upper stiffness value to maintain stability.
// This interaction is particularly useful for more realistic contact dynamics
// (greater difference in velocity provides sharper contacts, and reciprocally).
//
// #### Usage
//
// ```
// nlCollisionClipped(s, c, k, z, thres, x1r, x2r),_,_ : _,_
// ```
//
// Where:
//
// * `s`: collision linear stiffness parameter
// * `c`: collision cubic stiffness parameter
// * `k`: collision upper-bounding stiffness parameter
// * `z`: collision damping parameter
// * `thres`: threshold distance for the contact between elements
// * `x1r`: initial delayed position of mass 1
// * `x2r`: initial delayed position of mass 2
//---------------------------------------------------------
nlCollisionClipped(s, c, k, z, thres, x1r0, x2r0, x1, x2) = 
  nlSpringDamperClipped(s,c,k,z,x1r0,x2r0,x1+thres,x2) : (select2(comp,0,_),select2(comp,0,_))
with{
  comp = (x2-x1) < thres;
};