diff --git a/cms/envs/common.py b/cms/envs/common.py
index 1767202141..f1440c7292 100644
--- a/cms/envs/common.py
+++ b/cms/envs/common.py
@@ -35,6 +35,7 @@ from path import path
MITX_FEATURES = {
'USE_DJANGO_PIPELINE': True,
'GITHUB_PUSH': False,
+ 'ENABLE_DISCUSSION_SERVICE': False
}
# needed to use lms student app
diff --git a/common/djangoapps/student/models.py b/common/djangoapps/student/models.py
index c37b9fce16..7e8658045e 100644
--- a/common/djangoapps/student/models.py
+++ b/common/djangoapps/student/models.py
@@ -282,6 +282,9 @@ def add_user_to_default_group(user, group):
@receiver(post_save, sender=User)
def update_user_information(sender, instance, created, **kwargs):
+ if not settings.MITX_FEATURES['ENABLE_DISCUSSION_SERVICE']:
+ # Don't try--it won't work, and it will fill the logs with lots of errors
+ return
try:
cc_user = cc.User.from_django_user(instance)
cc_user.save()
diff --git a/common/lib/xmodule/xmodule/course_module.py b/common/lib/xmodule/xmodule/course_module.py
index f00a22782c..7aa904205d 100644
--- a/common/lib/xmodule/xmodule/course_module.py
+++ b/common/lib/xmodule/xmodule/course_module.py
@@ -99,7 +99,14 @@ class CourseDescriptor(SequenceDescriptor):
def definition_from_xml(cls, xml_object, system):
textbooks = []
for textbook in xml_object.findall("textbook"):
- textbooks.append(cls.Textbook.from_xml_object(textbook))
+ try:
+ txt = cls.Textbook.from_xml_object(textbook)
+ except:
+ # If we can't get to S3 (e.g. on a train with no internet), don't break
+ # the rest of the courseware.
+ log.exception("Couldn't load textbook")
+ continue
+ textbooks.append(txt)
xml_object.remove(textbook)
#Load the wiki tag if it exists
diff --git a/common/lib/xmodule/xmodule/js/src/capa/schematic.js b/common/lib/xmodule/xmodule/js/src/capa/schematic.js
index 92bc32441b..e07b98d63c 100644
--- a/common/lib/xmodule/xmodule/js/src/capa/schematic.js
+++ b/common/lib/xmodule/xmodule/js/src/capa/schematic.js
@@ -1,3 +1,1963 @@
+//////////////////////////////////////////////////////////////////////////////
+//
+// Circuit simulator
+//
+//////////////////////////////////////////////////////////////////////////////
+
+// Copyright (C) 2011 Massachusetts Institute of Technology
+
+
+// create a circuit for simulation using "new cktsim.Circuit()"
+
+// for modified nodal analysis (MNA) stamps see
+// http://www.analog-electronics.eu/analog-electronics/modified-nodal-analysis/modified-nodal-analysis.xhtml
+
+cktsim = (function() {
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Circuit
+ //
+ //////////////////////////////////////////////////////////////////////////////
+
+ // types of "nodes" in the linear system
+ T_VOLTAGE = 0;
+ T_CURRENT = 1;
+
+ v_newt_lim = 0.3; // Voltage limited Newton great for Mos/diodes
+ v_abstol = 1e-6; // Absolute voltage error tolerance
+ i_abstol = 1e-12; // Absolute current error tolerance
+ eps = 1.0e-12; // A very small number compared to one.
+ dc_max_iters = 1000; // max iterations before giving pu
+ max_tran_iters = 20; // max iterations before giving up
+ time_step_increase_factor = 2.0; // How much can lte let timestep grow.
+ lte_step_decrease_factor = 8; // Limit lte one-iter timestep shrink.
+ nr_step_decrease_factor = 4; // Newton failure timestep shink.
+ reltol = 0.0001; // Relative tol to max observed value
+ lterel = 10; // LTE/Newton tolerance ratio (> 10!)
+ res_check_abs = Math.sqrt(i_abstol); // Loose Newton residue check
+ res_check_rel = Math.sqrt(reltol); // Loose Newton residue check
+
+ function Circuit() {
+ this.node_map = new Array();
+ this.ntypes = [];
+ this.initial_conditions = []; // ic's for each element
+
+ this.devices = []; // list of devices
+ this.device_map = new Array(); // map name -> device
+ this.voltage_sources = []; // list of voltage sources
+ this.current_sources = []; // list of current sources
+
+ this.finalized = false;
+ this.diddc = false;
+ this.node_index = -1;
+
+ this.periods = 1
+ }
+
+ // index of ground node
+ Circuit.prototype.gnd_node = function() {
+ return -1;
+ }
+
+ // allocate a new node index
+ Circuit.prototype.node = function(name,ntype,ic) {
+ this.node_index += 1;
+ if (name) this.node_map[name] = this.node_index;
+ this.ntypes.push(ntype);
+ this.initial_conditions.push(ic);
+ return this.node_index;
+ }
+
+ // call to finalize the circuit in preparation for simulation
+ Circuit.prototype.finalize = function() {
+ if (!this.finalized) {
+ this.finalized = true;
+ this.N = this.node_index + 1; // number of nodes
+
+ // give each device a chance to finalize itself
+ for (var i = this.devices.length - 1; i >= 0; --i)
+ this.devices[i].finalize(this);
+
+ // set up augmented matrix and various temp vectors
+ this.matrix = mat_make(this.N, this.N+1);
+ this.Gl = mat_make(this.N, this.N); // Matrix for linear conductances
+ this.G = mat_make(this.N, this.N); // Complete conductance matrix
+ this.C = mat_make(this.N, this.N); // Matrix for linear L's and C's
+
+ this.soln_max = new Array(this.N); // max abs value seen for each unknown
+ this.abstol = new Array(this.N);
+ this.solution = new Array(this.N);
+ this.rhs = new Array(this.N);
+ for (var i = this.N - 1; i >= 0; --i) {
+ this.soln_max[i] = 0.0;
+ this.abstol[i] = this.ntypes[i] == T_VOLTAGE ? v_abstol : i_abstol;
+ this.solution[i] = 0.0;
+ this.rhs[i] = 0.0;
+ }
+
+ // Load up the linear elements once and for all
+ for (var i = this.devices.length - 1; i >= 0; --i) {
+ this.devices[i].load_linear(this)
+ }
+
+ // Check for voltage source loops.
+ n_vsrc = this.voltage_sources.length;
+ if (n_vsrc > 0) { // At least one voltage source
+ var GV = mat_make(n_vsrc, this.N); // Loop check
+ for (var i = n_vsrc - 1; i >= 0; --i) {
+ var branch = this.voltage_sources[i].branch;
+ for (var j = this.N - 1; j >= 0; j--)
+ GV[i][j] = this.Gl[branch][j];
+ }
+ var rGV = mat_rank(GV);
+ if (rGV < n_vsrc) {
+ alert('Warning!!! Circuit has a voltage source loop or a source or current probe shorted by a wire, please remove the source or the wire causing the short.');
+ alert('Warning!!! Simulator might produce meaningless results or no result with illegal circuits.');
+ return false;
+ }
+ }
+ }
+ return true;
+ }
+
+ // load circuit from JSON netlist (see schematic.js)
+ Circuit.prototype.load_netlist = function(netlist) {
+ // set up mapping for all ground connections
+ for (var i = netlist.length - 1; i >= 0; --i) {
+ var component = netlist[i];
+ var type = component[0];
+ if (type == 'g') {
+ var connections = component[3];
+ this.node_map[connections[0]] = this.gnd_node();
+ }
+ }
+
+ // process each component in the JSON netlist (see schematic.js for format)
+ var found_ground = false;
+ for (var i = netlist.length - 1; i >= 0; --i) {
+ var component = netlist[i];
+ var type = component[0];
+
+ // ignore wires, ground connections, scope probes and view info
+ if (type == 'view' || type == 'w' || type == 'g' || type == 's' || type == 'L') {
+ continue;
+ }
+
+ var properties = component[2];
+ var name = properties['name'];
+ if (name==undefined || name=='')
+ name = '_' + properties['_json_'].toString();
+
+ // convert node names to circuit indicies
+ var connections = component[3];
+ for (var j = connections.length - 1; j >= 0; --j) {
+ var node = connections[j];
+ var index = this.node_map[node];
+ if (index == undefined) index = this.node(node,T_VOLTAGE);
+ else if (index == this.gnd_node()) found_ground = true;
+ connections[j] = index;
+ }
+
+ // process the component
+ if (type == 'r') // resistor
+ this.r(connections[0],connections[1],properties['r'],name);
+ else if (type == 'd') // diode
+ this.d(connections[0],connections[1],properties['area'],properties['type'],name);
+ else if (type == 'c') // capacitor
+ this.c(connections[0],connections[1],properties['c'],name);
+ else if (type == 'l') // inductor
+ this.l(connections[0],connections[1],properties['l'],name);
+ else if (type == 'v') // voltage source
+ this.v(connections[0],connections[1],properties['value'],name);
+ else if (type == 'i') // current source
+ this.i(connections[0],connections[1],properties['value'],name);
+ else if (type == 'o') // op amp
+ this.opamp(connections[0],connections[1],connections[2],connections[3],properties['A'],name);
+ else if (type == 'n') // n fet
+ this.n(connections[0],connections[1],connections[2],properties['W/L'],name);
+ else if (type == 'p') // p fet
+ this.p(connections[0],connections[1],connections[2],properties['W/L'],name);
+ else if (type == 'a') // current probe == 0-volt voltage source
+ this.v(connections[0],connections[1],'0',name);
+ }
+
+ if (!found_ground) { // No ground on schematic
+ alert('Please make at least one connection to ground (inverted T symbol)');
+ return false;
+ }
+ return true;
+
+ }
+
+ // if converges: updates this.solution, this.soln_max, returns iter count
+ // otherwise: return undefined and set this.problem_node
+ // Load should compute -f and df/dx (note the sign pattern!)
+ Circuit.prototype.find_solution = function(load,maxiters) {
+ var soln = this.solution;
+ var rhs = this.rhs;
+ var d_sol = new Array();
+ var abssum_compare;
+ var converged,abssum_old=0, abssum_rhs;
+ var use_limiting = false;
+ var down_count = 0;
+
+ // iteratively solve until values convere or iteration limit exceeded
+ for (var iter = 0; iter < maxiters; iter++) {
+ // set up equations
+ load(this,soln,rhs);
+
+ // Compute norm of rhs, assume variables of v type go with eqns of i type
+ abssum_rhs = 0;
+ for (var i = this.N - 1; i >= 0; --i)
+ if (this.ntypes[i] == T_VOLTAGE)
+ abssum_rhs += Math.abs(rhs[i]);
+
+ if ((iter > 0) && (use_limiting == false) && (abssum_old < abssum_rhs)) {
+ // Old rhsnorm was better, undo last iter and turn on limiting
+ for (var i = this.N - 1; i >= 0; --i)
+ soln[i] -= d_sol[i];
+ iter -= 1;
+ use_limiting = true;
+ }
+ else { // Compute the Newton delta
+ //d_sol = mat_solve(this.matrix,rhs);
+ d_sol = mat_solve_rq(this.matrix,rhs);
+
+ // If norm going down for ten iters, stop limiting
+ if (abssum_rhs < abssum_old)
+ down_count += 1;
+ else
+ down_count = 0;
+ if (down_count > 10) {
+ use_limiting = false;
+ down_count = 0;
+ }
+
+ // Update norm of rhs
+ abssum_old = abssum_rhs;
+ }
+
+ // Update the worst case abssum for comparison.
+ if ((iter == 0) || (abssum_rhs > abssum_compare))
+ abssum_compare = abssum_rhs;
+
+ // Check residue convergence, but loosely, and give up
+ // on last iteration
+ if ( (iter < (maxiters - 1)) &&
+ (abssum_rhs > (res_check_abs+res_check_rel*abssum_compare)))
+ converged = false;
+ else converged = true;
+
+
+ // Update solution and check delta convergence
+ for (var i = this.N - 1; i >= 0; --i) {
+ // Simple voltage step limiting to encourage Newton convergence
+ if (use_limiting) {
+ if (this.ntypes[i] == T_VOLTAGE) {
+ d_sol[i] = (d_sol[i] > v_newt_lim) ? v_newt_lim : d_sol[i];
+ d_sol[i] = (d_sol[i] < -v_newt_lim) ? -v_newt_lim : d_sol[i];
+ }
+ }
+ soln[i] += d_sol[i];
+ thresh = this.abstol[i] + reltol*this.soln_max[i];
+ if (Math.abs(d_sol[i]) > thresh) {
+ converged = false;
+ this.problem_node = i;
+ }
+ }
+
+ //alert(numeric.prettyPrint(this.solution);)
+ if (converged == true) {
+ for (var i = this.N - 1; i >= 0; --i)
+ if (Math.abs(soln[i]) > this.soln_max[i])
+ this.soln_max[i] = Math.abs(soln[i]);
+
+ return iter+1;
+ }
+ }
+ return undefined;
+ }
+
+ // DC analysis
+ Circuit.prototype.dc = function() {
+
+ // Allocation matrices for linear part, etc.
+ if (this.finalize() == false)
+ return undefined;
+
+ // Define -f and df/dx for Newton solver
+ function load_dc(ckt,soln,rhs) {
+ // rhs is initialized to -Gl * soln
+ mat_v_mult(ckt.Gl, soln, rhs, -1.0);
+ // G matrix is initialized with linear Gl
+ mat_copy(ckt.Gl,ckt.G);
+ // Now load up the nonlinear parts of rhs and G
+ for (var i = ckt.devices.length - 1; i >= 0; --i)
+ ckt.devices[i].load_dc(ckt,soln,rhs);
+ // G matrix is copied in to the system matrix
+ mat_copy(ckt.G,ckt.matrix);
+ }
+
+ // find the operating point
+ var iterations = this.find_solution(load_dc,dc_max_iters);
+
+ if (typeof iterations == 'undefined') {
+ // too many iterations
+ if (this.current_sources.length > 0) {
+ alert('Newton Method Failed, do your current sources have a conductive path to ground?');
+ } else {
+ alert('Newton Method Failed, it may be your circuit or it may be our simulator.');
+ }
+
+ return undefined
+ } else {
+ // Note that a dc solution was computed
+ this.diddc = true;
+ // create solution dictionary
+ var result = new Array();
+ // capture node voltages
+ for (var name in this.node_map) {
+ var index = this.node_map[name];
+ result[name] = (index == -1) ? 0 : this.solution[index];
+ }
+ // capture branch currents from voltage sources
+ for (var i = this.voltage_sources.length - 1; i >= 0; --i) {
+ var v = this.voltage_sources[i];
+ result['I('+v.name+')'] = this.solution[v.branch];
+ }
+ return result;
+ }
+ }
+
+ // Transient analysis (needs work!)
+ Circuit.prototype.tran = function(ntpts, tstart, tstop, probenames, no_dc) {
+
+ // Define -f and df/dx for Newton solver
+ function load_tran(ckt,soln,rhs) {
+ // Crnt is initialized to -Gl * soln
+ mat_v_mult(ckt.Gl, soln, ckt.c,-1.0);
+ // G matrix is initialized with linear Gl
+ mat_copy(ckt.Gl,ckt.G);
+ // Now load up the nonlinear parts of crnt and G
+ for (var i = ckt.devices.length - 1; i >= 0; --i)
+ ckt.devices[i].load_tran(ckt,soln,ckt.c,ckt.time);
+ // Exploit the fact that storage elements are linear
+ mat_v_mult(ckt.C, soln, ckt.q, 1.0);
+ // -rhs = c - dqdt
+ for (var i = ckt.N-1; i >= 0; --i) {
+ var dqdt = ckt.alpha0*ckt.q[i] + ckt.alpha1*ckt.oldq[i] +
+ ckt.alpha2*ckt.old2q[i];
+ //alert(numeric.prettyPrint(dqdt));
+ rhs[i] = ckt.beta0[i]*ckt.c[i] + ckt.beta1[i]*ckt.oldc[i] - dqdt;
+ }
+ // matrix = beta0*G + alpha0*C.
+ mat_scale_add(ckt.G,ckt.C,ckt.beta0,ckt.alpha0,ckt.matrix);
+ }
+
+ var p = new Array(3);
+ function interp_coeffs(t, t0, t1, t2) {
+ // Poly coefficients
+ var dtt0 = (t - t0);
+ var dtt1 = (t - t1);
+ var dtt2 = (t - t2);
+ var dt0dt1 = (t0 - t1);
+ var dt0dt2 = (t0 - t2);
+ var dt1dt2 = (t1 - t2);
+ p[0] = (dtt1*dtt2)/(dt0dt1 * dt0dt2);
+ p[1] = (dtt0*dtt2)/(-dt0dt1 * dt1dt2);
+ p[2] = (dtt0*dtt1)/(dt0dt2 * dt1dt2);
+ return p;
+ }
+
+ function pick_step(ckt, step_index) {
+ var min_shrink_factor = 1.0/lte_step_decrease_factor;
+ var max_growth_factor = time_step_increase_factor;
+ var N = ckt.N;
+ var p = interp_coeffs(ckt.time, ckt.oldt, ckt.old2t, ckt.old3t);
+ var trapcoeff = 0.5*(ckt.time - ckt.oldt)/(ckt.time - ckt.old3t);
+ var maxlteratio = 0.0;
+ for (var i = ckt.N-1; i >= 0; --i) {
+ if (ckt.ltecheck[i]) { // Check lte on variable
+ var pred = p[0]*ckt.oldsol[i] + p[1]*ckt.old2sol[i] + p[2]*ckt.old3sol[i];
+ var lte = Math.abs((ckt.solution[i] - pred))*trapcoeff;
+ var lteratio = lte/(lterel*(ckt.abstol[i] + reltol*ckt.soln_max[i]));
+ maxlteratio = Math.max(maxlteratio, lteratio);
+ }
+ }
+ var new_step;
+ var lte_step_ratio = 1.0/Math.pow(maxlteratio,1/3); // Cube root because trap
+ if (lte_step_ratio < 1.0) { // Shrink the timestep to make lte
+ lte_step_ratio = Math.max(lte_step_ratio,min_shrink_factor);
+ new_step = (ckt.time - ckt.oldt)*0.75*lte_step_ratio;
+ new_step = Math.max(new_step, ckt.min_step);
+ } else {
+ lte_step_ratio = Math.min(lte_step_ratio, max_growth_factor);
+ if (lte_step_ratio > 1.2) /* Increase timestep due to lte. */
+ new_step = (ckt.time - ckt.oldt) * lte_step_ratio / 1.2;
+ else
+ new_step = (ckt.time - ckt.oldt);
+ new_step = Math.min(new_step, ckt.max_step);
+ }
+ return new_step;
+ }
+
+ // Standard to do a dc analysis before transient
+ // Otherwise, do the setup also done in dc.
+ no_dc = false;
+ if ((this.diddc == false) && (no_dc == false)) {
+ if (this.dc() == undefined) { // DC failed, realloc mats and vects.
+ alert('DC failed, trying transient analysis from zero.');
+ this.finalized = false; // Reset the finalization.
+ if (this.finalize() == false)
+ return undefined;
+ }
+ }
+ else {
+ if (this.finalize() == false) // Allocate matrices and vectors.
+ return undefined;
+ }
+
+ // Tired of typing this, and using "with" generates hate mail.
+ var N = this.N;
+
+ // build array to hold list of results for each variable
+ // last entry is for timepoints.
+ var response = new Array(N + 1);
+ for (var i = N; i >= 0; --i) response[i] = new Array();
+
+ // Allocate back vectors for up to a second order method
+ this.old3sol = new Array(this.N);
+ this.old3q = new Array(this.N);
+ this.old2sol = new Array(this.N);
+ this.old2q = new Array(this.N);
+ this.oldsol = new Array(this.N);
+ this.oldq = new Array(this.N);
+ this.q = new Array(this.N);
+ this.oldc = new Array(this.N);
+ this.c = new Array(this.N);
+ this.alpha0 = 1.0;
+ this.alpha1 = 0.0;
+ this.alpha2 = 0.0;
+ this.beta0 = new Array(this.N);
+ this.beta1 = new Array(this.N);
+
+ // Mark a set of algebraic variable (don't miss hidden ones!).
+ this.ar = this.algebraic(this.C);
+
+ // Non-algebraic variables and probe variables get lte
+ this.ltecheck = new Array(this.N);
+ for (var i = N; i >= 0; --i)
+ this.ltecheck[i] = (this.ar[i] == 0);
+
+ for (var name in this.node_map) {
+ var index = this.node_map[name];
+ for (var i = probenames.length; i >= 0; --i) {
+ if (name == probenames[i]) {
+ this.ltecheck[index] = true;
+ break;
+ }
+ }
+ }
+
+ // Check for periodic sources
+ var period = tstop - tstart;
+ for (var i = this.voltage_sources.length - 1; i >= 0; --i) {
+ var per = this.voltage_sources[i].src.period;
+ if (per > 0)
+ period = Math.min(period, per);
+ }
+ for (var i = this.current_sources.length - 1; i >= 0; --i) {
+ var per = this.current_sources[i].src.period;
+ if (per > 0)
+ period = Math.min(period, per);
+ }
+ this.periods = Math.ceil((tstop - tstart)/period);
+ //alert('number of periods ' + this.periods);
+
+
+ this.time = tstart;
+ // ntpts adjusted by numbers of periods in input
+ this.max_step = (tstop - tstart)/(this.periods*ntpts);
+ this.min_step = this.max_step/1e8;
+ var new_step = this.max_step/1e6;
+ this.oldt = this.time - new_step;
+
+ // Initialize old crnts, charges, and solutions.
+ load_tran(this,this.solution,this.rhs)
+ for (var i = N-1; i >= 0; --i) {
+ this.old3sol[i] = this.solution[i];
+ this.old2sol[i] = this.solution[i];
+ this.oldsol[i] = this.solution[i];
+ this.old3q[i] = this.q[i];
+ this.old2q[i] = this.q[i];
+ this.oldq[i] = this.q[i];
+ this.oldc[i] = this.c[i];
+ }
+
+
+ var beta0,beta1;
+ // Start with two pseudo-Euler steps, maximum 50000 steps/period
+ var max_nsteps = this.periods*50000;
+ for(var step_index = -3; step_index < max_nsteps; step_index++) {
+ // Save the just computed solution, and move back q and c.
+ for (var i = this.N - 1; i >= 0; --i) {
+ if (step_index >= 0)
+ response[i].push(this.solution[i]);
+ this.oldc[i] = this.c[i];
+ this.old3sol[i] = this.old2sol[i];
+ this.old2sol[i] = this.oldsol[i];
+ this.oldsol[i] = this.solution[i];
+ this.old3q[i] = this.oldq[i];
+ this.old2q[i] = this.oldq[i];
+ this.oldq[i] = this.q[i];
+
+ }
+
+ if (step_index < 0) { // Take a prestep using BE
+ this.old3t = this.old2t - (this.oldt-this.old2t)
+ this.old2t = this.oldt - (tstart-this.oldt)
+ this.oldt = tstart - (this.time - this.oldt);
+ this.time = tstart;
+ beta0 = 1.0;
+ beta1 = 0.0;
+ } else { // Take a regular step
+ // Save the time, and rotate time wheel
+ response[this.N].push(this.time);
+ this.old3t = this.old2t;
+ this.old2t = this.oldt;
+ this.oldt = this.time;
+ // Make sure we come smoothly in to the interval end.
+ if (this.time >= tstop) break; // We're done.
+ else if(this.time + new_step > tstop)
+ this.time = tstop;
+ else if(this.time + 1.5*new_step > tstop)
+ this.time += (2/3)*(tstop - this.time);
+ else
+ this.time += new_step;
+
+ // Use trap (average old and new crnts.
+ beta0 = 0.5;
+ beta1 = 0.5;
+ }
+
+ // For trap rule, turn off current avging for algebraic eqns
+ for (var i = this.N - 1; i >= 0; --i) {
+ this.beta0[i] = beta0 + this.ar[i]*beta1;
+ this.beta1[i] = (1.0 - this.ar[i])*beta1;
+ }
+
+ // Loop to find NR converging timestep with okay LTE
+ while (true) {
+ // Set the timestep coefficients (alpha2 is for bdf2).
+ this.alpha0 = 1.0/(this.time - this.oldt);
+ this.alpha1 = -this.alpha0;
+ this.alpha2 = 0;
+
+ // If timestep is 1/10,000th of tstop, just use BE.
+ if ((this.time-this.oldt) < 1.0e-4*tstop) {
+ for (var i = this.N - 1; i >= 0; --i) {
+ this.beta0[i] = 1.0;
+ this.beta1[i] = 0.0;
+ }
+ }
+ // Use Newton to compute the solution.
+ var iterations = this.find_solution(load_tran,max_tran_iters);
+
+ // If NR succeeds and stepsize is at min, accept and newstep=maxgrowth*minstep.
+ // Else if Newton Fails, shrink step by a factor and try again
+ // Else LTE picks new step, if bigger accept current step and go on.
+ if ((iterations != undefined) &&
+ (step_index <= 0 || (this.time-this.oldt) < (1+reltol)*this.min_step)) {
+ if (step_index > 0) new_step = time_step_increase_factor*this.min_step;
+ break;
+ } else if (iterations == undefined) { // NR nonconvergence, shrink by factor
+ //alert('timestep nonconvergence ' + this.time + ' ' + step_index);
+ this.time = this.oldt +
+ (this.time - this.oldt)/nr_step_decrease_factor;
+ } else { // Check the LTE and shrink step if needed.
+ new_step = pick_step(this, step_index);
+ if (new_step < (1.0 - reltol)*(this.time - this.oldt)) {
+ this.time = this.oldt + new_step; // Try again
+ }
+ else
+ break; // LTE okay, new_step for next step
+ }
+ }
+ }
+
+ // create solution dictionary
+ var result = new Array();
+ for (var name in this.node_map) {
+ var index = this.node_map[name];
+ result[name] = (index == -1) ? 0 : response[index];
+ }
+ // capture branch currents from voltage sources
+ for (var i = this.voltage_sources.length - 1; i >= 0; --i) {
+ var v = this.voltage_sources[i];
+ result['I('+v.name+')'] = response[v.branch];
+ }
+
+ result['_time_'] = response[this.N];
+ return result;
+ }
+
+ // AC analysis: npts/decade for freqs in range [fstart,fstop]
+ // result['_frequencies_'] = vector of log10(sample freqs)
+ // result['xxx'] = vector of dB(response for node xxx)
+ // NOTE: Normalization removed in schematic.js, jkw.
+ Circuit.prototype.ac = function(npts,fstart,fstop,source_name) {
+
+ if (this.dc() == undefined) { // DC failed, realloc mats and vects.
+ return undefined;
+ }
+
+ var N = this.N;
+ var G = this.G;
+ var C = this.C;
+
+ // Complex numbers, we're going to need a bigger boat
+ var matrixac = mat_make(2*N, (2*N)+1);
+
+ // Get the source used for ac
+ if (this.device_map[source_name] === undefined) {
+ alert('AC analysis refers to unknown source ' + source_name);
+ return 'AC analysis failed, unknown source';
+ }
+ this.device_map[source_name].load_ac(this,this.rhs);
+
+ // build array to hold list of magnitude and phases for each node
+ // last entry is for frequency values
+ var response = new Array(2*N + 1);
+ for (var i = 2*N; i >= 0; --i) response[i] = new Array();
+
+ // multiplicative frequency increase between freq points
+ var delta_f = Math.exp(Math.LN10/npts);
+
+ var phase_offset = new Array(N);
+ for (var i = N-1; i >= 0; --i) phase_offset[i] = 0;
+
+ var f = fstart;
+ fstop *= 1.0001; // capture that last freq point!
+ while (f <= fstop) {
+ var omega = 2 * Math.PI * f;
+ response[2*N].push(f); // 2*N for magnitude and phase
+
+ // Find complex x+jy that sats Gx-omega*Cy=rhs; omega*Cx+Gy=0
+ // Note: solac[0:N-1]=x, solac[N:2N-1]=y
+ for (var i = N-1; i >= 0; --i) {
+ // First the rhs, replicated for real and imaginary
+ matrixac[i][2*N] = this.rhs[i];
+ matrixac[i+N][2*N] = 0;
+
+ for (var j = N-1; j >= 0; --j) {
+ matrixac[i][j] = G[i][j];
+ matrixac[i+N][j+N] = G[i][j];
+ matrixac[i][j+N] = -omega*C[i][j];
+ matrixac[i+N][j] = omega*C[i][j];
+ }
+ }
+
+ // Compute the small signal response
+ var solac = mat_solve(matrixac);
+
+ // Save magnitude and phase
+ for (var i = N - 1; i >= 0; --i) {
+ var mag = Math.sqrt(solac[i]*solac[i] + solac[i+N]*solac[i+N]);
+ response[i].push(mag);
+
+ // Avoid wrapping phase, add or sub 180 for each jump
+ var phase = 180*(Math.atan2(solac[i+N],solac[i])/Math.PI);
+ var phasei = response[i+N];
+ var L = phasei.length;
+ // Look for a one-step jump greater than 90 degrees
+ if (L > 1) {
+ var phase_jump = phase + phase_offset[i] - phasei[L-1];
+ if (phase_jump > 90) {
+ phase_offset[i] -= 360;
+ } else if (phase_jump < -90) {
+ phase_offset[i] += 360;
+ }
+ }
+ response[i+N].push(phase + phase_offset[i]);
+ }
+ f *= delta_f; // increment frequency
+ }
+
+ // create solution dictionary
+ var result = new Array();
+ for (var name in this.node_map) {
+ var index = this.node_map[name];
+ result[name] = (index == -1) ? 0 : response[index];
+ result[name+'_phase'] = (index == -1) ? 0 : response[index+N];
+ }
+ result['_frequencies_'] = response[2*N];
+ return result;
+ }
+
+
+ // Helper for adding devices to a circuit, warns on duplicate device names.
+ Circuit.prototype.add_device = function(d,name) {
+ // Add device to list of devices and to device map
+ this.devices.push(d);
+ d.name = name;
+ if (name) {
+ if (this.device_map[name] === undefined)
+ this.device_map[name] = d;
+ else {
+ alert('Warning: two circuit elements share the same name ' + name);
+ this.device_map[name] = d;
+ }
+ }
+ return d;
+ }
+
+ Circuit.prototype.r = function(n1,n2,v,name) {
+ // try to convert string value into numeric value, barf if we can't
+ if ((typeof v) == 'string') {
+ v = parse_number(v,undefined);
+ if (v === undefined) return undefined;
+ }
+
+ if (v != 0) {
+ var d = new Resistor(n1,n2,v);
+ return this.add_device(d, name);
+ } else return this.v(n1,n2,'0',name); // zero resistance == 0V voltage source
+ }
+
+ Circuit.prototype.d = function(n1,n2,area,type,name) {
+ // try to convert string value into numeric value, barf if we can't
+ if ((typeof area) == 'string') {
+ area = parse_number(area,undefined);
+ if (area === undefined) return undefined;
+ }
+
+ if (area != 0) {
+ var d = new Diode(n1,n2,area,type);
+ return this.add_device(d, name);
+ } // zero area diodes discarded.
+ }
+
+
+ Circuit.prototype.c = function(n1,n2,v,name) {
+ // try to convert string value into numeric value, barf if we can't
+ if ((typeof v) == 'string') {
+ v = parse_number(v,undefined);
+ if (v === undefined) return undefined;
+ }
+ var d = new Capacitor(n1,n2,v);
+ return this.add_device(d, name);
+ }
+
+ Circuit.prototype.l = function(n1,n2,v,name) {
+ // try to convert string value into numeric value, barf if we can't
+ if ((typeof v) == 'string') {
+ v = parse_number(v,undefined);
+ if (v === undefined) return undefined;
+ }
+ var branch = this.node(undefined,T_CURRENT);
+ var d = new Inductor(n1,n2,branch,v);
+ return this.add_device(d, name);
+ }
+
+ Circuit.prototype.v = function(n1,n2,v,name) {
+ var branch = this.node(undefined,T_CURRENT);
+ var d = new VSource(n1,n2,branch,v);
+ this.voltage_sources.push(d);
+ return this.add_device(d, name);
+ }
+
+ Circuit.prototype.i = function(n1,n2,v,name) {
+ var d = new ISource(n1,n2,v);
+ this.current_sources.push(d);
+ return this.add_device(d, name);
+ }
+
+ Circuit.prototype.opamp = function(np,nn,no,ng,A,name) {
+ // try to convert string value into numeric value, barf if we can't
+ if ((typeof A) == 'string') {
+ ratio = parse_number(A,undefined);
+ if (A === undefined) return undefined;
+ }
+ var branch = this.node(undefined,T_CURRENT);
+ var d = new Opamp(np,nn,no,ng,branch,A,name);
+ return this.add_device(d, name);
+ }
+
+ Circuit.prototype.n = function(d,g,s, ratio, name) {
+ // try to convert string value into numeric value, barf if we can't
+ if ((typeof ratio) == 'string') {
+ ratio = parse_number(ratio,undefined);
+ if (ratio === undefined) return undefined;
+ }
+ var d = new Fet(d,g,s,ratio,name,'n');
+ return this.add_device(d, name);
+ }
+
+ Circuit.prototype.p = function(d,g,s, ratio, name) {
+ // try to convert string value into numeric value, barf if we can't
+ if ((typeof ratio) == 'string') {
+ ratio = parse_number(ratio,undefined);
+ if (ratio === undefined) return undefined;
+ }
+ var d = new Fet(d,g,s,ratio,name,'p');
+ return this.add_device(d, name);
+ }
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Support for creating conductance and capacitance matrices associated with
+ // modified nodal analysis (unknowns are node voltages and inductor and voltage
+ // source currents).
+ // The linearized circuit is written as
+ // C d/dt x = G x + rhs
+ // x - vector of node voltages and element currents
+ // rhs - vector of source values
+ // C - Matrix whose values are capacitances and inductances, has many zero rows.
+ // G - Matrix whose values are conductances and +-1's.
+ //
+ ////////////////////////////////////////////////////////////////////////////////
+
+ // add val component between two nodes to matrix M
+ // Index of -1 refers to ground node
+ Circuit.prototype.add_two_terminal = function(i,j,g,M) {
+ if (i >= 0) {
+ M[i][i] += g;
+ if (j >= 0) {
+ M[i][j] -= g;
+ M[j][i] -= g;
+ M[j][j] += g;
+ }
+ } else if (j >= 0)
+ M[j][j] += g;
+ }
+
+ // add val component between two nodes to matrix M
+ // Index of -1 refers to ground node
+ Circuit.prototype.get_two_terminal = function(i,j,x) {
+ var xi_minus_xj = 0;
+ if (i >= 0) xi_minus_xj = x[i];
+ if (j >= 0) xi_minus_xj -= x[j];
+ return xi_minus_xj
+ }
+
+ Circuit.prototype.add_conductance_l = function(i,j,g) {
+ this.add_two_terminal(i,j,g, this.Gl)
+ }
+
+ Circuit.prototype.add_conductance = function(i,j,g) {
+ this.add_two_terminal(i,j,g, this.G)
+ }
+
+ Circuit.prototype.add_capacitance = function(i,j,c) {
+ this.add_two_terminal(i,j,c,this.C)
+ }
+
+ // add individual conductance to Gl matrix
+ Circuit.prototype.add_to_Gl = function(i,j,g) {
+ if (i >=0 && j >= 0)
+ this.Gl[i][j] += g;
+ }
+
+ // add individual conductance to Gl matrix
+ Circuit.prototype.add_to_G = function(i,j,g) {
+ if (i >=0 && j >= 0)
+ this.G[i][j] += g;
+ }
+
+ // add individual capacitance to C matrix
+ Circuit.prototype.add_to_C = function(i,j,c) {
+ if (i >=0 && j >= 0)
+ this.C[i][j] += c;
+ }
+
+ // add source info to rhs
+ Circuit.prototype.add_to_rhs = function(i,v,rhs) {
+ if (i >= 0) rhs[i] += v;
+ }
+
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Generic matrix support - making, copying, factoring, rank, etc
+ // Note, Matrices are stored using nested javascript arrays.
+ ////////////////////////////////////////////////////////////////////////////////
+
+ // Allocate an NxM matrix
+ function mat_make(N,M) {
+ var mat = new Array(N);
+ for (var i = N - 1; i >= 0; --i) {
+ mat[i] = new Array(M);
+ for (var j = M - 1; j >= 0; --j) {
+ mat[i][j] = 0.0;
+ }
+ }
+ return mat;
+ }
+
+ // Form b = scale*Mx
+ function mat_v_mult(M,x,b,scale) {
+ var n = M.length;
+ var m = M[0].length;
+
+ if (n != b.length || m != x.length)
+ throw 'Rows of M mismatched to b or cols mismatch to x.';
+
+ for (var i = 0; i < n; i++) {
+ var temp = 0;
+ for (var j = 0; j < m; j++) temp += M[i][j]*x[j];
+ b[i] = scale*temp; // Recall the neg in the name
+ }
+ }
+
+ // C = scalea*A + scaleb*B, scalea, scaleb eithers numbers or arrays (row scaling)
+ function mat_scale_add(A, B, scalea, scaleb, C) {
+ var n = A.length;
+ var m = A[0].length;
+
+ if (n > B.length || m > B[0].length)
+ throw 'Row or columns of A to large for B';
+ if (n > C.length || m > C[0].length)
+ throw 'Row or columns of A to large for C';
+ if ((typeof scalea == 'number') && (typeof scaleb == 'number'))
+ for (var i = 0; i < n; i++)
+ for (var j = 0; j < m; j++)
+ C[i][j] = scalea*A[i][j] + scaleb*B[i][j];
+ else if ((typeof scaleb == 'number') && (scalea instanceof Array))
+ for (var i = 0; i < n; i++)
+ for (var j = 0; j < m; j++)
+ C[i][j] = scalea[i]*A[i][j] + scaleb*B[i][j];
+ else if ((typeof scaleb instanceof Array) && (scalea instanceof Array))
+ for (var i = 0; i < n; i++)
+ for (var j = 0; j < m; j++)
+ C[i][j] = scalea[i]*A[i][j] + scaleb[i]*B[i][j];
+ else
+ throw 'scalea and scaleb must be scalars or Arrays';
+ }
+
+ // Returns a vector of ones and zeros, ones denote algebraic
+ // variables (rows that can be removed without changing rank(M).
+ Circuit.prototype.algebraic = function(M) {
+ var Nr = M.length
+ Mc = mat_make(Nr, Nr);
+ mat_copy(M,Mc);
+ var R = mat_rank(Mc);
+
+ var one_if_alg = new Array(Nr);
+ for (var row = 0; row < Nr; row++) { // psuedo gnd row small
+ for (var col = Nr - 1; col >= 0; --col)
+ Mc[row][col] = 0;
+ if (mat_rank(Mc) == R) // Zeroing row left rank unchanged
+ one_if_alg[row] = 1;
+ else { // Zeroing row changed rank, put back
+ for (var col = Nr - 1; col >= 0; --col)
+ Mc[row][col] = M[row][col];
+ one_if_alg[row] = 0;
+ }
+ }
+ return one_if_alg;
+ }
+
+ // Copy A -> using the bounds of A
+ function mat_copy(src,dest) {
+ var n = src.length;
+ var m = src[0].length;
+ if (n > dest.length || m > dest[0].length)
+ throw 'Rows or cols > rows or cols of dest';
+
+ for (var i = 0; i < n; i++)
+ for (var j = 0; j < m; j++)
+ dest[i][j] = src[i][j];
+ }
+
+ // Copy and transpose A -> using the bounds of A
+ function mat_copy_transposed(src,dest) {
+ var n = src.length;
+ var m = src[0].length;
+ if (n > dest[0].length || m > dest.length)
+ throw 'Rows or cols > cols or rows of dest';
+
+ for (var i = 0; i < n; i++)
+ for (var j = 0; j < m; j++)
+ dest[j][i] = src[i][j];
+ }
+
+
+ // Uses GE to determine rank.
+ function mat_rank(Mo) {
+ var Nr = Mo.length; // Number of rows
+ var Nc = Mo[0].length; // Number of columns
+ var temp,i,j;
+ // Make a copy to avoid overwriting
+ M = mat_make(Nr, Nc);
+ mat_copy(Mo,M);
+
+ // Find matrix maximum entry
+ var max_abs_entry = 0;
+ for(var row = Nr-1; row >= 0; --row) {
+ for(var col = Nr-1; col >= 0; --col) {
+ if (Math.abs(M[row][col]) > max_abs_entry)
+ max_abs_entry = Math.abs(M[row][col]);
+ }
+ }
+
+ // Gaussian elimination to find rank
+ var the_rank = 0;
+ var start_col = 0;
+ for (var row = 0; row < Nr; row++) {
+ // Search for first nonzero column in the remaining rows.
+ for (var col = start_col; col < Nc; col++) {
+ var max_v = Math.abs(M[row][col]);
+ var max_row = row;
+ for (var i = row + 1; i < Nr; i++) {
+ temp = Math.abs(M[i][col]);
+ if (temp > max_v) { max_v = temp; max_row = i; }
+ }
+ // if max_v non_zero, column is nonzero, eliminate in subsequent rows
+ if (Math.abs(max_v) > eps*max_abs_entry) {
+ start_col = col+1;
+ the_rank += 1;
+ // Swap rows to get max in M[row][col]
+ temp = M[row];
+ M[row] = M[max_row];
+ M[max_row] = temp;
+
+ // now eliminate this column for all subsequent rows
+ for (var i = row + 1; i < Nr; i++) {
+ temp = M[i][col]/M[row][col]; // multiplier for current row
+ if (temp != 0) // subtract
+ for (var j = col; j < Nc; j++) M[i][j] -= M[row][j]*temp;
+ }
+ // Now move on to the next row
+ break;
+ }
+ }
+ }
+
+ // return the rank
+ return the_rank;
+ }
+
+ // Solve Mx=b and return vector x using R^TQ^T factorization.
+ // Multiplication by R^T implicit, should be null-space free soln.
+ // M should have the extra column!
+ // Almost everything is in-lined for speed, sigh.
+ function mat_solve_rq(M, rhs) {
+
+ var Nr = M.length; // Number of rows
+ var Nc = M[0].length; // Number of columns
+
+ // Copy the rhs in to the last column of M if one is given.
+ if (rhs != null) {
+ for (var row = Nr - 1; row >= 0; --row)
+ M[row][Nc-1] = rhs[row];
+ }
+
+ var mat_scale = 0; // Sets the scale for comparison to zero.
+ var max_nonzero_row = Nr-1; // Assumes M nonsingular.
+ for (var row = 0; row < Nr; row++) {
+ // Find largest row with largest 2-norm
+ var max_row = row;
+ var maxsumsq = 0;
+ for (var rowp = row; rowp < Nr; rowp++) {
+ var Mr = M[rowp];
+ var sumsq = 0;
+ for (var col = Nc-2; col >= 0; --col) // Last col=rhs
+ sumsq += Mr[col]*Mr[col];
+ if ((row == rowp) || (sumsq > maxsumsq)) {
+ max_row = rowp;
+ maxsumsq = sumsq;
+ }
+ }
+ if (max_row > row) { // Swap rows if not max row
+ var temp = M[row];
+ M[row] = M[max_row];
+ M[max_row] = temp;
+ }
+
+ // Calculate row norm, save if this is first (largest)
+ row_norm = Math.sqrt(maxsumsq);
+ if (row == 0) mat_scale = row_norm;
+
+ // Check for all zero rows
+ if (row_norm > mat_scale*eps)
+ scale = 1.0/row_norm;
+ else {
+ max_nonzero_row = row - 1; // Rest will be nullspace of M
+ break;
+ }
+
+
+ // Nonzero row, eliminate from rows below
+ var Mr = M[row];
+ for (var col = Nc-1; col >= 0; --col) // Scale rhs also
+ Mr[col] *= scale;
+ for (var rowp = row + 1; rowp < Nr; rowp++) { // Update.
+ var Mrp = M[rowp];
+ var inner = 0;
+ for (var col = Nc-2; col >= 0; --col) // Project
+ inner += Mr[col]*Mrp[col];
+ for (var col = Nc-1; col >= 0; --col) // Ortho (rhs also)
+ Mrp[col] -= inner *Mr[col];
+ }
+ }
+
+ // Last Column of M has inv(R^T)*rhs. Scale rows of Q to get x.
+ var x = new Array(Nc-1);
+ for (var col = Nc-2; col >= 0; --col)
+ x[col] = 0;
+ for (var row = max_nonzero_row; row >= 0; --row) {
+ Mr = M[row];
+ for (var col = Nc-2; col >= 0; --col) {
+ x[col] += Mr[col]*Mr[Nc-1];
+ }
+ }
+
+ // Return solution.
+ return x;
+ }
+
+ // solve Mx=b and return vector x given augmented matrix M = [A | b]
+ // Uses Gaussian elimination with partial pivoting
+ function mat_solve(M,rhs) {
+ var N = M.length; // augmented matrix M has N rows, N+1 columns
+ var temp,i,j;
+
+ // Copy the rhs in to the last column of M if one is given.
+ if (rhs != null) {
+ for (var row = 0; row < N ; row++)
+ M[row][N] = rhs[row];
+ }
+
+ // gaussian elimination
+ for (var col = 0; col < N ; col++) {
+ // find pivot: largest abs(v) in this column of remaining rows
+ var max_v = Math.abs(M[col][col]);
+ var max_col = col;
+ for (i = col + 1; i < N; i++) {
+ temp = Math.abs(M[i][col]);
+ if (temp > max_v) { max_v = temp; max_col = i; }
+ }
+
+ // if no value found, generate a small conductance to gnd
+ // otherwise swap current row with pivot row
+ if (max_v == 0) M[col][col] = eps;
+ else {
+ temp = M[col];
+ M[col] = M[max_col];
+ M[max_col] = temp;
+ }
+
+ // now eliminate this column for all subsequent rows
+ for (i = col + 1; i < N; i++) {
+ temp = M[i][col]/M[col][col]; // multiplier we'll use for current row
+ if (temp != 0)
+ // subtract current row from row we're working on
+ // remember to process b too!
+ for (j = col; j <= N; j++) M[i][j] -= M[col][j]*temp;
+ }
+ }
+
+ // matrix is now upper triangular, so solve for elements of x starting
+ // with the last row
+ var x = new Array(N);
+ for (i = N-1; i >= 0; --i) {
+ temp = M[i][N]; // grab b[i] from augmented matrix as RHS
+ // subtract LHS term from RHS using known x values
+ for (j = N-1; j > i; --j) temp -= M[i][j]*x[j];
+ // now compute new x value
+ x[i] = temp/M[i][i];
+ }
+
+ // return solution
+ return x;
+ }
+
+ // test solution code, expect x = [2,3,-1]
+ //M = [[2,1,-1,8],[-3,-1,2,-11],[-2,1,2,-3]];
+ //x = mat_solve(M);
+ //y = 1; // so we have place to set a breakpoint :)
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Device base class
+ //
+ ////////////////////////////////////////////////////////////////////////////////
+
+ function Device() {
+ }
+
+ // complete initial set up of device
+ Device.prototype.finalize = function() {
+ }
+
+ // Load the linear elements in to Gl and C
+ Device.prototype.load_linear = function(ckt) {
+ }
+
+ // load linear system equations for dc analysis
+ // (inductors shorted and capacitors opened)
+ Device.prototype.load_dc = function(ckt,soln,rhs) {
+ }
+
+ // load linear system equations for tran analysis
+ Device.prototype.load_tran = function(ckt,soln) {
+ }
+
+ // load linear system equations for ac analysis:
+ // current sources open, voltage sources shorted
+ // linear models at operating point for everyone else
+ Device.prototype.load_ac = function(ckt,rhs) {
+ }
+
+ // return time of next breakpoint for the device
+ Device.prototype.breakpoint = function(time) {
+ return undefined;
+ }
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Parse numbers in engineering notation
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ // convert first character of argument into an integer
+ function ord(ch) {
+ return ch.charCodeAt(0);
+ }
+
+ // convert string argument to a number, accepting usual notations
+ // (hex, octal, binary, decimal, floating point) plus engineering
+ // scale factors (eg, 1k = 1000.0 = 1e3).
+ // return default if argument couldn't be interpreted as a number
+ function parse_number(s,default_v) {
+ var slen = s.length;
+ var multiplier = 1;
+ var result = 0;
+ var index = 0;
+
+ // skip leading whitespace
+ while (index < slen && s.charAt(index) <= ' ') index += 1;
+ if (index == slen) return default_v;
+
+ // check for leading sign
+ if (s.charAt(index) == '-') {
+ multiplier = -1;
+ index += 1;
+ } else if (s.charAt(index) == '+')
+ index += 1;
+ var start = index; // remember where digits start
+
+ // if leading digit is 0, check for hex, octal or binary notation
+ if (index >= slen) return default_v;
+ else if (s.charAt(index) == '0') {
+ index += 1;
+ if (index >= slen) return 0;
+ if (s.charAt(index) == 'x' || s.charAt(index) == 'X') { // hex
+ while (true) {
+ index += 1;
+ if (index >= slen) break;
+ if (s.charAt(index) >= '0' && s.charAt(index) <= '9')
+ result = result*16 + ord(s.charAt(index)) - ord('0');
+ else if (s.charAt(index) >= 'A' && s.charAt(index) <= 'F')
+ result = result*16 + ord(s.charAt(index)) - ord('A') + 10;
+ else if (s.charAt(index) >= 'a' && s.charAt(index) <= 'f')
+ result = result*16 + ord(s.charAt(index)) - ord('a') + 10;
+ else break;
+ }
+ return result*multiplier;
+ } else if (s.charAt(index) == 'b' || s.charAt(index) == 'B') { // binary
+ while (true) {
+ index += 1;
+ if (index >= slen) break;
+ if (s.charAt(index) >= '0' && s.charAt(index) <= '1')
+ result = result*2 + ord(s.charAt(index)) - ord('0');
+ else break;
+ }
+ return result*multiplier;
+ } else if (s.charAt(index) != '.') { // octal
+ while (true) {
+ if (s.charAt(index) >= '0' && s.charAt(index) <= '7')
+ result = result*8 + ord(s.charAt(index)) - ord('0');
+ else break;
+ index += 1;
+ if (index >= slen) break;
+ }
+ return result*multiplier;
+ }
+ }
+
+ // read decimal integer or floating-point number
+ while (true) {
+ if (s.charAt(index) >= '0' && s.charAt(index) <= '9')
+ result = result*10 + ord(s.charAt(index)) - ord('0');
+ else break;
+ index += 1;
+ if (index >= slen) break;
+ }
+
+ // fractional part?
+ if (index < slen && s.charAt(index) == '.') {
+ while (true) {
+ index += 1;
+ if (index >= slen) break;
+ if (s.charAt(index) >= '0' && s.charAt(index) <= '9') {
+ result = result*10 + ord(s.charAt(index)) - ord('0');
+ multiplier *= 0.1;
+ } else break;
+ }
+ }
+
+ // if we haven't seen any digits yet, don't check
+ // for exponents or scale factors
+ if (index == start) return default_v;
+
+ // type of multiplier determines type of result:
+ // multiplier is a float if we've seen digits past
+ // a decimal point, otherwise it's an int or long.
+ // Up to this point result is an int or long.
+ result *= multiplier;
+
+ // now check for exponent or engineering scale factor. If there
+ // is one, result will be a float.
+ if (index < slen) {
+ var scale = s.charAt(index);
+ index += 1;
+ if (scale == 'e' || scale == 'E') {
+ var exponent = 0;
+ multiplier = 10.0;
+ if (index < slen) {
+ if (s.charAt(index) == '+') index += 1;
+ else if (s.charAt(index) == '-') {
+ index += 1;
+ multiplier = 0.1;
+ }
+ }
+ while (index < slen) {
+ if (s.charAt(index) >= '0' && s.charAt(index) <= '9') {
+ exponent = exponent*10 + ord(s.charAt(index)) - ord('0');
+ index += 1;
+ } else break;
+ }
+ while (exponent > 0) {
+ exponent -= 1;
+ result *= multiplier;
+ }
+ } else if (scale == 't' || scale == 'T') result *= 1e12;
+ else if (scale == 'g' || scale == 'G') result *= 1e9;
+ else if (scale == 'M') result *= 1e6;
+ else if (scale == 'k' || scale == 'K') result *= 1e3;
+ else if (scale == 'm') result *= 1e-3;
+ else if (scale == 'u' || scale == 'U') result *= 1e-6;
+ else if (scale == 'n' || scale == 'N') result *= 1e-9;
+ else if (scale == 'p' || scale == 'P') result *= 1e-12;
+ else if (scale == 'f' || scale == 'F') result *= 1e-15;
+ }
+ // ignore any remaining chars, eg, 1kohms returns 1000
+ return result;
+ }
+
+ Circuit.prototype.parse_number = parse_number; // make it easy to call from outside
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Sources
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ // argument is a string describing the source's value (see comments for details)
+ // source types: dc,step,square,triangle,sin,pulse,pwl,pwl_repeating
+
+ // returns an object with the following attributes:
+ // fun -- name of source function
+ // args -- list of argument values
+ // value(t) -- compute source value at time t
+ // inflection_point(t) -- compute time after t when a time point is needed
+ // dc -- value at time 0
+ // period -- repeat period for periodic sources (0 if not periodic)
+
+ function parse_source(v) {
+ // generic parser: parse v as either or (,...)
+ var src = new Object();
+ src.period = 0; // Default not periodic
+ src.value = function(t) { return 0; } // overridden below
+ src.inflection_point = function(t) { return undefined; }; // may be overridden below
+
+ // see if there's a "(" in the description
+ var index = v.indexOf('(');
+ var ch;
+ if (index >= 0) {
+ src.fun = v.slice(0,index); // function name is before the "("
+ src.args = []; // we'll push argument values onto this list
+ var end = v.indexOf(')',index);
+ if (end == -1) end = v.length;
+
+ index += 1; // start parsing right after "("
+ while (index < end) {
+ // figure out where next argument value starts
+ ch = v.charAt(index);
+ if (ch <= ' ') { index++; continue; }
+ // and where it ends
+ var arg_end = v.indexOf(',',index);
+ if (arg_end == -1) arg_end = end;
+ // parse and save result in our list of arg values
+ src.args.push(parse_number(v.slice(index,arg_end),undefined));
+ index = arg_end + 1;
+ }
+ } else {
+ src.fun = 'dc';
+ src.args = [parse_number(v,0)];
+ }
+
+ // post-processing for constant sources
+ // dc(v)
+ if (src.fun == 'dc') {
+ var v = arg_value(src.args,0,0);
+ src.args = [v];
+ src.value = function(t) { return v; } // closure
+ }
+
+ // post-processing for impulse sources
+ // impulse(height,width)
+ else if (src.fun == 'impulse') {
+ var h = arg_value(src.args,0,1); // default height: 1
+ var w = Math.abs(arg_value(src.args,2,1e-9)); // default width: 1ns
+ src.args = [h,w]; // remember any defaulted values
+ pwl_source(src,[0,0,w/2,h,w,0],false);
+ }
+
+ // post-processing for step sources
+ // step(v_init,v_plateau,t_delay,t_rise)
+ else if (src.fun == 'step') {
+ var v1 = arg_value(src.args,0,0); // default init value: 0V
+ var v2 = arg_value(src.args,1,1); // default plateau value: 1V
+ var td = Math.max(0,arg_value(src.args,2,0)); // time step starts
+ var tr = Math.abs(arg_value(src.args,3,1e-9)); // default rise time: 1ns
+ src.args = [v1,v2,td,tr]; // remember any defaulted values
+ pwl_source(src,[td,v1,td+tr,v2],false);
+ }
+
+ // post-processing for square wave
+ // square(v_init,v_plateau,freq,duty_cycle)
+ else if (src.fun == 'square') {
+ var v1 = arg_value(src.args,0,0); // default init value: 0V
+ var v2 = arg_value(src.args,1,1); // default plateau value: 1V
+ var freq = Math.abs(arg_value(src.args,2,1)); // default frequency: 1Hz
+ var duty_cycle = Math.min(100,Math.abs(arg_value(src.args,3,50))); // default duty cycle: 0.5
+ src.args = [v1,v2,freq,duty_cycle]; // remember any defaulted values
+
+ var per = freq == 0 ? Infinity : 1/freq;
+ var t_change = 0.01 * per; // rise and fall time
+ var t_pw = .01 * duty_cycle * 0.98 * per; // fraction of cycle minus rise and fall time
+ pwl_source(src,[0,v1,t_change,v2,t_change+t_pw,
+ v2,t_change+t_pw+t_change,v1,per,v1],true);
+ }
+
+ // post-processing for triangle
+ // triangle(v_init,v_plateua,t_period)
+ else if (src.fun == 'triangle') {
+ var v1 = arg_value(src.args,0,0); // default init value: 0V
+ var v2 = arg_value(src.args,1,1); // default plateau value: 1V
+ var freq = Math.abs(arg_value(src.args,2,1)); // default frequency: 1s
+ src.args = [v1,v2,freq]; // remember any defaulted values
+
+ var per = freq == 0 ? Infinity : 1/freq;
+ pwl_source(src,[0,v1,per/2,v2,per,v1],true);
+ }
+
+ // post-processing for pwl and pwlr sources
+ // pwl[r](t1,v1,t2,v2,...)
+ else if (src.fun == 'pwl' || src.fun == 'pwl_repeating') {
+ pwl_source(src,src.args,src.fun == 'pwl_repeating');
+ }
+
+ // post-processing for pulsed sources
+ // pulse(v_init,v_plateau,t_delay,t_rise,t_fall,t_width,t_period)
+ else if (src.fun == 'pulse') {
+ var v1 = arg_value(src.args,0,0); // default init value: 0V
+ var v2 = arg_value(src.args,1,1); // default plateau value: 1V
+ var td = Math.max(0,arg_value(src.args,2,0)); // time pulse starts
+ var tr = Math.abs(arg_value(src.args,3,1e-9)); // default rise time: 1ns
+ var tf = Math.abs(arg_value(src.args,4,1e-9)); // default rise time: 1ns
+ var pw = Math.abs(arg_value(src.args,5,1e9)); // default pulse width: "infinite"
+ var per = Math.abs(arg_value(src.args,6,1e9)); // default period: "infinite"
+ src.args = [v1,v2,td,tr,tf,pw,per];
+
+ var t1 = td; // time when v1 -> v2 transition starts
+ var t2 = t1 + tr; // time when v1 -> v2 transition ends
+ var t3 = t2 + pw; // time when v2 -> v1 transition starts
+ var t4 = t3 + tf; // time when v2 -> v1 transition ends
+
+ pwl_source(src,[t1,v1, t2,v2, t3,v2, t4,v1, per,v1],true);
+ }
+
+ // post-processing for sinusoidal sources
+ // sin(v_offset,v_amplitude,freq_hz,t_delay,phase_offset_degrees)
+ else if (src.fun == 'sin') {
+ var voffset = arg_value(src.args,0,0); // default offset voltage: 0V
+ var va = arg_value(src.args,1,1); // default amplitude: -1V to 1V
+ var freq = Math.abs(arg_value(src.args,2,1)); // default frequency: 1Hz
+ src.period = 1.0/freq;
+
+ var td = Math.max(0,arg_value(src.args,3,0)); // default time delay: 0sec
+ var phase = arg_value(src.args,4,0); // default phase offset: 0 degrees
+ src.args = [voffset,va,freq,td,phase];
+
+ phase /= 360.0;
+
+ // return value of source at time t
+ src.value = function(t) { // closure
+ if (t < td) return voffset + va*Math.sin(2*Math.PI*phase);
+ else return voffset + va*Math.sin(2*Math.PI*(freq*(t - td) + phase));
+ }
+
+ // return time of next inflection point after time t
+ src.inflection_point = function(t) { // closure
+ if (t < td) return td;
+ else return undefined;
+ }
+ }
+
+ // object has all the necessary info to compute the source value and inflection points
+ src.dc = src.value(0); // DC value is value at time 0
+ return src;
+ }
+
+ function pwl_source(src,tv_pairs,repeat) {
+ var nvals = tv_pairs.length;
+ if (repeat)
+ src.period = tv_pairs[nvals-2]; // Repeat period of source
+ if (nvals % 2 == 1) npts -= 1; // make sure it's even!
+
+ if (nvals <= 2) {
+ // handle degenerate case
+ src.value = function(t) { return nvals == 2 ? tv_pairs[1] : 0; }
+ src.inflection_point = function(t) { return undefined; }
+ } else {
+ src.value = function(t) { // closure
+ if (repeat)
+ // make time periodic if values are to be repeated
+ t = Math.fmod(t,tv_pairs[nvals-2]);
+ var last_t = tv_pairs[0];
+ var last_v = tv_pairs[1];
+ if (t > last_t) {
+ var next_t,next_v;
+ for (var i = 2; i < nvals; i += 2) {
+ next_t = tv_pairs[i];
+ next_v = tv_pairs[i+1];
+ if (next_t > last_t) // defend against bogus tv pairs
+ if (t < next_t)
+ return last_v + (next_v - last_v)*(t - last_t)/(next_t - last_t);
+ last_t = next_t;
+ last_v = next_v;
+ }
+ }
+ return last_v;
+ }
+ src.inflection_point = function(t) { // closure
+ if (repeat)
+ // make time periodic if values are to be repeated
+ t = Math.fmod(t,tv_pairs[nvals-2]);
+ for (var i = 0; i < nvals; i += 2) {
+ var next_t = tv_pairs[i];
+ if (t < next_t) return next_t;
+ }
+ return undefined;
+ }
+ }
+ }
+
+ // helper function: return args[index] if present, else default_v
+ function arg_value(args,index,default_v) {
+ if (index < args.length) {
+ var result = args[index];
+ if (result === undefined) result = default_v;
+ return result;
+ } else return default_v;
+ }
+
+ // we need fmod in the Math library!
+ Math.fmod = function(numerator,denominator) {
+ var quotient = Math.floor(numerator/denominator);
+ return numerator - quotient*denominator;
+ }
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Sources
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ function VSource(npos,nneg,branch,v) {
+ Device.call(this);
+
+ this.src = parse_source(v);
+ this.npos = npos;
+ this.nneg = nneg;
+ this.branch = branch;
+ }
+ VSource.prototype = new Device();
+ VSource.prototype.constructor = VSource;
+
+ // load linear part for source evaluation
+ VSource.prototype.load_linear = function(ckt) {
+ // MNA stamp for independent voltage source
+ ckt.add_to_Gl(this.branch,this.npos,1.0);
+ ckt.add_to_Gl(this.branch,this.nneg,-1.0);
+ ckt.add_to_Gl(this.npos,this.branch,1.0);
+ ckt.add_to_Gl(this.nneg,this.branch,-1.0);
+ }
+
+ // Source voltage added to b.
+ VSource.prototype.load_dc = function(ckt,soln,rhs) {
+ ckt.add_to_rhs(this.branch,this.src.dc,rhs);
+ }
+
+ // Load time-dependent value for voltage source for tran
+ VSource.prototype.load_tran = function(ckt,soln,rhs,time) {
+ ckt.add_to_rhs(this.branch,this.src.value(time),rhs);
+ }
+
+ // return time of next breakpoint for the device
+ VSource.prototype.breakpoint = function(time) {
+ return this.src.inflection_point(time);
+ }
+
+ // small signal model ac value
+ VSource.prototype.load_ac = function(ckt,rhs) {
+ ckt.add_to_rhs(this.branch,1.0,rhs);
+ }
+
+ function ISource(npos,nneg,v) {
+ Device.call(this);
+
+ this.src = parse_source(v);
+ this.npos = npos;
+ this.nneg = nneg;
+ }
+ ISource.prototype = new Device();
+ ISource.prototype.constructor = ISource;
+
+ ISource.prototype.load_linear = function(ckt) {
+ // Current source is open when off, no linear contribution
+ }
+
+ // load linear system equations for dc analysis
+ ISource.prototype.load_dc = function(ckt,soln,rhs) {
+ var is = this.src.dc;
+
+ // MNA stamp for independent current source
+ ckt.add_to_rhs(this.npos,-is,rhs); // current flow into npos
+ ckt.add_to_rhs(this.nneg,is,rhs); // and out of nneg
+ }
+
+ // load linear system equations for tran analysis (just like DC)
+ ISource.prototype.load_tran = function(ckt,soln,rhs,time) {
+ var is = this.src.value(time);
+
+ // MNA stamp for independent current source
+ ckt.add_to_rhs(this.npos,-is,rhs); // current flow into npos
+ ckt.add_to_rhs(this.nneg,is,rhs); // and out of nneg
+ }
+
+ // return time of next breakpoint for the device
+ ISource.prototype.breakpoint = function(time) {
+ return this.src.inflection_point(time);
+ }
+
+ // small signal model: open circuit
+ ISource.prototype.load_ac = function(ckt,rhs) {
+ // MNA stamp for independent current source
+ ckt.add_to_rhs(this.npos,-1.0,rhs); // current flow into npos
+ ckt.add_to_rhs(this.nneg,1.0,rhs); // and out of nneg
+ }
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Resistor
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ function Resistor(n1,n2,v) {
+ Device.call(this);
+ this.n1 = n1;
+ this.n2 = n2;
+ this.g = 1.0/v;
+ }
+ Resistor.prototype = new Device();
+ Resistor.prototype.constructor = Resistor;
+
+ Resistor.prototype.load_linear = function(ckt) {
+ // MNA stamp for admittance g
+ ckt.add_conductance_l(this.n1,this.n2,this.g);
+ }
+
+ Resistor.prototype.load_dc = function(ckt) {
+ // Nothing to see here, move along.
+ }
+
+ Resistor.prototype.load_tran = function(ckt,soln) {
+ }
+
+ Resistor.prototype.load_ac = function(ckt) {
+ }
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Diode
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ function Diode(n1,n2,v,type) {
+ Device.call(this);
+ this.anode = n1;
+ this.cathode = n2;
+ this.area = v;
+ this.type = type; // 'normal' or 'ideal'
+ this.is = 1.0e-14;
+ this.ais = this.area * this.is;
+ this.vt = (type == 'normal') ? 25.8e-3 : 0.1e-3; // 26mv or .1mv
+ this.exp_arg_max = 50; // less than single precision max.
+ this.exp_max = Math.exp(this.exp_arg_max);
+ }
+ Diode.prototype = new Device();
+ Diode.prototype.constructor = Diode;
+
+ Diode.prototype.load_linear = function(ckt) {
+ // Diode is not linear, has no linear piece.
+ }
+
+ Diode.prototype.load_dc = function(ckt,soln,rhs) {
+ var vd = ckt.get_two_terminal(this.anode, this.cathode, soln);
+ var exp_arg = vd / this.vt;
+ var temp1, temp2;
+ // Estimate exponential with a quadratic if arg too big.
+ var abs_exp_arg = Math.abs(exp_arg);
+ var d_arg = abs_exp_arg - this.exp_arg_max;
+ if (d_arg > 0) {
+ var quad = 1 + d_arg + 0.5*d_arg*d_arg;
+ temp1 = this.exp_max * quad;
+ temp2 = this.exp_max * (1 + d_arg);
+ } else {
+ temp1 = Math.exp(abs_exp_arg);
+ temp2 = temp1;
+ }
+ if (exp_arg < 0) { // Use exp(-x) = 1.0/exp(x)
+ temp1 = 1.0/temp1;
+ temp2 = (temp1*temp2)*temp1;
+ }
+ var id = this.ais * (temp1 - 1);
+ var gd = this.ais * (temp2 / this.vt);
+
+ // MNA stamp for independent current source
+ ckt.add_to_rhs(this.anode,-id,rhs); // current flows into anode
+ ckt.add_to_rhs(this.cathode,id,rhs); // and out of cathode
+ ckt.add_conductance(this.anode,this.cathode,gd);
+ }
+
+ Diode.prototype.load_tran = function(ckt,soln,rhs,time) {
+ this.load_dc(ckt,soln,rhs);
+ }
+
+ Diode.prototype.load_ac = function(ckt) {
+ }
+
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Capacitor
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ function Capacitor(n1,n2,v) {
+ Device.call(this);
+ this.n1 = n1;
+ this.n2 = n2;
+ this.value = v;
+ }
+ Capacitor.prototype = new Device();
+ Capacitor.prototype.constructor = Capacitor;
+
+ Capacitor.prototype.load_linear = function(ckt) {
+ // MNA stamp for capacitance matrix
+ ckt.add_capacitance(this.n1,this.n2,this.value);
+ }
+
+ Capacitor.prototype.load_dc = function(ckt,soln,rhs) {
+ }
+
+ Capacitor.prototype.load_ac = function(ckt) {
+ }
+
+ Capacitor.prototype.load_tran = function(ckt) {
+ }
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Inductor
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ function Inductor(n1,n2,branch,v) {
+ Device.call(this);
+ this.n1 = n1;
+ this.n2 = n2;
+ this.branch = branch;
+ this.value = v;
+ }
+ Inductor.prototype = new Device();
+ Inductor.prototype.constructor = Inductor;
+
+ Inductor.prototype.load_linear = function(ckt) {
+ // MNA stamp for inductor linear part
+ // L on diag of C because L di/dt = v(n1) - v(n2)
+ ckt.add_to_Gl(this.n1,this.branch,1);
+ ckt.add_to_Gl(this.n2,this.branch,-1);
+ ckt.add_to_Gl(this.branch,this.n1,-1);
+ ckt.add_to_Gl(this.branch,this.n2,1);
+ ckt.add_to_C(this.branch,this.branch,this.value)
+ }
+
+ Inductor.prototype.load_dc = function(ckt,soln,rhs) {
+ // Inductor is a short at dc, so is linear.
+ }
+
+ Inductor.prototype.load_ac = function(ckt) {
+ }
+
+ Inductor.prototype.load_tran = function(ckt) {
+ }
+
+
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Simple Voltage-Controlled Voltage Source Op Amp model
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+ function Opamp(np,nn,no,ng,branch,A,name) {
+ Device.call(this);
+ this.np = np;
+ this.nn = nn;
+ this.no = no;
+ this.ng = ng;
+ this.branch = branch;
+ this.gain = A;
+ this.name = name;
+ }
+
+ Opamp.prototype = new Device();
+ Opamp.prototype.constructor = Opamp;
+
+ Opamp.prototype.load_linear = function(ckt) {
+ // MNA stamp for VCVS: 1/A(v(no) - v(ng)) - (v(np)-v(nn))) = 0.
+ var invA = 1.0/this.gain;
+ ckt.add_to_Gl(this.no,this.branch,1);
+ ckt.add_to_Gl(this.ng,this.branch,-1);
+ ckt.add_to_Gl(this.branch,this.no,invA);
+ ckt.add_to_Gl(this.branch,this.ng,-invA);
+ ckt.add_to_Gl(this.branch,this.np,-1);
+ ckt.add_to_Gl(this.branch,this.nn,1);
+ }
+
+ Opamp.prototype.load_dc = function(ckt,soln,rhs) {
+ // Op-amp is linear.
+ }
+
+ Opamp.prototype.load_ac = function(ckt) {
+ }
+
+ Opamp.prototype.load_tran = function(ckt) {
+ }
+
+
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Simplified MOS FET with no bulk connection and no body effect.
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+
+
+ function Fet(d,g,s,ratio,name,type) {
+ Device.call(this);
+ this.d = d;
+ this.g = g;
+ this.s = s;
+ this.name = name;
+ this.ratio = ratio;
+ if (type != 'n' && type != 'p')
+ { throw 'fet type is not n or p';
+ }
+ this.type_sign = (type == 'n') ? 1 : -1;
+ this.vt = 0.5;
+ this.kp = 20e-6;
+ this.beta = this.kp * this.ratio;
+ this.lambda = 0.05;
+ }
+ Fet.prototype = new Device();
+ Fet.prototype.constructor = Fet;
+
+ Fet.prototype.load_linear = function(ckt) {
+ // FET's are nonlinear, just like javascript progammers
+ }
+
+ Fet.prototype.load_dc = function(ckt,soln,rhs) {
+ var vds = this.type_sign * ckt.get_two_terminal(this.d, this.s, soln);
+ if (vds < 0) { // Drain and source have swapped roles
+ var temp = this.d;
+ this.d = this.s;
+ this.s = temp;
+ vds = this.type_sign * ckt.get_two_terminal(this.d, this.s, soln);
+ }
+ var vgs = this.type_sign * ckt.get_two_terminal(this.g, this.s, soln);
+ var vgst = vgs - this.vt;
+ with (this) {
+ var gmgs,ids,gds;
+ if (vgst > 0.0 ) { // vgst < 0, transistor off, no subthreshold here.
+ if (vgst < vds) { /* Saturation. */
+ gmgs = beta * (1 + (lambda * vds)) * vgst;
+ ids = type_sign * 0.5 * gmgs * vgst;
+ gds = 0.5 * beta * vgst * vgst * lambda;
+ } else { /* Linear region */
+ gmgs = beta * (1 + lambda * vds);
+ ids = type_sign * gmgs * vds * (vgst - 0.50 * vds);
+ gds = gmgs * (vgst - vds) + beta * lambda * vds * (vgst - 0.5 * vds);
+ gmgs *= vds;
+ }
+ ckt.add_to_rhs(d,-ids,rhs); // current flows into the drain
+ ckt.add_to_rhs(s, ids,rhs); // and out the source
+ ckt.add_conductance(d,s,gds);
+ ckt.add_to_G(s,s, gmgs);
+ ckt.add_to_G(d,s,-gmgs);
+ ckt.add_to_G(d,g, gmgs);
+ ckt.add_to_G(s,g,-gmgs);
+ }
+ }
+ }
+
+ Fet.prototype.load_tran = function(ckt,soln,rhs) {
+ this.load_dc(ckt,soln,rhs);
+ }
+
+ Fet.prototype.load_ac = function(ckt) {
+ }
+
+
+ ///////////////////////////////////////////////////////////////////////////////
+ //
+ // Module definition
+ //
+ ///////////////////////////////////////////////////////////////////////////////
+ var module = {
+ 'Circuit': Circuit,
+ 'parse_number': parse_number,
+ 'parse_source': parse_source,
+ }
+ return module;
+ }());
+
/////////////////////////////////////////////////////////////////////////////
//
// Simple schematic capture
diff --git a/common/lib/xmodule/xmodule/seq_module.py b/common/lib/xmodule/xmodule/seq_module.py
index fee4d53700..65f692957c 100644
--- a/common/lib/xmodule/xmodule/seq_module.py
+++ b/common/lib/xmodule/xmodule/seq_module.py
@@ -29,6 +29,8 @@ class SequenceModule(XModule):
shared_state=None, **kwargs):
XModule.__init__(self, system, location, definition, descriptor,
instance_state, shared_state, **kwargs)
+ # NOTE: Position is 1-indexed. This is silly, but there are now student
+ # positions saved on prod, so it's not easy to fix.
self.position = 1
if instance_state is not None:
diff --git a/common/lib/xmodule/xmodule/x_module.py b/common/lib/xmodule/xmodule/x_module.py
index be61498de6..e21e858baa 100644
--- a/common/lib/xmodule/xmodule/x_module.py
+++ b/common/lib/xmodule/xmodule/x_module.py
@@ -212,7 +212,7 @@ class XModule(HTMLSnippet):
return self.metadata.get('display_name',
self.url_name.replace('_', ' '))
def __unicode__(self):
- return '' % (self.name, self.category, self.id)
+ return ''.format(self.id)
def get_children(self):
'''
@@ -465,6 +465,16 @@ class XModuleDescriptor(Plugin, HTMLSnippet):
return self._child_instances
+
+ def get_child_by_url_name(self, url_name):
+ """
+ Return a child XModuleDescriptor with the specified url_name, if it exists, and None otherwise.
+ """
+ for c in self.get_children():
+ if c.url_name == url_name:
+ return c
+ return None
+
def xmodule_constructor(self, system):
"""
Returns a constructor for an XModule. This constructor takes two
diff --git a/common/test/data/full/course.xml b/common/test/data/full/course.xml
index c365e68cc1..4f093a1128 100644
--- a/common/test/data/full/course.xml
+++ b/common/test/data/full/course.xml
@@ -1 +1 @@
-
+
diff --git a/common/test/data/full/html/sound_labs/mosfet_amplifier.html b/common/test/data/full/html/sound_labs/mosfet_amplifier.html
deleted file mode 100644
index c7f2f1ad81..0000000000
--- a/common/test/data/full/html/sound_labs/mosfet_amplifier.html
+++ /dev/null
@@ -1,124 +0,0 @@
-
-
-
-
-
-
LAB 5B: MOSFET AMPLIFIER EXPERIMENT
-
-
-
Note: This part of the lab is just to develop your intuition about
-amplifiers and biasing, and to have fun with music! There are no responses
-that need to be checked.
-
The graph plots the selected voltages from the amplifier circuit below. You
-can also listen to various signals by selecting from the radio buttons to
-the right of the graph. This way you can both see and hear various signals.
-You can use the sliders to the right of the amplifier circuit to control
-various parameters of the MOSFET and the amplifier. The parameter \(V_{MAX}\)
-sets the maximum range on the plots. You can also select an input voltage
-type (e.g., sine wave, square wave, various types of music) using the drop
-down menu to the right of the graph. When describing AC signals, the
-voltages on the sliders refer to peak-to-peak values.
-
1. To begin your first experiment, go ahead and use the pull down menu to
-select a sine wave input. Then, adjust the sliders to an approximate
-baseline setting shown below.
You will observe in the plot that the baseline setting of the sliders for
-the various amplifiers parameters produces a distorted sine wave signal for
-\(v_{OUT}\). Next, go ahead and select one of the music signals as the input and
-listen to each of \(v_{IN}\) and \(v_{OUT}\), and confirm for yourself that the
-output sounds distorted for the chosen slider settings. You will notice
-that the graph now plots the music signal waveforms. Think about all the
-reasons why the amplifier is producing a distorted output.
-
2. For the second experiment, we will study the amplifier's small signal
-behavior. Select a sine wave as the input signal. To study the small
-signal behavior, reduce the value of \(v_{IN}\) to 0.1V (peak-to-peak) by
-using the \(v_{IN}\) slider. Keeping the rest of the parameters at their
-baseline settings, derive an appropriate value of \(V_{BIAS}\) that will ensure
-saturation region operation for the MOSFET for the 0.1V peak-to-peak swing
-for \(v_{IN}\). Make sure to think about both positive and negative excursions
-of the signals.
-
Next, use the \(V_{BIAS}\) slider to choose your computed value for \(V_{BIAS}\) and
-see if the observed plot of \(v_{OUT}\) is more or less distortion free. If
-your calculation was right, then the output will indeed be distortion free.
-
Next, select one of the music signals as the input and listen to each of
-\(v_{IN}\) and \(v_{OUT}\), and confirm for yourself that the output sounds much
-better than in Step 1. Also, based on sound volume, confirm that \(v_{OUT}\) is
-an amplified version of \(v_{IN}\).
-
3. Now go ahead and experiment with various other settings while listening
-to the music signal at \(v_{OUT}\). Observe the plots and listen to \(v_{OUT}\) as
-you change, for example, the bias voltage \(V_{BIAS}\). You will notice that
-the amplifier distorts the input signal when \(V_{BIAS}\) becomes too small, or
-when it becomes too large. You can also experiment with various values of
-\(v_{IN}\), \(R_{L}\), etc., and see how they affect the amplification and distortion.
LAB 10B: RC FILTERS WITH FREQUENCY RESPONSE EXPERIMENT
-
-
-
Note: Use this part of the lab to build your intuition about filters and frequency response, and to have fun with music! There are no responses that need to be checked.
-
Recall from the audio lab in Week 5 that the graph plots the selected voltages from the circuit shown below. This week the circuit is an RC filter. You can also listen to various signals by selecting from the radio buttons to the right of the graph. This way you can both see and hear various signals. You can use the sliders to the right of the circuit to control various circuit and input signal parameters. (Note that you can get finer control of some of the slider values by clicking on the slider and using the arrow keys). Recall that the parameter \(V_{MAX}\) sets the maximum range on the graph. You can also select an input voltage type (e.g., sine wave, square wave, various types of music) using the drop down menu to the right of the graph. When describing AC signals, the voltages on the sliders refer to peak-to-peak values.
-
1. To begin your first experiment, use the pull down menu to select a sine wave input. Then, adjust the sliders to these approximate baseline settings:
-
-\(v_{IN} = 3V\), \(Frequency = 1000 Hz\), \(V_{BIAS} = 0V\), \(R = 1K\Omega\), \(v_C(0) = 0V\), \(C = 110nF\), \(V_{MAX} = 2V\).
-
-Observe the waveforms for \(v_{IN}\) and \(v_C\) in the graph. You can also listen to \(v_{IN}\) and \(v_C\). You will observe that the amplitude of \(v_C\) is slightly smaller than the amplitude of \(v_{IN}\).
-
-Compute the break frequency of the filter circuit for the given circuit parameters. (Note that the break frequency is also called the cutoff frequency or the corner frequency).
-
-Change the frequency of the sinusoid so that it is approximately 3 times the break frequency.
-
-Observe the waveforms for \(v_{IN}\) and \(v_C\) in the graph. Also listen to \(v_{IN}\) and \(v_C\). Think about why the sinusoid at \(v_C\) is significantly more attenuated than the original 1KHz sinusoid.
-
-Keeping the input signal unchanged, observe the waveforms for \(v_{IN}\) and \(v_R\) in the graph. Also listen to \(v_{IN}\) and \(v_R\). Think about why the sinusoid at \(v_R\) is significantly louder than the sinusoid at \(v_C\).
-
2. Next, use the pull down menu to select a music signal of your choice. Adjust the sliders to the approximate baseline settings:
-
-\(v_{IN} = 3V\), \(V_{BIAS} = 0V\), \(R = 1K\Omega\), \(v_C(0) = 0V\), \(C = 110nF\), \(V_{MAX} = 2V\).
-
-Listen to the signals at \(v_{IN}\) and \(v_C\). Notice any difference between the signals?
-
-Next, increase the capacitance value and observe the difference in the sound of \(v_{IN}\) and \(v_C\) as the capacitance increases. You should notice that the higher frequency components of \(v_C\) are attenuated as the capacitance is increased.
-Convince yourself that when the signal is taken at \(v_C\), the circuit behaves like a low-pass filter.
-
3. Re-adjust the sliders to the approximate baseline settings:
-
-\(v_{IN} = 3V\), \(V_{BIAS} = 0V\), \(R = 1K\Omega\), \(v_C(0) = 0V\), \(C = 110nF\), \(V_{MAX} = 2V\).
-
-Try to create a high-pass filter from the same circuit by taking the signal output across a different element and possibly changing some of the element values.
-