kicad-source/pcb_calculator/calculator_panels/panel_fusing_current.cpp
Seth Hillbrand 0b2d4d4879 Revise Copyright statement to align with TLF
Recommendation is to avoid using the year nomenclature as this
information is already encoded in the git repo.  Avoids needing to
repeatly update.

Also updates AUTHORS.txt from current repo with contributor names
2025-01-01 14:12:04 -08:00

234 lines
7.8 KiB
C++

/*
* This program source code file is part of KICAD, a free EDA CAD application.
*
* Copyright The KiCad Developers, see AUTHORS.txt for contributors.
*
* This program is free software; you can redistribute it and/or
* modify it under the terms of the GNU General Public License
* as published by the Free Software Foundation; either version 3
* of the License, or (at your option) any later version.
*
* This program is distributed in the hope that it will be useful,
* but WITHOUT ANY WARRANTY; without even the implied warranty of
* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
* GNU General Public License for more details.
*
* You should have received a copy of the GNU General Public License along
* with this program. If not, see <http://www.gnu.org/licenses/>.
*/
// See equation 9b in this paper:
// https://adam-research.de/pdfs/TRM_WhitePaper10_AdiabaticWire.pdf
// See equation 8
//https://scholar.google.com/scholar?hl=en&as_sdt=0%2C5&q=Fusing+of+wires+by+electrical+current&btnG=
#define ABS_ZERO ( -273.15 )
#include <calculator_panels/panel_fusing_current.h>
#include <pcb_calculator_settings.h>
#include <string_utils.h>
#include <widgets/unit_selector.h>
#include <i18n_utility.h> // For _HKI definition
wxString fusing_current_help =
#include "fusing_current_help.h"
PANEL_FUSING_CURRENT::PANEL_FUSING_CURRENT( wxWindow * parent, wxWindowID id,
const wxPoint& pos, const wxSize& size,
long style, const wxString& name ) :
PANEL_FUSING_CURRENT_BASE( parent, id, pos, size, style, name )
{
m_ambientUnit->SetLabel( wxT( "°C" ) );
m_meltingUnit->SetLabel( wxT( "°C" ) );
// Set some defaults
m_ambientValue->SetValue( wxString::Format( wxT( "%i" ), 25 ) );
m_meltingValue->SetValue( wxString::Format( wxT( "%i" ), 1084 ) ); // Value for copper
m_meltingValue->SetEditable( false ); // For now, this panel only works for copper.
m_widthValue->SetValue( wxString::Format( wxT( "%f" ), 0.1 ) );
m_thicknessValue->SetValue( wxString::Format( wxT( "%f" ), 0.035 ) );
m_currentValue->SetValue( wxString::Format( wxT( "%f" ), 10.0 ) );
m_timeValue->SetValue( wxString::Format( wxT( "%f" ), 0.01 ) );
// show markdown formula explanation in lower help panel
wxString msg;
ConvertMarkdown2Html( wxGetTranslation( fusing_current_help ), msg );
m_htmlHelp->SetPage( msg );
// Needed on wxWidgets 3.0 to ensure sizers are correctly set
GetSizer()->SetSizeHints( this );
}
PANEL_FUSING_CURRENT::~PANEL_FUSING_CURRENT()
{
}
void PANEL_FUSING_CURRENT::ThemeChanged()
{
// Update the HTML window with the help text
m_htmlHelp->ThemeChanged();
}
void PANEL_FUSING_CURRENT::m_onCalculateClick( wxCommandEvent& event )
{
double Tm, Ta, I, W, T, time;
bool valid_Tm, valid_Ta, valid_I, valid_W, valid_T, valid_time;
valid_Tm = m_meltingValue->GetValue().ToDouble( &Tm );
valid_Ta = m_ambientValue->GetValue().ToDouble( &Ta );
valid_I = m_currentValue->GetValue().ToDouble( &I );
valid_W = m_widthValue->GetValue().ToDouble( &W );
valid_T = m_thicknessValue->GetValue().ToDouble( &T );
valid_time = m_timeValue->GetValue().ToDouble( &time );
double scalingT, scalingW;
scalingT = m_thicknessUnit->GetUnitScale();
scalingW = m_widthUnit->GetUnitScale();
T *= scalingT;
W *= scalingW;
valid_Tm &= std::isfinite( Tm );
valid_Ta &= std::isfinite( Ta );
valid_I &= std::isfinite( I );
valid_W &= std::isfinite( W );
valid_T &= std::isfinite( T );
valid_time &= std::isfinite( time );
if( valid_Tm && valid_Ta )
{
valid_Tm &= ( Tm > Ta );
valid_Ta &= ( Tm > Ta ) && ( Ta > ABS_ZERO );
}
valid_I &= ( I > 0 );
valid_W &= ( W > 0 );
valid_T &= ( T > 0 );
valid_time &= ( time > 0 );
double A = W * T;
// The energy required for copper to change phase ( fusion ) is 13.05 kJ / mol.
// Copper molar mass is 0.06355 kg/mol
// => The copper energy required for the phase change is 205.35 kJ / kg
double latentHeat = 205350.0;
// The change in enthalpy is deltaH = deltaU + delta P * deltaV
// with U the internal energy, P the pressure and V the volume
// But for constant pressure, the change in enthalpy is simply the thermal energy
// Copper specific heat energy is 0.385 kJ / kg / K.
// The change in heat energy is then 0.385 kJ / kg per degree.
double cp = 385; // Heat capacity in J / kg / K
double deltaEnthalpy = ( Tm - Ta ) * cp;
double density = 8940; // Density of copper to kilogram per cubic meter;
double volumicEnergy = density * ( deltaEnthalpy + latentHeat );
// Equation (3) is equivalent to :
// VolumicEnergy * Volume = R * I^2 * t
// If we consider the resistivity of copper instead of its resistance:
// VolumicEnergy * Volume = resistivity * length / Area * I^2 * t
// For a unit length:
// VolumicEnergy * Area = resistivity / Area * I^2 * t
// We can rewrite it as:
// VolumicEnergy * ( Area / I )^2 / resistivity = t
// coeff * ( Area / I ) ^2 = t with coeff = VolumicEnergy / resistivity
// Copper resistivity at 20C ( 293K ) is 1.72e-8 ohm m
// Copper temperature coefficient is 0.00393 per degree
double Ra = ( ( Ta - ABS_ZERO - 293 ) * 0.00393 + 1 ) * 1.72e-8;
double Rm = ( ( Tm - ABS_ZERO - 293 ) * 0.00393 + 1 ) * 1.72e-8;
// Let's consider the average resistivity
double R = ( Rm + Ra ) / 2;
double coeff = volumicEnergy / R;
bool valid = valid_I && valid_W && valid_T && valid_Ta && valid_Tm && valid_time;
if( m_widthRadio->GetValue() )
{
if( valid )
{
A = I / sqrt( coeff / time );
W = A / T;
m_widthValue->SetValue( wxString::Format( wxT( "%f" ), W / scalingW ) );
}
else
{
m_widthValue->SetValue( _( "Error" ) );
}
}
else if( m_thicknessRadio->GetValue() )
{
if( valid )
{
A = I / sqrt( coeff / time );
T = A / W;
m_thicknessValue->SetValue( wxString::Format( wxT( "%f" ), T / scalingT ) );
}
else
{
m_thicknessValue->SetValue( _( "Error" ) );
}
}
else if( m_currentRadio->GetValue() )
{
if( valid )
{
I = A * sqrt( coeff / time );
m_currentValue->SetValue( wxString::Format( wxT( "%f" ), I ) );
}
else
{
m_currentValue->SetValue( _( "Error" ) );
}
}
else if( m_timeRadio->GetValue() )
{
if( valid )
{
time = coeff * A * A / I / I;
m_timeValue->SetValue( wxString::Format( wxT( "%f" ), time ) );
}
else
{
m_timeValue->SetValue( _( "Error" ) );
}
}
else
{
// What happened ??? an extra radio button ?
}
// Now let's check the validity domain using the formula from the paper.
// https://adam-research.de/pdfs/TRM_WhitePaper10_AdiabaticWire.pdf
// We approximate the track with a circle having the same area.
double r = sqrt( A / M_PI ); // radius in m;
double epsilon = 5.67e-8; // Stefan-Boltzmann constant in W / ( m^2 K^4 )
double sigma = 0.5; // Surface radiative emissivity ( no unit )
// sigma is according to paper, between polished and oxidized
double tmKelvin = Tm - ABS_ZERO;
double frad = 0.5 * ( tmKelvin + 293 ) * ( tmKelvin + 293 ) * ( tmKelvin + 293 );
double tau = cp * density * r / ( epsilon * sigma * frad * 2 );
if( 2 * time < tau )
{
m_comment->SetLabel( "" );
}
else
{
m_comment->SetLabel( _( "Current calculation is underestimated due to long fusing time."
) );
}
}