232 lines
7.8 KiB
C++
232 lines
7.8 KiB
C++
/*
|
|
* This program source code file is part of KICAD, a free EDA CAD application.
|
|
*
|
|
* Copyright (C) 1992-2021 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 )
|
|
{
|
|
// Set some defaults
|
|
wxString wxs( "" );
|
|
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( 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."
|
|
) );
|
|
}
|
|
} |