From e40982c2ec958ff8219510de568fa8e3ab035a5a Mon Sep 17 00:00:00 2001 From: miguel Date: Wed, 25 Nov 2020 18:12:22 +1100 Subject: [PATCH] Updated Coax with Z. Added Z in help. --- inductor.html | 6 ++-- inductor_imp.html | 6 ++-- inductor_lrg.html | 76 +++++++++++++++++++++++++++-------------------- 3 files changed, 49 insertions(+), 39 deletions(-) diff --git a/inductor.html b/inductor.html index 09b05c2..c052fae 100644 --- a/inductor.html +++ b/inductor.html @@ -65,8 +65,9 @@
  • Rdc : DC resistance is calculated using conductor length divided by the conductor cross-sectional area, assuming a copper conductor.
  • SRF : Self-resonant frequency (MHz) for the unloaded coil. Currently using a lumped reactances model. (Looking into modifying the model to use the conductor length and velocity factor as described by Knight (2016).
  • -
  • Xl : Inductive reactance at the given frequency. (Ω)
  • -
  • δ : Skin depth due to skin effect (μm)
  • +
  • Xₗ : Inductive reactance at the given frequency. (Ω)
  • +
  • |Z| : Impedance at the given frequency. (Ω)
  • +
  • δ : Skin depth due to skin effect (μm)
  • Rac : AC resistance is calculated using the skin effect and proximity resistance from empirical data collected by Medhurst using the spacing ratio, and length-to-diameter ratio.
  • Q : Quality factor of device, based on reactance (X) ÷ resistance (Rac) at the given frequency.
  • @@ -115,7 +116,6 @@ var Zl = math.complex(inductor.Rac, inductor.Xl); var Zc = math.complex(0, inductor.Xc); inductor.Z = math.divide(math.multiply(Zl, Zc), math.add(Zl, Zc)).toPolar(); - // Redraw the canvas: drawDesign(); } diff --git a/inductor_imp.html b/inductor_imp.html index 2988bd7..0c8bd26 100644 --- a/inductor_imp.html +++ b/inductor_imp.html @@ -65,8 +65,9 @@
  • Rdc : DC resistance is calculated using conductor length divided by the conductor cross-sectional area, assuming a copper conductor.
  • SRF : Self-resonant frequency (MHz) for the unloaded coil. Currently using a lumped reactances model. (Looking into modifying the model to use the conductor length and velocity factor as described by Knight (2016).
  • -
  • Xl : Inductive reactance at the given frequency. (Ω)
  • -
  • δ : Skin depth due to skin effect (μm)
  • +
  • Xₗ : Inductive reactance at the given frequency. (Ω)
  • +
  • |Z| : Impedance at the given frequency. (Ω)
  • +
  • δ : Skin depth due to skin effect (μm)
  • Rac : AC resistance is calculated using the skin effect and proximity resistance from empirical data collected by Medhurst using the spacing ratio, and length-to-diameter ratio.
  • Q : Quality factor of device, based on reactance (X) ÷ resistance (Rac) at the given frequency.
  • @@ -115,7 +116,6 @@ var Zl = math.complex(inductor.Rac, inductor.Xl); var Zc = math.complex(0, inductor.Xc); inductor.Z = math.divide(math.multiply(Zl, Zc), math.add(Zl, Zc)).toPolar(); - // Redraw the canvas: drawDesign(); } diff --git a/inductor_lrg.html b/inductor_lrg.html index 63df87e..297db44 100644 --- a/inductor_lrg.html +++ b/inductor_lrg.html @@ -15,12 +15,12 @@
    - +
    - - + +
    @@ -67,13 +67,15 @@
  • Rdc : DC resistance is calculated using conductor length divided by the conductor cross-sectional area, assuming a copper conductor.
  • SRF : Self-resonant frequency (MHz) for the unloaded coil. Currently using a lumped reactances model. (Looking into modifying the model to use the conductor length and velocity factor as described by Knight (2016).
  • -
  • Xl : Inductive reactance at the given frequency. (Ω)
  • -
  • δ : Skin depth due to skin effect (μm)
  • +
  • Xₗ : Inductive reactance at the given frequency. (Ω)
  • +
  • |Z| : Impedance at the given frequency. (Ω)
  • +
  • δ : Skin depth due to skin effect (μm)
  • Rac : AC resistance is calculated using the skin effect and proximity resistance from empirical data collected by Medhurst using the spacing ratio, and length-to-diameter ratio.
  • Q : Quality factor of device, based on reactance (X) ÷ resistance (Rac) at the given frequency.
  • +