Complete low pass report

6 years ago · 70aa45bbd6
42 changed files with 17013 additions and 330 deletions
--- a/Chebyshev/Multisim/band_pass_chebyshev.ms14
+++ b/Chebyshev/Multisim/band_pass_chebyshev.ms14
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev.ms14
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev.ms14
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_bode_plotter.csv
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_bode_plotter.csv
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_bode_plotter.svg
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_bode_plotter.svg
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_bode_plotter_with_values.svg
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_bode_plotter_with_values.svg
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope.csv
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope.csv
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope_combined_input_output_sig.svg
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope_combined_input_output_sig.svg
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope_input_sig.svg
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope_input_sig.svg
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope_output_sig.svg
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_oscilloscope_output_sig.svg
--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_spectrum_analyzer_combined_input_output.svg
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_spectrum_analyzer_combined_input_output.svg
@ -0,0 +1,347 @@
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      >0</text
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    ><g transform="translate(348.2,792.208)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.6</text
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    ><g transform="translate(738.8,792.208)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.8</text
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    ><g transform="translate(869,792.208)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >1</text
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    ><g transform="translate(999.2,792.208)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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    ><g transform="translate(1259.6,792.208)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >1.6</text
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    ><g transform="translate(1389.8,792.208)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >1.8</text
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      >2</text
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      >Frequency (Hz)</text
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      >#</text
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    ><g transform="translate(1488,847)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >10</text
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    ><g transform="translate(1511,837)" style="text-rendering:geometricPrecision; font-size:16px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      /><line y2="689.875" style="fill:none;" x1="223.208" x2="212.792" y1="689.875"
      /><line y2="600.75" style="fill:none;" x1="223.208" x2="212.792" y1="600.75"
      /><line y2="511.625" style="fill:none;" x1="223.208" x2="212.792" y1="511.625"
      /><line y2="422.5" style="fill:none;" x1="223.208" x2="212.792" y1="422.5"
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      /><line y2="244.25" style="fill:none;" x1="223.208" x2="212.792" y1="244.25"
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    ><g transform="translate(204.792,779)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-12" xml:space="preserve" y="8" style="stroke:none;"
      >0</text
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    ><g transform="translate(204.792,689.875)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.1</text
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    ><g transform="translate(204.792,600.75)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.2</text
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    ><g transform="translate(204.792,511.625)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.3</text
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    ><g transform="translate(204.792,422.5)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.4</text
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    ><g transform="translate(204.792,333.375)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.5</text
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    ><g transform="translate(204.792,244.25)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.6</text
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    ><g transform="translate(204.792,155.125)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.7</text
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    ><g transform="translate(204.792,66)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.8</text
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    ><g transform="translate(170.792,422.4997) rotate(-90)" style="text-rendering:geometricPrecision; font-size:22px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >Spectrum analyzer plot</text
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--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_spectrum_analyzer_input.csv
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_spectrum_analyzer_input.csv
@ -0,0 +1,513 @@
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    ><g transform="translate(1589.2,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >Frequency (Hz)</text
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    ><g transform="translate(1690,884)" style="font-size:20px; text-rendering:geometricPrecision; color-rendering:optimizeQuality; image-rendering:optimizeQuality; font-family:'mwb_cmsy10'; color-interpolation:linearRGB;"
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      >#</text
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    ><g transform="translate(1706,884)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >10</text
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      >4</text
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      /><line y2="628.5" style="fill:none;" x1="255.952" x2="244.048" y1="628.5"
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      /><line y2="255.5" style="fill:none;" x1="255.952" x2="244.048" y1="255.5"
      /><line y2="162.25" style="fill:none;" x1="255.952" x2="244.048" y1="162.25"
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    ><g transform="translate(236.048,815)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0</text
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      >0.1</text
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    ><g transform="translate(236.048,628.5)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.2</text
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      >0.3</text
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    ><g transform="translate(236.048,442)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.4</text
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      >0.5</text
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    ><g transform="translate(236.048,255.5)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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      >0.7</text
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    ><g transform="translate(236.048,69)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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    ><g transform="translate(202.048,441.9996) rotate(-90)" style="text-rendering:geometricPrecision; font-size:22px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
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--- a/Chebyshev/Multisim/low_pass_inversed_chebyshev_spectrum_analyzer_output.csv
+++ b/Chebyshev/Multisim/low_pass_inversed_chebyshev_spectrum_analyzer_output.csv
@ -0,0 +1,513 @@
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    ><text x="-6" xml:space="preserve" y="21" style="stroke:none;"
      >0</text
    ></g
    ><g transform="translate(398.8,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >0.2</text
    ></g
    ><g transform="translate(547.6,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >0.4</text
    ></g
    ><g transform="translate(696.4,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >0.6</text
    ></g
    ><g transform="translate(845.2,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >0.8</text
    ></g
    ><g transform="translate(994,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-6" xml:space="preserve" y="21" style="stroke:none;"
      >1</text
    ></g
    ><g transform="translate(1142.8,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >1.2</text
    ></g
    ><g transform="translate(1291.6,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >1.4</text
    ></g
    ><g transform="translate(1440.4,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >1.6</text
    ></g
    ><g transform="translate(1589.2,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-14" xml:space="preserve" y="21" style="stroke:none;"
      >1.8</text
    ></g
    ><g transform="translate(1738,828.952)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-6" xml:space="preserve" y="21" style="stroke:none;"
      >2</text
    ></g
    ><g transform="translate(994.0007,856.952)" style="text-rendering:geometricPrecision; font-size:22px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-76" xml:space="preserve" y="23" style="stroke:none;"
      >Frequency (Hz)</text
    ></g
    ><g transform="translate(1690,884)" style="font-size:20px; text-rendering:geometricPrecision; color-rendering:optimizeQuality; image-rendering:optimizeQuality; font-family:'mwb_cmsy10'; color-interpolation:linearRGB;"
    ><text x="0" xml:space="preserve" y="0" style="stroke:none;"
      >#</text
    ></g
    ><g transform="translate(1706,884)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="0" xml:space="preserve" y="0" style="stroke:none;"
      >10</text
    ></g
    ><g transform="translate(1729,874)" style="text-rendering:geometricPrecision; font-size:16px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="0" xml:space="preserve" y="0" style="stroke:none;"
      >4</text
    ></g
    ><g style="text-rendering:geometricPrecision; color-interpolation:linearRGB; color-rendering:optimizeQuality; stroke-linejoin:round; image-rendering:optimizeQuality;"
    ><line y2="69" style="fill:none;" x1="250" x2="250" y1="815"
      /><line y2="815" style="fill:none;" x1="255.952" x2="244.048" y1="815"
      /><line y2="721.75" style="fill:none;" x1="255.952" x2="244.048" y1="721.75"
      /><line y2="628.5" style="fill:none;" x1="255.952" x2="244.048" y1="628.5"
      /><line y2="535.25" style="fill:none;" x1="255.952" x2="244.048" y1="535.25"
      /><line y2="442" style="fill:none;" x1="255.952" x2="244.048" y1="442"
      /><line y2="348.75" style="fill:none;" x1="255.952" x2="244.048" y1="348.75"
      /><line y2="255.5" style="fill:none;" x1="255.952" x2="244.048" y1="255.5"
      /><line y2="162.25" style="fill:none;" x1="255.952" x2="244.048" y1="162.25"
      /><line y2="69" style="fill:none;" x1="255.952" x2="244.048" y1="69"
    /></g
    ><g transform="translate(236.048,815)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-12" xml:space="preserve" y="8" style="stroke:none;"
      >0</text
    ></g
    ><g transform="translate(236.048,721.75)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.1</text
    ></g
    ><g transform="translate(236.048,628.5)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.2</text
    ></g
    ><g transform="translate(236.048,535.25)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.3</text
    ></g
    ><g transform="translate(236.048,442)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.4</text
    ></g
    ><g transform="translate(236.048,348.75)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.5</text
    ></g
    ><g transform="translate(236.048,255.5)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.6</text
    ></g
    ><g transform="translate(236.048,162.25)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.7</text
    ></g
    ><g transform="translate(236.048,69)" style="text-rendering:geometricPrecision; font-size:20px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-28" xml:space="preserve" y="8" style="stroke:none;"
      >0.8</text
    ></g
    ><g transform="translate(202.048,441.9996) rotate(-90)" style="text-rendering:geometricPrecision; font-size:22px; color-interpolation:linearRGB; color-rendering:optimizeQuality; image-rendering:optimizeQuality;"
    ><text x="-67" xml:space="preserve" y="-5" style="stroke:none;"
      >Amplitude (V)</text
    ></g
    ><g transform="translate(994.0009,66.25)" style="font-size:22px; text-rendering:geometricPrecision; color-rendering:optimizeQuality; image-rendering:optimizeQuality; color-interpolation:linearRGB; font-weight:bold;"
    ><text x="-121.5" xml:space="preserve" y="-5" style="stroke:none;"
      >Spectrum analyzer plot</text
    ></g
    ><g style="stroke-linecap:butt; fill:green; text-rendering:geometricPrecision; color-rendering:optimizeQuality; image-rendering:optimizeQuality; stroke-linejoin:round; color-interpolation:linearRGB; stroke:green;"
    ><path d="M250 442.3347 L257.44 815 L264.88 815 L272.32 815 L279.76 814.4417 L287.2 815 L294.64 815 L302.08 815 L309.52 814.5945 L316.96 815 L324.4 815 L331.84 815 L339.28 814.9423 L346.72 815 L354.16 815 L361.6 815 L369.04 814.4802 L376.48 815 L383.92 815 L391.36 815 L398.8 250.7004 L406.24 815 L413.68 815 L421.12 815 L428.56 814.8175 L436 815 L443.44 815 L450.88 815 L458.32 814.6912 L465.76 815 L473.2 815 L480.64 815 L488.08 814.5645 L495.52 815 L502.96 815 L510.4 815 L517.84 814.7742 L525.28 815 L532.72 815 L540.16 815 L547.6 640.4994 L555.04 815 L562.48 815 L569.92 815 L577.36 814.3147 L584.8 815 L592.24 815 L599.68 815 L607.12 814.7845 L614.56 815 L622 815 L629.44 815 L636.88 814.7793 L644.32 815 L651.76 815 L659.2 815 L666.64 814.3551 L674.08 815 L681.52 815 L688.96 815 L696.4 700.627 L703.84 815 L711.28 815 L718.72 815 L726.16 814.7458 L733.6 815 L741.04 815 L748.48 815 L755.92 814.5542 L763.36 815 L770.8 815 L778.24 815 L785.68 814.7042 L793.12 815 L800.56 815 L808 815 L815.44 814.8155 L822.88 815 L830.32 815 L837.76 815 L845.2 705.172 L852.64 815 L860.08 815 L867.52 815 L874.96 814.4556 L882.4 815 L889.84 815 L897.28 815 L904.72 814.9313 L912.16 815 L919.6 815 L927.04 815 L934.48 814.5969 L941.92 815 L949.36 815 L956.8 815 L964.24 814.4819 L971.68 815 L979.12 815 L986.56 815 L994 814.8243 L1001.44 815 L1008.88 815 L1016.32 815 L1023.76 814.3969 L1031.2 815 L1038.64 815 L1046.08 815 L1053.52 814.5908 L1060.96 815 L1068.4 815 L1075.84 815 L1083.28 814.9525 L1090.72 815 L1098.16 815 L1105.6 815 L1113.04 814.5018 L1120.48 815 L1127.92 815 L1135.36 815 L1142.8 812.4291 L1150.24 815 L1157.6801 815 L1165.12 815 L1172.5601 814.8193 L1180 815 L1187.4399 815 L1194.88 815 L1202.3199 814.6769 L1209.76 815 L1217.2 815 L1224.64 815 L1232.08 814.5731 L1239.52 815 L1246.96 815 L1254.4 815 L1261.84 814.7996 L1269.28 815 L1276.72 815 L1284.16 815 L1291.6 812.4006 L1299.04 815 L1306.48 815 L1313.92 815 L1321.36 814.2698 L1328.8 815 L1336.24 815 L1343.6801 815 L1351.12 814.7893 L1358.5601 815 L1366 815 L1373.4399 815 L1380.88 814.7736 L1388.3199 815 L1395.76 815 L1403.2 815 L1410.64 814.3908 L1418.08 815 L1425.52 815 L1432.96 815 L1440.4 812.0226 L1447.84 815 L1455.28 815 L1462.72 815 L1470.16 814.7148 L1477.6 815 L1485.04 815 L1492.48 815 L1499.92 814.5422 L1507.36 815 L1514.8 815 L1522.24 815 L1529.6801 814.7159 L1537.12 815 L1544.5601 815 L1552 815 L1559.4399 814.8132 L1566.88 815 L1574.3199 815 L1581.76 815 L1589.2 810.9329 L1596.64 815 L1604.08 815 L1611.52 815 L1618.96 814.4285 L1626.4 815 L1633.84 815 L1641.28 815 L1648.72 814.9194 L1656.16 815 L1663.6 815 L1671.04 815 L1678.48 814.598 L1685.92 815 L1693.36 815 L1700.8 815 L1708.24 814.5176 L1715.6801 815 L1723.12 815 L1730.5601 815 L1738 814.8212 L1738.1488 814.8248" style="fill:none; fill-rule:evenodd;"
    /></g
  ></g
 ></svg
 >
--- a/Chebyshev/Multisim/multisim_csv_plot.m
+++ b/Chebyshev/Multisim/multisim_csv_plot.m
@ -1,4 +1,5 @@
-multisim = csvread('low_pass_inversed_chebyshev_bode_plot.csv', 1, 0);
+%{
 multisim = csvread('low_pass_inversed_chebyshev_bode_plotter.csv', 1, 0);
 % Create figure
 figure1 = figure('Name','Bode plot','Color',[1 1 1]);
@ -8,7 +9,6 @@ hold(axes1,'on');
 % Create semilogx
 semilogx(multisim(:, 1),20*log10(multisim(:, 2)),'Color',[1 0.501960813999176 0]);
 xlabel('Frequency (Hz)');
 ylabel('Gain (dB)');
 ylim(axes1,[-90 10]);
@ -17,3 +17,125 @@ set(axes1,'Color',[0 0 0],'GridAlpha',0.5,'GridColor',[1 1 1],...
    'GridLineStyle',':','MinorGridAlpha',0.5,'MinorGridColor',[1 1 1],'TickDir',...
    'both','TickLength',[0.004 0.0025],'XColor',[0 0 0],'XGrid','on',...
    'XMinorTick','on','XScale','log','YColor',[0 0 0],'YGrid','on');
 %=======================================================================================
 multisim = csvread('low_pass_inversed_chebyshev_oscilloscope.csv', 1, 0);
 % Create figure
 figure1 = figure('Name','Oscilloscope plot','Color',[1 1 1]);
 axes1 = axes('Parent',figure1);
 hold(axes1,'on');
 plot(multisim(:, 1),multisim(:, 2),'Color',[1 0.501960813999176 0]);
 xlabel('Time (s)');
 ylabel('Voltage (V)');
 ylim(axes1,[-1.5 1.5]);
 xlim(axes1,[-1e-05 0.005]);
 title('Oscilloscope plot')
 set(axes1,'Color',[0 0 0],'GridAlpha',0.5,'GridColor',[1 1 1],...
    'GridLineStyle',':','MinorGridAlpha',0.5,'MinorGridColor',[1 1 1],'TickDir',...
    'both','TickLength',[0.004 0.0025],'XColor',[0 0 0],'XGrid','on',...
    'XMinorTick','on','YColor',[0 0 0],'YGrid','on');
 %=======================================================================================
 % Create figure
 figure1 = figure('Name','Oscilloscope plot','Color',[1 1 1]);
 axes1 = axes('Parent',figure1);
 hold(axes1,'on');
 plot(multisim(:, 4),multisim(:, 5),'Color',[0 0.5 0]);
 xlabel('Time (s)');
 ylabel('Voltage (V)');
 ylim(axes1,[-1.5 1.5]);
 xlim(axes1,[-1e-05 0.005]);
 title('Oscilloscope plot')
 set(axes1,'Color',[0 0 0],'GridAlpha',0.5,'GridColor',[1 1 1],...
    'GridLineStyle',':','MinorGridAlpha',0.5,'MinorGridColor',[1 1 1],'TickDir',...
    'both','TickLength',[0.004 0.0025],'XColor',[0 0 0],'XGrid','on',...
    'XMinorTick','on','YColor',[0 0 0],'YGrid','on');
 %=======================================================================================
 % Create figure
 figure1 = figure('Name','Oscilloscope plot','Color',[1 1 1]);
 axes1 = axes('Parent',figure1);
 hold(axes1,'on');
 plot(multisim(:, 1),multisim(:, 2),'Color',[1 0.501960813999176 0]);
 plot(multisim(:, 4),multisim(:, 5),'Color',[0 0.5 0]);
 xlabel('Time (s)');
 ylabel('Voltage (V)');
 ylim(axes1,[-1.5 1.5]);
 xlim(axes1,[-1e-05 0.005]);
 title('Oscilloscope plot')
 set(axes1,'Color',[0 0 0],'GridAlpha',0.5,'GridColor',[1 1 1],...
    'GridLineStyle',':','MinorGridAlpha',0.5,'MinorGridColor',[1 1 1],'TickDir',...
    'both','TickLength',[0.004 0.0025],'XColor',[0 0 0],'XGrid','on',...
    'XMinorTick','on','YColor',[0 0 0],'YGrid','on');
 %}
 %=======================================================================================
 multisim = csvread('low_pass_inversed_chebyshev_spectrum_analyzer_input.csv', 1, 0);
 % Create figure
 figure1 = figure('Name','Spectrum analyzer plot','Color',[1 1 1]);
 axes1 = axes('Parent',figure1);
 hold(axes1,'on');
 plot(multisim(:, 1),multisim(:, 2),'Color',[1 0.501960813999176 0]);
 xlabel('Frequency (Hz)');
 ylabel('Amplitude (V)');
 ylim(axes1,[0 0.8]);
 xlim(axes1,[0 20000]);
 title('Spectrum analyzer plot')
 set(axes1,'Color',[0 0 0],'GridAlpha',0.5,'GridColor',[1 1 1],...
    'GridLineStyle',':','MinorGridAlpha',0.5,'MinorGridColor',[1 1 1],'TickDir',...
    'both','TickLength',[0.004 0.0025],'XColor',[0 0 0],'XGrid','on',...
    'XMinorTick','on','YColor',[0 0 0],'YGrid','on');
 %=======================================================================================
 multisim2 = csvread('low_pass_inversed_chebyshev_spectrum_analyzer_output.csv', 1, 0);
 % Create figure
 figure1 = figure('Name','Spectrum analyzer plot','Color',[1 1 1]);
 axes1 = axes('Parent',figure1);
 hold(axes1,'on');
 plot(multisim2(:, 1),multisim2(:, 2),'Color',[0 0.5 0]);
 xlabel('Frequency (Hz)');
 ylabel('Amplitude (V)');
 ylim(axes1,[0 0.8]);
 xlim(axes1,[0 20000]);
 title('Spectrum analyzer plot')
 set(axes1,'Color',[0 0 0],'GridAlpha',0.5,'GridColor',[1 1 1],...
    'GridLineStyle',':','MinorGridAlpha',0.5,'MinorGridColor',[1 1 1],'TickDir',...
    'both','TickLength',[0.004 0.0025],'XColor',[0 0 0],'XGrid','on',...
    'XMinorTick','on','YColor',[0 0 0],'YGrid','on');
 %=======================================================================================
 % Create figure
 figure1 = figure('Name','Spectrum analyzer plot','Color',[1 1 1]);
 axes1 = axes('Parent',figure1);
 hold(axes1,'on');
 plot(multisim(:, 1),multisim(:, 2),'Color',[1 0.501960813999176 0]);
 plot(multisim2(:, 1),multisim2(:, 2),'Color',[0 0.5 0]);
 xlabel('Frequency (Hz)');
 ylabel('Amplitude (V)');
 ylim(axes1,[0 0.8]);
 xlim(axes1,[0 20000]);
 title('Spectrum analyzer plot')
 set(axes1,'Color',[0 0 0],'GridAlpha',0.5,'GridColor',[1 1 1],...
    'GridLineStyle',':','MinorGridAlpha',0.5,'MinorGridColor',[1 1 1],'TickDir',...
    'both','TickLength',[0.004 0.0025],'XColor',[0 0 0],'XGrid','on',...
    'XMinorTick','on','YColor',[0 0 0],'YGrid','on');
--- a/Chebyshev/low_pass_inversed_chebyshev_combined_input_output_sig.svg
+++ b/Chebyshev/low_pass_inversed_chebyshev_combined_input_output_sig.svg
--- a/Chebyshev/low_pass_inversed_chebyshev_input_spectrum.svg
+++ b/Chebyshev/low_pass_inversed_chebyshev_input_spectrum.svg
--- a/Chebyshev/low_pass_inversed_chebyshev_input_spectrum_zoom.svg
+++ b/Chebyshev/low_pass_inversed_chebyshev_input_spectrum_zoom.svg
--- a/Chebyshev/low_pass_inversed_chebyshev_output_spectrum.svg
+++ b/Chebyshev/low_pass_inversed_chebyshev_output_spectrum.svg
--- a/Chebyshev/low_pass_inversed_chebyshev_output_spectrum_zoom.svg
+++ b/Chebyshev/low_pass_inversed_chebyshev_output_spectrum_zoom.svg
--- a/report/0_intro/0_intro.pug
+++ b/report/0_intro/0_intro.pug
@ -46,7 +46,7 @@ figure.block-center.width-15cm
 		tbody
 			tr
 				td πόλος
-				td Μπορεί να εννοείται ζεύγος συζηγών πόλων #[br/](έναντι ενός, μοναδικού πόλου)
+				td Μπορεί να εννοείται ζεύγος συζυγών πόλων #[br/](έναντι ενός, μοναδικού πόλου)
 			tr
 				td LP
 				td Low pass filter
@ -68,4 +68,9 @@ figure.block-center.width-15cm
 	figcaption
 		.reference #[span.table-count]
 		.caption.
-			Ειδικοί όροι που χρησιμοποιούνται
+			Ειδικοί όροι που χρησιμοποιούνται.
 br/
 br/
 p.
 	#[strong Σημείωση:] Τα διάγραμμα των οργάνων του Multisim παράχθηκαν στο Matlab, ωστόσο οι τιμές εξάχθηκαν από το Multisim. Αυτό έγινε για παραγωγή καλύτερης ποιότητας διαγραμμάτων σε σχέση με άλλες μεθόδους όπως screenshot. Μετά την διεξαγωγή των πειραμάτων, χρησιμοποιήθηκε το view "Grapher" του Multisim, από το οποίο αποκτήθηκαν αρχεία comma separated values (.csv) για κάθε όργανο, τα οποία περιείχαν τις τιμές των αποτελεσμάτων. Έπειτα τα αρχεία χρησιμοποιήθηκαν στο Matlab για την παραγωγή όμορφων διαγραμμάτων σε μορφή scalable vector graphics (.svg) τα οποία παραμένουν αναλλοίωτα στη μεγέθυνση.
--- a/report/1_low_pass/1_low_pass.pug
+++ b/report/1_low_pass/1_low_pass.pug
@ -5,7 +5,7 @@ br/
 // Chapter description/introduction
 p.
-	Με βάση το ΑΕΜ (8261), υπολογίστηκαν οι προδιαγραφές του κατωδιαβατού φίλτρου προς σχεδίαση:
+	Με βάση τον αριθμό ΑΕΜ (8261), υπολογίστηκαν οι προδιαγραφές του κατωδιαβατού φίλτρου προς σχεδίαση:
 figure.block-center.width-15cm
 	table.ui.celled.table.teal.striped.center.aligned
--- a/report/1_low_pass/1_low_pass_design.pug
+++ b/report/1_low_pass/1_low_pass_design.pug
@ -14,10 +14,11 @@ figure.block-center.width-15cm
 		div.item Κλιμακοποίηση του κυκλώματος με στόχο τη μεταφορά στις πραγματικές συχνότητες και σε στοιχεία με πρακτικές (υλοποιήσιμες) τιμές.
 		div.item Έλεγχος των κερδών των μονάδων και ρύθμιση κέρδους με επιβολή απόσβεσης ή ενίσχυσης.
 div(style="page-break-before:always")
 h4 Υπολογισμός συνάρτησης μεταφοράς
 p.
-	Αρχικά σχεδιάζεται ένα πρότυπο κατωδιαβατό Chebyshev φίλτρο, το οποίο αργότερα να μετατραπεί στο επιθυμητό αντίστροφο Chebyshev.
+	Αρχικά σχεδιάζεται ένα πρότυπο κατωδιαβατό Chebyshev φίλτρο, το οποίο αργότερα θα μετατραπεί στο επιθυμητό αντίστροφο Chebyshev.
 p Γίνεται κανονικοποίηση των συχνοτήτων ώστε να επιτευχθεί Ω#[sub s]=1 rad/s:
@ -49,6 +50,7 @@ p.
 p.latex-equation.
 	$$\Omega_{hp} = \frac{1}{cosh(\frac{1}{n}cosh^{-1}(\frac{1}{\varepsilon}))} = \frac{1}{cosh(\frac{1}{4}cosh^{-1}(\frac{1}{0.065}))} = 0.7196\frac{rad}{s}$$
 div(style="page-break-before:always")
 p και στη συνέχεια μεταφέρεται στη πραγματική συχνότητα:
 p.latex-equation.
@ -92,12 +94,13 @@ p.
 p.latex-equation.
 	$$\omega_{0_k} = \frac{1}{\Omega_{0_k}}$$
 div(style="page-break-before:always")
 p.
 	Από τον μετασχηματισμό προκύπτουν οι πόλοι του #[strong αντίστροφου Chebyshev]:
 p.latex-equation.
-	$$\text{Pole 1: } \Omega_0 = 0.963 \text{, }Q = 0.582$$
+	$$\text{Pole 1: } \omega_0 = 0.963 \text{, }Q = 0.582$$
-	$$\text{Pole 2: } \Omega_0 = 0.748 \text{, }Q = 1.809$$
+	$$\text{Pole 2: } \omega_0 = 0.748 \text{, }Q = 1.809$$
 p.
 	Κατά τον μετασχηματισμό προκύπτουν επίσης, με βάση την εξίσωση #[span.course-notes-equation 9-143]:
@ -122,6 +125,7 @@ figure.block-center.width-19cm
 		.caption.
 			Πόλοι και μηδενικά του αντίστροφου Chebyshev
 div(style="page-break-before:always")
 p.
 	Οι πόλοι και τα μηδενικά ομαδοποιούνται όπως φαίνεται στο παρακάτω διάγραμμα:
@ -182,6 +186,7 @@ figure.block-center.width-15cm
 		.caption.
 			Προδιαγραφές πρώτης μονάδας low pass notch
 div(style="page-break-before:always")
 p.
 	Γίνεται κανονικοποίηση των συχνοτήτων ως προς το ω#[sub 0], ώστε Ω#[sub 0]=1:
@ -221,11 +226,12 @@ p.latex-equation.
 p #[strong Κλιμακοποίηση]
 p.
-	Γίνεται κλιμακωποίηση των στοιχείων της μονάδας για να μεταφερθούν οι συχνότητες στις πραγματικές τιμές. Επιλέγεται:
+	Γίνεται κλιμακoποίηση των στοιχείων της μονάδας για να μεταφερθούν οι συχνότητες στις πραγματικές τιμές. Επιλέγεται:
 p.latex-equation.
 	$$k_{f} = \omega_s\omega_0 = 72570.79*0.963 = 69885.7$$
 div(style="page-break-before:always")
 p.
 	Με βάση τον αριθμό ΑΕΜ (8261) επιλέγεται κατάλληλος συντελεστής κλιμακοποίησης πλάτους ώστε να επιτευχθεί τιμή πυκνωτών ίση με 0.1μF, γίνεται χρήση του τύπου #[span.course-notes-equation 6-33]:
@ -350,7 +356,7 @@ p.latex-equation.
 p #[strong Κλιμακοποίηση]
 p.
-	Γίνεται κλιμακωποίηση των στοιχείων της μονάδας για να μεταφερθούν οι συχνότητες στις πραγματικές τιμές. Επιλέγεται:
+	Γίνεται κλιμακoποίηση των στοιχείων της μονάδας για να μεταφερθούν οι συχνότητες στις πραγματικές τιμές. Επιλέγεται:
 p.latex-equation.
 	$$k_{f} = \omega_s\omega_0 = 72570.79*0.7484 = 54311.9$$
@ -417,7 +423,7 @@ p.
 	Με βάση τον αριθμό ΑΕΜ (8261) πραγματοποιείται ρύθμιση κέρδους με στόχο την επίτευξη κέρδους 0 dB στις χαμηλές συχνότητες.
 p.
-	Κατά την υλοποίηση των μονάδων Fried διαπιστώθηκε ότι κάθε μονάδα εισάγει μία απόσβεση. Κάτι το οποίο ήταν αναμενόμενο με βάση τη θεωρεία των μονάδων αυτών. Το συνολικό κέρδος που εισάγουν οι μονάδες είναι:
+	Κατά την υλοποίηση των μονάδων Fried διαπιστώθηκε ότι κάθε μονάδα εισάγει ένα κέρδος. Κάτι το οποίο ήταν αναμενόμενο με βάση τη θεωρεία των μονάδων αυτών. Το συνολικό κέρδος που εισάγουν οι μονάδες είναι:
 p.latex-equation.
 	$$k = k_{low}^1k_{low}^2 = 0.4411*4.2573 = 1.878$$
@ -477,4 +483,4 @@ figure.block-center.width-19cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.
-			Κύκλωμα κατωδιαβατού φίλτρου
+			Κύκλωμα κατωδιαβατού φίλτρου
--- a/report/1_low_pass/1_low_pass_transfer_function_matlab.pug
+++ b/report/1_low_pass/1_low_pass_transfer_function_matlab.pug
@ -1,12 +1,13 @@
 h3 Μελέτη συνάρτησης μεταφοράς στο Matlab
 p.
-	Η σχεδίαση του φίλτρου έγινε στο λογισμικό Matlab. Σχεδιάστηκαν, με χρήση της συνάρτησης plot_transfer_function που δόθηκε καθώς και της ltiview που παρέχει το λογισμικό, οι αποκρίσεις πλάτους σε dB των επιμέρους μονάδων, καθώς και του συνολικού φίλτρου. Επίσης η συνολική απόκριση του φίλτρου ελέγχθηκαν σε σήμα εισόδου που καθόρισε η εκφώνηση.
+	Η σχεδίαση του φίλτρου έγινε στο λογισμικό Matlab. Σχεδιάστηκαν, με χρήση της συνάρτησης plot_transfer_function που δόθηκε καθώς και της ltiview που παρέχει το λογισμικό, οι αποκρίσεις πλάτους σε dB των επιμέρους μονάδων, καθώς και του συνολικού φίλτρου.
 div(style="page-break-before:always")
 p.
-	Παρακάτω φαίνονται οι αποκρίσεις όπως προέκυψαν στο Matlab από την plot_transfer_function, με ορίσματα κάθε φορά την συνάρτηση μεταφοράς των επί μέρους συστημάτων, καθώς και τυχόν κρίσιμες συχνότητες:
+	Παρακάτω φαίνονται οι αποκρίσεις όπως προέκυψαν στο Matlab από την plot_transfer_function, με ορίσματα κάθε φορά την συνάρτηση μεταφοράς του επί μέρους συστήματος, καθώς και τυχόν κρίσιμες συχνότητες:
-figure.block-center.width-19cm
+figure.block-center.width-15cm
-	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_notch_unit_1_transfer_function.svg").width-19cm
+	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_notch_unit_1_transfer_function.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
@ -14,8 +15,8 @@ figure.block-center.width-19cm
 		.caption.
 			Παρατηρούμε ότι η μονάδα, ορθώς, έχει χαμηλότερη απόκριση στις υψηλές συχνότητες σε σχέση με τις χαμηλές. Στο γράφημα φαίνεται επίσης η απόκριση της συνάρτησης μεταφοράς στις χαμηλές συχνότητες, από όπου μπορούμε να επιβεβαιώσουμε ότι το κέρδος -7,1 dB που υπολογίστηκε νωρίτερα για την μονάδα είναι σωστό.
-figure.block-center.width-19cm
+figure.block-center.width-15cm
-	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_notch_unit_2_transfer_function.svg").width-19cm
+	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_notch_unit_2_transfer_function.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
@ -23,8 +24,8 @@ figure.block-center.width-19cm
 		.caption.
 			Παρατηρούμε ότι η μονάδα, ορθώς, έχει χαμηλότερη απόκριση στις υψηλές συχνότητες σε σχέση με τις χαμηλές. Στο γράφημα φαίνεται επίσης η απόκριση της συνάρτησης μεταφοράς στις χαμηλές συχνότητες, από όπου μπορούμε να επιβεβαιώσουμε ότι το κέρδος 12,6 dB που υπολογίστηκε νωρίτερα για την μονάδα είναι σωστό.
-figure.block-center.width-19cm
+figure.block-center.width-15cm
-	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_total_transfer_function.svg").width-19cm
+	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_total_transfer_function.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
@ -32,15 +33,15 @@ figure.block-center.width-19cm
 		.caption.
 			Παρατηρούμε ότι η συνάρτηση μεταφοράς του φίλτρου έχει το αναμενόμενο σχήμα ενός κατωδιαβατού αντίστροφου Chebyshev φίλτρου. Πιο συγκεκριμένα, στις χαμηλές συχνότητες η συνάρτηση μεταφοράς είναι επίπεδη, ενώ στην αποκοπή εμφανίζει ταλάντωση (ripples). Μάλιστα ο αριθμός των ripples (δύο) είναι σωστός με βάση τη τάξη του φίλτρου (τέταρτης τάξης) και τη θεωρία του αντίστροφου Chebyshev. Στο γράφημα φαίνεται επίσης η απόκριση της συνάρτησης μεταφοράς στις κρίσιμες συχνότητες: (τυχαία) χαμηλή συχνότητα=10 Hz, f#[sub p]=5500 Hz, f#[sub hp]=8313.16 Hz και f#[sub s]=11550 Hz.
-figure.block-center.width-19cm
+figure.block-center.width-15cm
-	img(src="1_low_pass/assets/diagrams/matlab_combined_transfer_functions_bode.svg").width-19cm
+	img(src="1_low_pass/assets/diagrams/matlab_combined_transfer_functions_bode.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
-			Συνδυαστηκό γράφημα συναρτήσεων μεταφοράς επιμέρους μονάδων και συνολικού φίλτρου.
+			Συνδυαστικό γράφημα συναρτήσεων μεταφοράς επιμέρους μονάδων και συνολικού φίλτρου.
-figure.block-center.width-19cm
+figure.block-center.width-15cm
-	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_total_attenuation.svg").width-19cm
+	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_total_attenuation.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
@ -49,16 +50,16 @@ figure.block-center.width-19cm
 			Στο γράφημα φαίνεται η απόσβεση του φίλτρου για τις κρίσιμες συχνότητες: (τυχαία) χαμηλή συχνότητα=10 Hz, f#[sub p]=5500 Hz, f#[sub hp]=8313.16 Hz και f#[sub s]=11550 Hz.
 p.
-	Στα γραφήματα 2.2.3 και 2.2.5 έχουν σημειωθεί οι κρίσιμες συχνότητες οι οποίες καθορίζουν την ζώνη διόδου και αποκοπής, δηλαδή η f#[sub p]=5500 Hz και η f#[sub s]=11550 Hz, καθώς και οι αντίστοιχες αποσβέσεις. Παρατηρούμε ότι η απόκριση του φίλτρου στην ζώνη διόδου είναι 0.07 dB, ενώ στη ζώνη αποκοπής είναι 23.75 dB. Επομένως είναι φανερό ότι πληρείται ακριβώς η προδιαγραφή a#[sub min]=23.75 dB ενώ η προδιαγραφή a#[sub max]=0.35 dB υπερκαλύπτεται.
+	Στα γραφήματα 2.2.3 και 2.2.5 έχουν σημειωθεί οι κρίσιμες συχνότητες οι οποίες καθορίζουν την ζώνη διόδου και αποκοπής, δηλαδή η f#[sub p]=5500 Hz και η f#[sub s]=11550 Hz, καθώς και οι αντίστοιχες αποσβέσεις. Παρατηρούμε ότι η απόκριση του φίλτρου στην ζώνη διόδου είναι 0.07 dB, ενώ στη ζώνη αποκοπής είναι 23.75 dB. Επομένως είναι φανερό ότι πληρείτε ακριβώς η προδιαγραφή a#[sub min]=23.75 dB ενώ η προδιαγραφή a#[sub max]=0.35 dB υπερκαλύπτεται.
 p.
-	Πριν τη ρύθμιση κέρδους η συνάρτηση απόσβεσης δίνεται από το παρακάτω διάγραμμα:
+	Η συνάρτηση απόσβεσης, πριν τη ρύθμιση κέρδους, δίνεται από το παρακάτω διάγραμμα:
-figure.block-center.width-19cm
+figure.block-center.width-15cm
-	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_original_gain_attenuation.svg").width-19cm
+	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inverse_chebyshev_original_gain_attenuation.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Απόσβεση φίλτρου πριν τη ρύθμιση κέρδους.
 		.caption.
-			Στο γράφημα σημειώνονται οι ίδιες κρίσιμες συχνότητες: (τυχαία) χαμηλή συχνότητα=10 Hz, f#[sub p]=5500 Hz, f#[sub hp]=8313.16 Hz και f#[sub s]=11550 Hz.
+			Στο γράφημα σημειώνονται οι ίδιες κρίσιμες συχνότητες: (τυχαία) χαμηλή συχνότητα=10 Hz, f#[sub p]=5500 Hz, f#[sub hp]=8313.16 Hz και f#[sub s]=11550 Hz.
--- a/report/1_low_pass/1_low_pass_transfer_function_multisim.pug
+++ b/report/1_low_pass/1_low_pass_transfer_function_multisim.pug
@ -1,7 +1,7 @@
 h3 Υλοποίηση κυκλώματος στο Multisim
 p.
 	Το κύκλωμα του φίλτρου που σχεδιάστηκε προηγουμένως, εισάγεται στο λογισμικό Multisim όπου θα ελεγχθεί η ορθότητα της σχεδίασης του μέσω διάφορων πειραμάτων και θα εξαχθούν χρήσιμα συμπεράσματα για τη λειτουργία του φίλτρου.
-	Το κύκλωμα, μαζί με τα διάφορα εργαλεία που χρησιμοποιούνται για τον έλεγχό του φαίνεται στο επόμενο σχηματικό:
+	Το κύκλωμα, μαζί με τα διάφορα εργαλεία που χρησιμοποιούνται για τον έλεγχό του, φαίνεται στο επόμενο σχηματικό:
 figure.block-center.width-19cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inverse_chebyshev_layout.svg").width-19cm
@ -13,10 +13,10 @@ figure.block-center.width-19cm
 			Εκτός από το κύκλωμα του φίλτρου, το σχηματικό περιλαμβάνει ένα bode plotter (XBP1), δύο spectrum analyzers (XSA1 και XSA2) και ένα oscilloscope (XSC1) για την καταγραφή των εισόδων και εξόδων του φίλτρου. Επίσης έχουν τοποθετηθεί μία πηγή στοιχειώδους περιοδικού σήματος (V1), μία πηγή τετραγωνικών παλμών (V2) και ένας διακόπτης (S1) για την επιλογή του σήματος εισόδου.
 p.
-	Ο διακόπτης S1 τοποθετείται στην αριστερή επαφή ώστε να επιλεγχθεί ως σήμα εισόδου του φίλτρου το στοιχειώδες ημιτονοειδές σήμα της πηγής V1 με χαρακτηριστικά Vpp=1 V, f=1 kHz. Χρησιμοποιώντας το εργαλείο bode plotter, εξάγεται η απόκριση συχνότητας του κυκλώματος. Το διάγραμμα και οι επιλεγμένες τιμές του εργαλείου φαίνονται παρακάτω:
+	Ο διακόπτης S1 τοποθετείται στην αριστερή επαφή ώστε να επιλεχθεί ως σήμα εισόδου του φίλτρου το στοιχειώδες ημιτονοειδές σήμα της πηγής V1 με χαρακτηριστικά Vpp=1 V, f=1 kHz. Χρησιμοποιώντας το εργαλείο bode plotter (XBP1), εξάγεται η απόκριση συχνότητας του κυκλώματος. Το διάγραμμα και οι επιλεγμένες τιμές του εργαλείου φαίνονται παρακάτω:
-figure.block-center.width-19cm
+figure.block-center.width-15cm
-	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_bode_plotter.svg").width-19cm
+	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_bode_plotter.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
@ -28,5 +28,169 @@ figure.block-center.width-19cm
 			#[br/]#[strong Vertical:] Log με #[strong F:] 0 dB και #[strong I:] -200 dB
 			#[br/]#[strong Set...] με #[strong Resolution points:] 1000
 p.
 	Το παρακάτω διάγραμμα είναι ίδιο με το προηγούμενο, σημειώνονται όμως οι αποκρίσεις στις κρίσιμες συχνότητες:
 figure.block-center.width-15cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_bode_plotter_with_values.svg").width-15cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Έξοδος bode plotter-XBP1 κατωδιαβατού αντίστροφου Chebyshev φίλτρου από το Multisim με σημειωμένες τις αποκρίσεις στις κρίσιμες συχνότητες.
 		.caption.
 			Οι επιλογές του bode plotter που χρησιμοποιήθηκαν:
 			#[br/]#[strong Mode:] Magnitude
 			#[br/]#[strong Horizontal:] Log με #[strong F:] 1 MHz και #[strong I:] 10 Hz
 			#[br/]#[strong Vertical:] Log με #[strong F:] 0 dB και #[strong I:] -200 dB
 			#[br/]#[strong Set...] με #[strong Resolution points:] 1000
 			#[br/]Οι συχνότητες που σημειώνονται είναι f#[sub p]=5500 Hz, f#[sub hp]=8313.16 Hz και f#[sub s]=11550 Hz.
 p.
 	Από το διάγραμμα 2.3.3 γίνεται φανερό ότι η ανάλυση του κυκλώματος στο Multisim συμφωνεί με τη θεωρητική ανάλυση που προηγήθηκε κάθως και την ανάλυση που έγινε χρησιμοποιώντας το Matlab. Παρατηρούνται ωστόσο μικρές αποκλίσεις, της τάξης 10#[sup -3], οι οποίες αποδίδονται στο γεγονός ότι οι τιμές των στοιχείων που χρησιμοποιήθηκαν στο Multisim έχουν μικρότερη ακρίβεια από ότι οι αντίστοιχες τιμές στην ανάλυση στο Matlab.
 p.
 	Ο διακόπτης S1 τοποθετείται τώρα στην δεξιά επαφή ώστε να επιλεχθεί ως σήμα εισόδου του φίλτρου ο τετραγωνικός παλμός της πηγής V2 με χαρακτηριστικά V#[sub 0]=0 V, Vp=1 V, f=2 kHz, duty cycle ίσο με 40%. Χρησιμοποιώντας το εργαλείο oscilloscope (XSC1), εξάγεται η κυματομορφή του σήματος εισόδου. Το διάγραμμα και οι επιλεγμένες τιμές του εργαλείου φαίνονται παρακάτω:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_oscilloscope_input_sig.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Έξοδος oscilloscope-XSC1 (μόνο channel A) κατωδιαβατού αντίστροφου Chebyshev φίλτρου από το Multisim.
 		.caption.
 			Οι επιλογές του oscilloscope που χρησιμοποιήθηκαν:
 			#[br/]#[strong Timebase:] #[strong Scale:] 500 us/Div, #[strong X pos.:] 0 και #[strong mode:] Y/T
 			#[br/]#[strong Channel:] #[strong Scale:] 500 mV/Div, #[strong Y pos.:] 0 και #[strong mode:] DC
 p.
 	Χρησιμοποιώντας το ίδιο εργαλείο (XSC1), εξάγεται η κυματομορφή της εξόδου. Το διάγραμμα και οι επιλεγμένες τιμές του εργαλείου φαίνονται παρακάτω:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_oscilloscope_output_sig.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Έξοδος oscilloscope-XSC1 (μόνο channel B) κατωδιαβατού αντίστροφου Chebyshev φίλτρου από το Multisim.
 		.caption.
 			Οι επιλογές του oscilloscope που χρησιμοποιήθηκαν:
 			#[br/]#[strong Timebase:] #[strong Scale:] 500 us/Div, #[strong X pos.:] 0 και #[strong mode:] Y/T
 			#[br/]#[strong Channel:] #[strong Scale:] 500 mV/Div, #[strong Y pos.:] 0 και #[strong mode:] DC & -
 p.
 	Χρησιμοποιώντας και τα δύο κανάλια του εργαλείου (XSC1), εξάγεται η κυματομορφή της εισόδου και της εξόδου στο ίδιο διάγραμμα. Το διάγραμμα και οι επιλεγμένες τιμές του εργαλείου φαίνονται παρακάτω:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_oscilloscope_combined_input_output_sig.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Έξοδος oscilloscope-XSC1 κατωδιαβατού αντίστροφου Chebyshev φίλτρου από το Multisim.
 		.caption.
 			Οι επιλογές του oscilloscope που χρησιμοποιήθηκαν:
 			#[br/]#[strong Timebase:] #[strong Scale:] 500 us/Div, #[strong X pos.:] 0 και #[strong mode:] Y/T
 			#[br/]#[strong Channel A:] (input signal) #[strong Scale:] 500 mV/Div, #[strong Y pos.:] 0 και #[strong mode:] DC
 			#[br/]#[strong Channel B:] (output signal) #[strong Scale:] 500 mV/Div, #[strong Y pos.:] 0 και #[strong mode:] DC & -
 p.
 	Στα παραπάνω διαγράμματα μπορούμε να δούμε αναλυτικά τα σήματα εισόδου και εξόδου στο χρόνο. Στις περιγραφές των διαγραμμάτων φαίνονται οι επιλογές που έγιναν στον παλμογράφο για να προκύψουν οι αντίστοιχες παραστάσεις.
 p.
 	Η συνολική απόκριση του φίλτρου στο σήμα εισόδου (τετραγωνικός παλμός) που καθόρισε η εκφώνηση, ελέγχθηκε στο λογισμικό Matlab. Η είσοδος και η έξοδος του φίλτρου στο χρόνο, όπως προέκυψαν στο Matlab, φαίνονται στο παρακάτω διάγραμμα:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inversed_chebyshev_combined_input_output_sig.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Σήματα εισόδου και εξόδου στο χρόνο, διάγραμμα από Matlab.
 		.caption.
 			Παρατηρείται ότι τα σήματα συμφωνούν με αυτά του Multisim.
 p.
 	Χρησιμοποιήθηκαν οι εντολές fft και lsim που παρέχονται από το λογισμικό για να εξαχθεί η απόκριση και στη συνέχεια το φάσμα της απόκρισης τόσο για την είσοδο όπως και για την έξοδο. Το φάσμα του σήματος εισόδου φαίνεται στο παρακάτω διάγραμμα:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inversed_chebyshev_input_spectrum.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Φάσμα σήματος εισόδου, διάγραμμα από Matlab.
 p.
 	Στο επόμενο διάγραμμα φαίνεται και πάλι το φάσμα του σήματος εισόδου με μεγέθυνση στη περιοχή ενδιαφέροντος:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inversed_chebyshev_input_spectrum_zoom.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Φάσμα σήματος εισόδου, διάγραμμα από Matlab.
 div(style="page-break-before:always")
 p.
 	Το φάσμα του σήματος εξόδου φαίνεται στο παρακάτω διάγραμμα:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inversed_chebyshev_output_spectrum.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Φάσμα σήματος εξόδου, διάγραμμα από Matlab.
 p.
 	Στο επόμενο διάγραμμα φαίνεται και πάλι το φάσμα του σήματος εξόδου με μεγέθυνση στη περιοχή ενδιαφέροντος:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/matlab_low_pass_inversed_chebyshev_output_spectrum_zoom.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Φάσμα σήματος εξόδου, διάγραμμα από Matlab.
 p.
 	Η ίδια απόκριση ελέγχθηκε και στο Multisim. Διατηρώντας τον διακόπτη S1 στη δεξιά επαφή, χρησιμοποιείται το εργαλείο spectrum analyzer (XSA1) για να εξαχθεί το φάσμα εισόδου. Το διάγραμμα και οι επιλεγμένες τιμές του εργαλείου φαίνονται παρακάτω:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_spectrum_analyzer_input.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Φάσμα σήματος εισόδου, έξοδος spectrum analyzer-XSA1 από Multisim.
 		.caption.
 			Οι επιλογές του spectrum analyzer που χρησιμοποιήθηκαν:
 			#[br/]#[strong Frequency:] #[strong Span:] 20 kHz, #[strong Start:] 0 Hz, #[strong Center:] 10 kHz και #[strong End:] 20 kHz
 			#[br/]#[strong Amplitude:] #[strong lin] και #[strong Range:] 0.1 V/Div
 			#[br/]#[strong Resolution freq.:] 100 Hz
 p.
 	Με τον ίδιο τρόπο, χρησιμοποιείται το εργαλείο spectrum analyzer (XSA2) για να εξαχθεί το φάσμα εξόδου. Το διάγραμμα και οι επιλεγμένες τιμές του εργαλείου φαίνονται παρακάτω:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_spectrum_analyzer_output.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Φάσμα σήματος εξόδου, έξοδος spectrum analyzer-XSA2 από Multisim.
 		.caption.
 			Οι επιλογές του spectrum analyzer που χρησιμοποιήθηκαν:
 			#[br/]#[strong Frequency:] #[strong Span:] 20 kHz, #[strong Start:] 0 Hz, #[strong Center:] 10 kHz και #[strong End:] 20 kHz
 			#[br/]#[strong Amplitude:] #[strong lin] και #[strong Range:] 0.1 V/Div
 			#[br/]#[strong Resolution freq.:] 100 Hz
 div(style="page-break-before:always")
 p.
 	Τα δύο παραπάνω διαγράμματα συνδυάστηκαν σε ένα για ευκολότερη εξαγωγή συμπερασμάτων:
 figure.block-center.width-17cm
 	img(src="1_low_pass/assets/diagrams/multisim_low_pass_inversed_chebyshev_spectrum_analyzer_combined_input_output.svg").width-17cm
 	figcaption
 		.reference #[span.plot-count]
 		.caption.title.
 			Φάσματα σημάτων εισόδου και εξόδου, εξόδου spectrum analyzers-XSA1 και XSA2 από Multisim.
 p.
 	Από τα παραπάνω διαγράμματα συμπεραίνουμε καταρχάς ότι η ανάλυση του φίλτρου που έγινε στο Matlab συμφωνεί με αυτή που έγινε στο Multisim. Το συμπέρασμα αυτό προέρχεται από το γεγονός ότι τα φάσματα εισόδου και εξόδου του σήματος εισόδου και εξόδου του φίλτρου είναι ίδια στα δύο πειράματα.
 p.
 	Επίσης από τα φάσματα και κυρίως από το τελευταίο διάγραμμα (2.3.14) γίνεται εύκολα αντιληπτό ότι το κύκλωμα που σχεδιάστηκε υλοποιεί επιτυχώς το επιθυμητό κατωδιαβατό φίλτρο.
 p.
 	Πιο συγκεκριμένα παρατηρείται ότι το φάσμα εξόδου είναι ίδιο με το φάσμα εισόδου στις χαμηλές συχνότητες, δηλαδή στη ζώνη διόδου μέχρι τα 5500 Hz. Ταυτόχρονα, οι συχνότητες της ζώνης αποκοπής, πάνω από 11550 Hz, υπέστησαν τόσο σημαντική απόσβεση, ώστε σχεδόν να μη φαίνονται στο φάσμα εξόδου, δείχνοντας ότι οι υψηλές συχνότητες κόβονται από το κύκλωμα. Τέλος σημειώνεται ότι η συχνότητα των 8000 Hz, η οποία βρίσκεται μέσα στη ζώνη μετάβασης του φίλτρου, έχει επίσης υποστεί κάποια απόσβεση, είναι όμως εμφανής και στο φάσμα εξόδου.
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 		<text transform="matrix(1 0 0 1 640 -41)" class="st2 st3">1.4</text>
 	</g>
 	<g transform="translate(1440.4,828.952)">
 		<text transform="matrix(1 0 0 1 640 -41)" class="st2 st3">1.6</text>
 	</g>
 	<g transform="translate(1589.2,828.952)">
 		<text transform="matrix(1 0 0 1 640 -41)" class="st2 st3">1.8</text>
 	</g>
 	<g transform="translate(1738,828.952)">
 		<text transform="matrix(1 0 0 1 648 -41)" class="st2 st3">2</text>
 	</g>
 	<g transform="translate(994.0007,856.952)">
 		<text transform="matrix(1 0 0 1 578 -39)" class="st2 st4">Frequency (Hz)</text>
 	</g>
 	<g transform="translate(1690,884)">
 		<text transform="matrix(1 0 0 1 654 -62)" class="st2 st3">#</text>
 	</g>
 	<g transform="translate(1706,884)">
 		<text transform="matrix(1 0 0 1 654 -62)" class="st2 st3">10</text>
 	</g>
 	<g transform="translate(1729,874)">
 		<text transform="matrix(1 0 0 1 654 -62)" class="st2 st5">4</text>
 	</g>
 	<g>
 		<line class="st1" x1="904" y1="753" x2="904" y2="7"/>
 		<line class="st1" x1="910" y1="753" x2="898" y2="753"/>
 		<line class="st1" x1="910" y1="659.8" x2="898" y2="659.8"/>
 		<line class="st1" x1="910" y1="566.5" x2="898" y2="566.5"/>
 		<line class="st1" x1="910" y1="473.3" x2="898" y2="473.3"/>
 		<line class="st1" x1="910" y1="380" x2="898" y2="380"/>
 		<line class="st1" x1="910" y1="286.8" x2="898" y2="286.8"/>
 		<line class="st1" x1="910" y1="193.5" x2="898" y2="193.5"/>
 		<line class="st1" x1="910" y1="100.3" x2="898" y2="100.3"/>
 		<line class="st1" x1="910" y1="7" x2="898" y2="7"/>
 	</g>
 	<g transform="translate(236.048,815)">
 		<text transform="matrix(1 0 0 1 642 -54)" class="st2 st3">0</text>
 	</g>
 	<g transform="translate(236.048,721.75)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.1</text>
 	</g>
 	<g transform="translate(236.048,628.5)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.2</text>
 	</g>
 	<g transform="translate(236.048,535.25)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.3</text>
 	</g>
 	<g transform="translate(236.048,442)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.4</text>
 	</g>
 	<g transform="translate(236.048,348.75)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.5</text>
 	</g>
 	<g transform="translate(236.048,255.5)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.6</text>
 	</g>
 	<g transform="translate(236.048,162.25)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.7</text>
 	</g>
 	<g transform="translate(236.048,69)">
 		<text transform="matrix(1 0 0 1 626 -54)" class="st2 st3">0.8</text>
 	</g>
 	<g transform="translate(202.048,441.9996) rotate(-90)">
 		<text transform="matrix(1 0 0 1 -5.0004 649)" class="st2 st4">Amplitude (V)</text>
 	</g>
 	<g transform="translate(994.0009,66.25)">
 		<text transform="matrix(1 0 0 1 532.5 -67)" class="st6 st4">Spectrum analyzer plot</text>
 	</g>
 	<g>
 		<path class="st7" d="M904,380.3l7.4,372.7h7.4h7.4l7.4-0.6l7.4,0.6h7.4h7.4l7.4-0.4l7.4,0.4h7.4h7.4l7.4-0.1l7.4,0.1h7.4h7.4
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 </g>
 </svg>
--- a/report/diagrams/diagram.mermaid
+++ b/report/diagrams/diagram.mermaid
@ -1,6 +0,0 @@
 graph LR
  mermaid --> svg
  vega-lite --> svg
  svg --> html
  pug --> html
  html -->|Chrome| pdf
--- a/report/diagrams/diagram.svg
+++ b/report/diagrams/diagram.svg
--- a/report/diagrams/plot.svg
+++ b/report/diagrams/plot.svg
--- a/report/diagrams/plot.vegalite.json
+++ b/report/diagrams/plot.vegalite.json
@ -1,18 +0,0 @@
 {
  "$schema": "https://vega.github.io/schema/vega-lite/v2.0.json",
  "data": {
    "values": [
      {"a": "A","b": 28}, {"a": "B","b": 55}, {"a": "C","b": 43},
      {"a": "D","b": 91}, {"a": "E","b": 81}, {"a": "F","b": 53},
      {"a": "G","b": 19}, {"a": "H","b": 87}, {"a": "I","b": 52},
      {"a": "J","b": 19}, {"a": "K","b": 87}, {"a": "L","b": 52},
      {"a": "M","b": 19}, {"a": "N","b": 87}, {"a": "O","b": 52}
    ]
   },
  "mark": "bar",
  "encoding": {
    "x": {"field": "a", "type": "ordinal"},
    "y": {"field": "b", "type": "quantitative"},
    "color": {"value": "#b4588c"}
  }
 }