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calculator:current_loop_rectangular_axis [2025/01/13 23:30] stan_zurekcalculator:current_loop_rectangular_axis [2025/01/18 23:01] (current) stan_zurek
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 ==== Calculator of H along axis of rectangular current loop ==== ==== Calculator of H along axis of rectangular current loop ====
  
-|< 100% >| +<box 100% #efffef> 
-| //[[user/Stan Zurek]], Calculator of H along axis of rectangular current loop, Encyclopedia Magnetica//, \\ @PAGEL@, {accessed: @YEAR@-@MONTH@-@DAY@} | +|< 100% 10% 90% >| 
- +|  {{/calculator/icon_calc.png?60&nolink}}  | //[[user/Stan Zurek]], Calculator of H along axis of rectangular current loop, Encyclopedia Magnetica//, \\ @PAGEL@, {accessed: @YEAR@-@MONTH@-@DAY@} | 
-{{page>insert/calc}}+</box>
  
-<box 30% right #f0f0f0>+<box 25% right #f0f0f0>
 [[/Rectangular current loop]] [[/Rectangular current loop]]
 [[file/current_loop_rectangular_magnetica_png|{{/current_loop_rectangular_magnetica.png}}]] [[file/current_loop_rectangular_magnetica_png|{{/current_loop_rectangular_magnetica.png}}]]
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 ^  [[/Magnetic field strength]] //H// of rectangular [[/current loop]] along its axis  ^^ ^  [[/Magnetic field strength]] //H// of rectangular [[/current loop]] along its axis  ^^
 +| //Source: [1] [[https://isbnsearch.org/isbn/9780122572517|Fausto Fiorillo, Measurement and Characterization of Magnetic Materials, Academic Press, 2005, ISBN 9780122572517]]//  ||
 +| //[1], eq. (4.6), p. 108  (converted by [[/user/Stan Zurek]] to use notation will full length of sides)//  |
 | $$ H(t,x) = I(t)· \frac{2}{π}·\frac{a·b}{\sqrt{4·x^2 + a^2 + b^2} }·\left(\frac{1}{4·x^2 + a^2} + \frac{1}{4·x^2 + b^2}  \right) $$ |  (A/m)  |  | $$ H(t,x) = I(t)· \frac{2}{π}·\frac{a·b}{\sqrt{4·x^2 + a^2 + b^2} }·\left(\frac{1}{4·x^2 + a^2} + \frac{1}{4·x^2 + b^2}  \right) $$ |  (A/m)  | 
 | where: $I(t)$ - current (A) at time $t$ (s), $a$ and $b$ - length of sides of the rectangular loop (m), $x$ - location (m) from the centre of the loop (the centre is located at point //x// = 0); assuming infinitely thin wire and a rectangular loop placed in a [[/uniform]] medium; (use $a=b$ for a square loop)  || | where: $I(t)$ - current (A) at time $t$ (s), $a$ and $b$ - length of sides of the rectangular loop (m), $x$ - location (m) from the centre of the loop (the centre is located at point //x// = 0); assuming infinitely thin wire and a rectangular loop placed in a [[/uniform]] medium; (use $a=b$ for a square loop)  ||
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 // calculate the main function // calculate the main function
-result1 = current * (2/pi) * a * b / Math.pow((4*x*x + a*a + b*b),0.5) * (1/(4*x*x + a*a) + 1/(4*x*x + b*b))+result1 = current * 2 * a * b / Math.pow( (4*x*x + a*a + b*b),0.5) * ( 1/(4*x*x + a*a) + 1/(4*x*x + b*b) ) /pi
  
 // format number to x digits precision, otherwise result will equal 5.611e+2 // format number to x digits precision, otherwise result will equal 5.611e+2
-result1 = result1.toPrecision(4)+result1 = result1.toPrecision(5)
  
 // display result // display result
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 </HTML> </HTML>
  
-<WRAP lo right>//[[https://www.e-magnetica.pl/doku.php/calculator/current_loop_rectangular_axis|[open]]]//</WRAP+<box 100% #efffef></box
- +{{page>insert/paypal}}
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 {{tag>Calculators}} {{tag>Calculators}}
calculator/current_loop_rectangular_axis.1736807435.txt.gz · Last modified: 2025/01/13 23:30 by stan_zurek

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