FORMULARIO PARA OBTENER LA RESISTENCIA A TIERRA

FORMULARIO PARA OBTENER LA RESISTENCIA A TIERRA - MathCAD 2000 Pro Por Roberto Ruelas-Gómez. Universidad DeLaSalle Bajío. León, Gto. México 071219 r.r

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FORMULARIO PARA OBTENER LA RESISTENCIA A TIERRA - MathCAD 2000 Pro Por Roberto Ruelas-Gómez. Universidad DeLaSalle Bajío. León, Gto. México 071219 [email protected] _______________________________________________________________________________________ NOTA: Estos valores son válidos solamente cuando la corriente a tierra es de naturaleza estacionaria (c.d.) o casi estacionaria (50-60 Hz). Datos del Terreno: ρ = Resistividad (Ω-m) ρs = Resistividad superficial (Ω-m) H = Espesor de la capa superficial (m) Datos de las varillas electrodo: r = radio (m) L = largo (m) d = espaciamiento (m) r1 = radio (m) de la capa de material de resistividad ρ1 (Ω-m), rodeando al electrodo

Datos del conductor enterrado: a = radio (m) B = longitud total (m) S = profundidad (m) w = ancho del concreto conductor D = diámetro del anillo descrito g = separación entre electrodos de concreto Datos de la malla: l1 = longitud del lado corto (m) l2 = longitud del lado largo (m) n = número de varillas dentro de A A = área total (m2) encerrada dentro de la malla.

ρ := 100 ⋅ ohm ⋅ m ρs := 10000 ⋅ ohm ⋅ m H := 0.60 ⋅ m r := 0.008 ⋅ m L := 3 ⋅ m d := 10 ⋅ m r1 := 0.1524 ⋅ m ρ1 := 0.25 ⋅ ohm ⋅ m

bentonita => 0.25 ohm*m [6.2] concreto enterrado => 30 ohm*m

a := 0.0064 ⋅ m

4/0 AWG => 0.0064 m

B := 20 ⋅ m S := 0.5 ⋅ m w := 0.5m D := 10 ⋅ m g := 5 ⋅ m L1 := 20 ⋅ m L2 := 30 ⋅ m n := 6 A := 600 ⋅ m ⋅ m

L1 * L2 solo en mallas rectangulares.

1. VARILLAS ELECTRODO 1.1 UNA VARILLA electrodo de longitud L, radio r enterrada en un terreno de resistividad ρ. Uso: General L = 3m r = 0.008 m

H.B.Dwight [6.1]

  L  − 1 = 33.493 Ω   2⋅ π ⋅L   r   ρ

⋅  ln  4 ⋅

ρ = 100 Ω ⋅ m R. Rüdenberg [6.3]

ρ 2⋅ π ⋅L

 L  = 35.121 Ω   r

⋅ ln  2 ⋅

Sankosha [6.7]

ρ 2.73 ⋅ L

 L  = 35.105 Ω   r

⋅ log  2 ⋅

1.2 DOS VARILLAS electrodo de longitud L y radio r enterradas con un espaciamiento d en un terreno de resistividad ρ, conectadas en paralelo. Uso: General

L = 3m r = 0.008 m

2 4  ρ L 2 ⋅ L    L  − 1 ⋅1 − + = 17.521 Ω  + 2 4 4⋅ π ⋅L   r   4 ⋅ π ⋅ d  3⋅d 5 ⋅ d 

ρ

d>L H.B.Dwight [6.1]

d = 10 m ρ = 100 Ω ⋅ m

⋅  ln  4 ⋅

2 4   L  d d d  ⋅ L + − + = 17.796 Ω + ln 4 − 2    4⋅ π ⋅L   r  d 2 ⋅ L 16 ⋅ L2 512 ⋅ L4    

ρ

d

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