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Hydraulic elements in series and parallel

Storyboard

When hydraulic elements are connected in series, the flow remains constant, but each hydraulic element experiences a pressure drop. The sum of these pressure drops equals the total drop, and therefore, the total hydraulic resistance is equal to the sum of all individual hydraulic resistances. On the other hand, the inverse of the total hydraulic conductivity is equal to the sum of the inverses of the hydraulic conductivities.

>Model

ID:(2109, 0)



Mechanisms

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Code
Concept

Mechanisms

ID:(15955, 0)



Hydraulic resistance of series and parallel elements

Concept

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In the case of a sum where the elements are connected in series, the total hydraulic resistance of the system is calculated by summing the individual resistances of each element.



One way to model a tube with varying cross-section is to divide it into sections with constant radius and then sum the hydraulic resistances in series. Suppose we have a series of the hydraulic resistance in a network (R_{hk}), which depends on the viscosity (\eta), the cylinder k radio (R_k), and the tube k length (\Delta L_k) via the following equation:

R_h =\displaystyle\frac{8 \eta | \Delta L | }{ \pi R ^4}



In each segment, there will be a pressure difference in a network (\Delta p_k) with the hydraulic resistance in a network (R_{hk}) and the volume flow (J_V) to which Darcy's Law is applied:

\Delta p_1 = R_{pt} J_{Vt}



the total pressure difference (\Delta p_t) will be equal to the sum of the individual pressure difference in a network (\Delta p_k):

\Delta p_t =\displaystyle\sum_k \Delta p_k



therefore,

\Delta p_t=\displaystyle\sum_k \Delta p_k=\displaystyle\sum_k (R_{hk}J_V)=\left(\displaystyle\sum_k R_{hk}\right)J_V\equiv R_{st}J_V



Thus, the system can be modeled as a single conduit with the hydraulic resistance calculated as the sum of the individual components:

R_{st} =\displaystyle\sum_k R_{hk}

ID:(15957, 0)



Model

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Parameters

Symbol
Text
Variable
Value
Units
Calculate
MKS Value
MKS Units
R_{h1}
R_h1
Hydraulic Resistance 1
kg/m^4s
R_{h2}
R_h2
Hydraulic Resistance 2
kg/m^4s
R_{h3}
R_h3
Hydraulic Resistance 3
kg/m^4s
R_{pt}
R_pt
Total hydraulic resistance in parallel
kg/m^4s
R_{st}
R_st
Total hydraulic resistance in series
kg/m^4s

Variables

Symbol
Text
Variable
Value
Units
Calculate
MKS Value
MKS Units
J_{Vt}
J_Vt
Flujo de Volumen Total
m^3/s
\Delta p_1
Dp_1
Pressure Difference 1
Pa
\Delta p_3
Dp_3
Pressure Difference 3
Pa
\Delta p_t
Dp_t
Total pressure difference
Pa
J_{V1}
J_V1
Volume flow 1
m^3/s
J_{V2}
J_V2
Volume flow 2
m^3/s

Calculations


First, select the equation: to , then, select the variable: to
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

Calculations

Symbol
Equation
Solved
Translated

Calculations

Symbol
Equation
Solved
Translated

Variable Given Calculate Target : Equation To be used
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2




Equations

#
Equation

\Delta p_t = R_{st} J_{Vt}

Dp = R_h * J_V


\Delta p_1 = R_{pt} J_{Vt}

Dp = R_h * J_V


\Delta p_3 = R_{h3} J_{Vt}

Dp = R_h * J_V


\Delta p_1 = R_{h1} J_{V1}

Dp = R_h * J_V


\Delta p_1 = R_{h2} J_{V2}

Dp = R_h * J_V


\Delta p_t = \Delta p_1 + \Delta p_3

Dp_t = Dp_1 + Dp_2


J_{Vt} = J_{V1} + J_{V2}

J_Vt = J_V1 + J_V2


R_{st} = R_{pt} + R_{h3}

R_st = R_h1 + R_h2


\displaystyle\frac{1}{ R_{pt} }=\displaystyle\frac{1}{ R_{h1} }+\displaystyle\frac{1}{ R_{h2} }

1/ R_pt =1/ R_h1 +1/ R_h2

ID:(15956, 0)



Sum of resistors in series (2)

Equation

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The series combination of the hydraulic Resistance 1 (R_{h1}) and the hydraulic Resistance 2 (R_{h2}) results in a total sum of the total hydraulic resistance in series (R_{st}):

R_{st} = R_{pt} + R_{h3}

R_{st} = R_{h1} + R_{h2}

R_{h1}
R_{pt}
Total hydraulic resistance in parallel
kg/m^4s
5429
R_{h2}
R_{h3}
Hydraulic Resistance 3
kg/m^4s
5427
R_{st}
Total hydraulic resistance in series
kg/m^4s
5428
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

ID:(3854, 0)



Sum of resistors in parallel (2)

Equation

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The parallel combination of the hydraulic Resistance 1 (R_{h1}) and the hydraulic Resistance 2 (R_{h2}) results in a total equivalent of the total hydraulic resistance in series (R_{st}):

\displaystyle\frac{1}{ R_{pt} }=\displaystyle\frac{1}{ R_{h1} }+\displaystyle\frac{1}{ R_{h2} }

R_{h1}
Hydraulic Resistance 1
kg/m^4s
5425
R_{h2}
Hydraulic Resistance 2
kg/m^4s
5426
R_{pt}
Total hydraulic resistance in parallel
kg/m^4s
5429
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

ID:(3858, 0)



Total Pressure difference of series resistors (2)

Equation

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In the case of hydraulic resistances in series, the pressure drops across each of them, and the sum of these pressure drops is equal to the total pressure difference across the entire series.

For two resistances in series, the hydraulic Resistance 1 (R_{h1}) and the hydraulic Resistance 2 (R_{h2}), with their respective pressure drops the pressure Difference 1 (\Delta p_1) and the pressure Difference 2 (\Delta p_2), the sum of these drops equals the total pressure difference the total pressure difference (\Delta p_t):

\Delta p_t = \Delta p_1 + \Delta p_3

\Delta p_t = \Delta p_1 + \Delta p_2

\Delta p_1
Pressure Difference 1
Pa
9841
\Delta p_2
\Delta p_3
Pressure Difference 3
Pa
5447
\Delta p_t
Total pressure difference
Pa
9842
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

ID:(9943, 0)



Total flow (2)

Equation

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The flujo de Volumen Total (J_{Vt}) represents the total sum of the individual contributions from the volume flow 1 (J_{V1}) and the volume flow 2 (J_{V2}), from the elements connected in parallel:

J_{Vt} = J_{V1} + J_{V2}

J_{Vt}
Flujo de Volumen Total
m^3/s
6611
J_{V1}
Volume flow 1
m^3/s
8478
J_{V2}
Volume flow 2
m^3/s
8479
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

ID:(12800, 0)



Darcy's law and hydraulic resistance (1)

Equation

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Darcy rewrites the Hagen Poiseuille equation so that the pressure difference (\Delta p) is equal to the hydraulic resistance (R_h) times the volume flow (J_V):

\Delta p_t = R_{st} J_{Vt}

\Delta p = R_h J_V

R_h
R_{st}
Total hydraulic resistance in series
kg/m^4s
5428
\Delta p
\Delta p_t
Total pressure difference
Pa
9842
J_V
J_{Vt}
Flujo de Volumen Total
m^3/s
6611
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

The volume flow (J_V) can be calculated from the hydraulic conductance (G_h) and the pressure difference (\Delta p) using the following equation:

J_V = G_h \Delta p



Furthermore, using the relationship for the hydraulic resistance (R_h):

R_h = \displaystyle\frac{1}{ G_h }



results in:

\Delta p = R_h J_V

ID:(3179, 1)



Darcy's law and hydraulic resistance (2)

Equation

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Darcy rewrites the Hagen Poiseuille equation so that the pressure difference (\Delta p) is equal to the hydraulic resistance (R_h) times the volume flow (J_V):

\Delta p_1 = R_{pt} J_{Vt}

\Delta p = R_h J_V

R_h
R_{pt}
Total hydraulic resistance in parallel
kg/m^4s
5429
\Delta p
\Delta p_1
Pressure Difference 1
Pa
9841
J_V
J_{Vt}
Flujo de Volumen Total
m^3/s
6611
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

The volume flow (J_V) can be calculated from the hydraulic conductance (G_h) and the pressure difference (\Delta p) using the following equation:

J_V = G_h \Delta p



Furthermore, using the relationship for the hydraulic resistance (R_h):

R_h = \displaystyle\frac{1}{ G_h }



results in:

\Delta p = R_h J_V

ID:(3179, 2)



Darcy's law and hydraulic resistance (3)

Equation

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Darcy rewrites the Hagen Poiseuille equation so that the pressure difference (\Delta p) is equal to the hydraulic resistance (R_h) times the volume flow (J_V):

\Delta p_3 = R_{h3} J_{Vt}

\Delta p = R_h J_V

R_h
R_{h3}
Hydraulic Resistance 3
kg/m^4s
5427
\Delta p
\Delta p_3
Pressure Difference 3
Pa
5447
J_V
J_{Vt}
Flujo de Volumen Total
m^3/s
6611
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

The volume flow (J_V) can be calculated from the hydraulic conductance (G_h) and the pressure difference (\Delta p) using the following equation:

J_V = G_h \Delta p



Furthermore, using the relationship for the hydraulic resistance (R_h):

R_h = \displaystyle\frac{1}{ G_h }



results in:

\Delta p = R_h J_V

ID:(3179, 3)



Darcy's law and hydraulic resistance (4)

Equation

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Darcy rewrites the Hagen Poiseuille equation so that the pressure difference (\Delta p) is equal to the hydraulic resistance (R_h) times the volume flow (J_V):

\Delta p_1 = R_{h1} J_{V1}

\Delta p = R_h J_V

R_h
R_{h1}
Hydraulic Resistance 1
kg/m^4s
5425
\Delta p
\Delta p_1
Pressure Difference 1
Pa
9841
J_V
J_{V1}
Volume flow 1
m^3/s
8478
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

The volume flow (J_V) can be calculated from the hydraulic conductance (G_h) and the pressure difference (\Delta p) using the following equation:

J_V = G_h \Delta p



Furthermore, using the relationship for the hydraulic resistance (R_h):

R_h = \displaystyle\frac{1}{ G_h }



results in:

\Delta p = R_h J_V

ID:(3179, 4)



Darcy's law and hydraulic resistance (5)

Equation

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Darcy rewrites the Hagen Poiseuille equation so that the pressure difference (\Delta p) is equal to the hydraulic resistance (R_h) times the volume flow (J_V):

\Delta p_1 = R_{h2} J_{V2}

\Delta p = R_h J_V

R_h
R_{h2}
Hydraulic Resistance 2
kg/m^4s
5426
\Delta p
\Delta p_1
Pressure Difference 1
Pa
9841
J_V
J_{V2}
Volume flow 2
m^3/s
8479
Dp_t = R_st * J_Vt Dp_1 = R_pt * J_Vt Dp_3 = R_h3 * J_Vt Dp_1 = R_h1 * J_V1 Dp_1 = R_h2 * J_V2 R_st = R_pt + R_h3 1/ R_pt =1/ R_h1 +1/ R_h2 Dp_t = Dp_1 + Dp_3 J_Vt = J_V1 + J_V2 J_VtR_h1R_h2R_h3Dp_1Dp_3R_ptR_stDp_tJ_V1J_V2

The volume flow (J_V) can be calculated from the hydraulic conductance (G_h) and the pressure difference (\Delta p) using the following equation:

J_V = G_h \Delta p



Furthermore, using the relationship for the hydraulic resistance (R_h):

R_h = \displaystyle\frac{1}{ G_h }



results in:

\Delta p = R_h J_V

ID:(3179, 5)