LIBRARY

Fittings.FlowDivider

Splits an incoming mass flow from port_a such that the flow to port_b is reduced by a factor n, with the remainder exiting via an open port.

This component models a flow splitting device where an incoming mass flow rate, $dot{m}_a$ (represented by m_flow_a and sourced from port_a.m_flow), is divided. A fraction of this flow is directed to port_b, resulting in an outgoing mass flow rate, $dot{m}_b$ (represented by m_flow_b and connected to port_b.m_flow). The governing equations are:

$$\begin{gathered} dot{m}_b= \\ frac \\ dot{m}_{a}n \\ dot{m}_{open}= \\ dot{m}_a- \\ dot{m}_b \end{gathered}$$

where n is the division factor parameter and $dot{m}_{open}$ is the mass flow rate expelled through the open port. This ensures mass conservation. The component is useful for modeling parallel tubes efficiently by placing a FlowDivider on each end of a tube, with the extra flow being dumped into the open port.

Usage

HydraulicComponents.Fittings.FlowDivider(n)

Parameters:

Name	Description	Units	Default value
n	Divide flow from port_a to port_b by n	–

Connectors

• port_a - (Port)

• port_b - (Port)

• open - (Port)

Variables

Name	Description	Units
m_flow_a	Mass flow of port_a	kg/s
m_flow_b	Mass flow of port_b	kg/s

Behavior

Behavior of this component cannot be rendered because it includes path variables.

Source

"""
Splits an incoming mass flow from `port_a` such that the flow to `port_b` is reduced by a factor `n`, with the remainder exiting via an `open` port.

This component models a flow splitting device where an incoming mass flow rate,
$\\dot{m}_{a}$ (represented by `m_flow_a` and sourced from `port_a.m_flow`), is divided.
A fraction of this flow is directed to `port_b`, resulting in an outgoing mass flow rate,
$\\dot{m}_{b}$ (represented by `m_flow_b` and connected to `port_b.m_flow`).
The governing equations are:

math \dot{m}{b} = \frac{\dot{m}{a}}{n}
\dot{m}{open} = \dot{m} - \dot{m}_

where `n` is the division factor parameter and $\\dot{m}_{open}$ is the mass flow
rate expelled through the `open` port. This ensures mass conservation.
The component is useful for modeling parallel tubes efficiently by placing
a `FlowDivider` on each end of a tube, with the extra flow being dumped
into the `open` port.
"""
component FlowDivider
  "Input port for the flow to be divided"
  port_a = HydraulicComponents.Interfaces.Port() {
    "Dyad": {
      "placement": {
        "diagram": {"x1": -20, "x2": 20, "y1": 480, "y2": 520, "sh": 1, "sw": 1, "rot": 0}
      }
    }
  }
  "Output port for the main divided flow"
  port_b = HydraulicComponents.Interfaces.Port() {
    "Dyad": {
      "placement": {
        "diagram": {"x1": 980, "x2": 1020, "y1": 480, "y2": 520, "sh": 1, "sw": 1, "rot": 0}
      }
    }
  }
  "Output port for the remaining (excess) flow"
  open = HydraulicComponents.Interfaces.Port() {
    "Dyad": {
      "placement": {
        "diagram": {"x1": 480, "x2": 520, "y1": 980, "y2": 1020, "sh": 1, "sw": 1, "rot": 0}
      }
    }
  }
  "Divide flow from `port_a` to `port_b` by `n`"
  parameter n::Real
  "Mass flow of `port_a`"
  variable m_flow_a::MassFlowRate
  "Mass flow of `port_b`"
  variable m_flow_b::MassFlowRate
relations
  continuity(port_a.medium, port_b.medium, open.medium)
  m_flow_a = port_a.m_flow
  m_flow_b = port_b.m_flow
  m_flow_b = m_flow_a / n
  open.m_flow = m_flow_a - m_flow_b
metadata {
  "Dyad": {
    "icons": {"default": "dyad://HydraulicComponents/FlowDivider.svg"},
    "labels": [{"label": "$(instance)", "x": 500, "y": 1100, "rot": 0}]
  }
}
end

Flattened Source

"""
Splits an incoming mass flow from `port_a` such that the flow to `port_b` is reduced by a factor `n`, with the remainder exiting via an `open` port.

This component models a flow splitting device where an incoming mass flow rate,
$\\dot{m}_{a}$ (represented by `m_flow_a` and sourced from `port_a.m_flow`), is divided.
A fraction of this flow is directed to `port_b`, resulting in an outgoing mass flow rate,
$\\dot{m}_{b}$ (represented by `m_flow_b` and connected to `port_b.m_flow`).
The governing equations are:

math \dot{m}{b} = \frac{\dot{m}{a}}{n}
\dot{m}{open} = \dot{m} - \dot{m}_

where `n` is the division factor parameter and $\\dot{m}_{open}$ is the mass flow
rate expelled through the `open` port. This ensures mass conservation.
The component is useful for modeling parallel tubes efficiently by placing
a `FlowDivider` on each end of a tube, with the extra flow being dumped
into the `open` port.
"""
component FlowDivider
  "Input port for the flow to be divided"
  port_a = HydraulicComponents.Interfaces.Port() {
    "Dyad": {
      "placement": {
        "diagram": {"x1": -20, "x2": 20, "y1": 480, "y2": 520, "sh": 1, "sw": 1, "rot": 0}
      }
    }
  }
  "Output port for the main divided flow"
  port_b = HydraulicComponents.Interfaces.Port() {
    "Dyad": {
      "placement": {
        "diagram": {"x1": 980, "x2": 1020, "y1": 480, "y2": 520, "sh": 1, "sw": 1, "rot": 0}
      }
    }
  }
  "Output port for the remaining (excess) flow"
  open = HydraulicComponents.Interfaces.Port() {
    "Dyad": {
      "placement": {
        "diagram": {"x1": 480, "x2": 520, "y1": 980, "y2": 1020, "sh": 1, "sw": 1, "rot": 0}
      }
    }
  }
  "Divide flow from `port_a` to `port_b` by `n`"
  parameter n::Real
  "Mass flow of `port_a`"
  variable m_flow_a::MassFlowRate
  "Mass flow of `port_b`"
  variable m_flow_b::MassFlowRate
relations
  continuity(port_a.medium, port_b.medium, open.medium)
  m_flow_a = port_a.m_flow
  m_flow_b = port_b.m_flow
  m_flow_b = m_flow_a / n
  open.m_flow = m_flow_a - m_flow_b
metadata {
  "Dyad": {
    "icons": {"default": "dyad://HydraulicComponents/FlowDivider.svg"},
    "labels": [{"label": "$(instance)", "x": 500, "y": 1100, "rot": 0}]
  }
}
end

Test Cases

No test cases defined.

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