Engee documentation

Ball Poppet with Conical Seat (IL)

Page in progress.

Spherical valve with conical seat with sharp edges.

ball poppet with conical seat il

Description

Block Ball Poppet with Conical Seat (IL) represents the one-dimensional movement of a spherical valve with a conical seat.

The resultant force acting on the valve is due to the pressure force and external forces. The pressure at port B is assumed to act on the active region adjacent to the orifice and tends to open the orifice. The pressure at port A acts on the remaining area of the ball. These assumptions give the pressure force acting on the balloon. This force can be corrected using the hydrodynamic force.

The displacement and velocity of the piston are input to port R_s. There are no limits on the displacement value in the block, but limits can be provided by the attached block using end stops.

Lift is the variable associated with this displacement. Naturally, the limits of this lift are associated with the limit for the displacement values. If the ball lift is more than 20% of the ball diameter, accuracy will be reduced.

The bore area should never exceed the throat bore area defined by the seat diameter and stem diameter (seat side). However, it is sometimes useful to limit the orifice area to a minimum and/or maximum value. The minimum area can be used to model a leak or a special flow-through orifice, even when the ball is fully seated. The maximum area can be used to model the flow area adjacent to the orifice when the valve is wide open.

Note that the flow rate is calculated taking into account the ball movement.

Equations

The balloon lift is calculated as:

where

  • - rise corresponding to the zero offset, the value of parameters Lift corresponding to zero displacement;

  • - is the piston displacement that is input to port R_s.

The equations that the block uses depend on the model Flow force model:

  • Simple - simple hydrodynamic force model;

  • Corrected by effective pressure area factor - hydrodynamic force model with correction for the effective pressure area coefficient, for details see [1-2];

  • Advanced active area - hydrodynamic force model with a modification of the calculation of the active area upstream, for details see [3].

Equations for a simple model

ball poppet with conical seat 1

The minimum flow area is defined by the curved surface of a truncated cone, as shown in the figure. It is assumed that this surface divides the area occupied by the fluid into two areas with different pressures. One of these regions is subject to the pressure , and the other is subject to the pressure . This assumption is reasonable if the ball lift is small compared to the diameter of the saddle. If the ball lift is large, it is obvious that at some point the smallest constraint will be the throat area.

The condition must be satisfied:

If this condition is violated, the ball will not be able to rest on the conical seat.

The area of the hole is defined as:

where

  • , where is half the angle of solution of the conical seat;

  • - ball diameter.

The hydraulic diameter is calculated as:

Active diameter is calculated as:

Note that the value used for , is limited between and the smaller of and , where is the lift value at which the calculated area becomes equal to the neck area:

The value of is always greater than .

The value of is normally zero, but can be set higher to model the leakage flow rate. The value of is usually very large (e.g. Inf), but can be set much lower to model an additional orifice.

The volume of fluid , the pressure at which is equal to the pressure , additional to the volume when the valve is closed, is calculated as:

The value of the additional volume is important when calculating the pressure dynamics (frequency analysis).

The derivative of the additional volume by is calculated as:

The volume of fluid that is discharged to port B is calculated as:

where is the value of the parameters Volume at port B corresponding to zero lift.

The volume of liquid that is output to port A is calculated as:

where is the value of the parameters Volume at port A corresponding to zero lift.

Flow coefficient is calculated as

where

  • - is the pressure drop between the ports;

  • - hydraulic diameter;

  • - kinematic viscosity;

  • - average density of the fluid.

The average density is calculated at the average pressure .

The flow coefficient is calculated as

where

  • - maximum flow coefficient, the value of parameters Maximum flow coefficient;

  • - critical flow coefficient, parameter value Critical flow number.

For , the value of does not change much. For low the value of varies linearly with the change of .

A reasonable value of by default is 1000. However, for holes with complex (rough) geometry it may be less than 50. For very smooth geometry it can be set to 50000.

The average fluid velocity is:

The volume flow rate is:

where

  • - is the area of the through hole;

  • - is the density of the liquid at atmospheric pressure.

Volume flow rates at ports B and A are calculated as:



where

  • - is the density of the liquid at port pressure B, ;

  • - density of liquid at port pressure A, ;

  • - stem velocity at port R_s.

The hydrodynamic force is determined by evaluating the change in momentum. This force tends to close the valve. For steady-state fluid flow, the hydrodynamic force is equal to:

where is the angle of inclination of the jet:

The dependence of the hydrodynamic force on the lift is defined as follows:

where is the value of parameters Lift corresponding to minimum area.

The force at port R_s is calculated as:

where is the force that enters the R_p port.

Equations for the model with correction for the effective pressure area factor

The model Corrected by effective pressure area factor differs from Simple in that the value of active diameter and hydrodynamic force is calculated taking into account the type of flow (laminar or turbulent).

In this section, the equations for calculating the corrected parameters are given, the other parameters are calculated in the same way as for the model Simple.

The active diameter is defined as:

Active area is defined as:

The actual active area depends on the type of flow (laminar or turbulent):

  • If the flow is laminar:

  • If the current is turbulent:

In these formulas is the value of the parameters Turbulent effective pressure area factor.

The hydrodynamic force also varies with the fluid velocity at the inlet and outlet of the orifice:

where

  • - is the fluid velocity at the inlet to the orifice:

  • - liquid velocity at the outlet of the orifice:

The force at the port R_s is calculated as:

where is the force that enters the R_p port.

Equations with modification of calculation of active areas upstream

The model Advanced active area differs from Simple in that the upstream active areas (minimum and maximum) are calculated.

In this section, the equations to calculate the adjusted parameters are given, the rest of the parameters are calculated in the same way as for the model. Simple.

ball poppet with conical seat 2 en

The maximum active area upstream is calculated as:

The minimum active area upstream is calculated as follows:

ball poppet with conical seat il 3

The active area upstream is calculated as:

It should be noted that the calculation performed is only valid for the incoming jet and not valid for the outgoing jet. Consequently, the upstream jet must be on the saddle side. Then the force at the port R_s is calculated as:

where is the active diameter calculated from the upstream active area value .

Ports

Conserving

# A — isothermal liquid port
isothermal liquid

Details

Port of isothermal liquid, corresponds to inlet or outlet.

Program usage name

port_a

# B — isothermal liquid port
isothermal liquid

Details

Port of isothermal liquid, corresponds to inlet or outlet.

Program usage name

port_b

# R_p — stem
translational mechanics

Details

A mechanical progressive port corresponding to the rod on the side opposite the seat side.

Program usage name

rod_flange_b

# R_s — stem
translational mechanics

Details

A mechanical progressive port corresponding to the stem on the seat side.

Program usage name

rod_flange_a

Parameters

Parameters

# Flow force model — hydrodynamic force model
Simple | Corrected by effective pressure area factor | Advanced active area

Details

Hydrodynamic force model:

  • Simple - A simple hydrodynamic force model;

  • Corrected by effective pressure area factor - hydrodynamic force model with correction for the effective pressure area coefficient;

  • Advanced active area - hydrodynamic force model with modification of calculation of active area upstream.

Values

Simple | Corrected by effective pressure area factor | Advanced active area

Default value

Simple

Program usage name

flow_force_model

Evaluatable

No

# Seat diameter (hole) — conical seat diameter at the base
m | cm | ft | in | km | mi | mm | um | yd

Details

Seat diameter, .

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

5.0 mm

Program usage name

seat_diameter

Evaluatable

Yes

# Seat semi-angle (between 0 and 90) — half of the angle of the conical seat solution
deg | rad | rev | mrad

Details

Half angle of conical seat solution, .

Units

deg | rad | rev | mrad

Default value

45.0 deg

Program usage name

conical_seat_semi_angle

Evaluatable

Yes

# Ball diameter — ball diameter
m | cm | ft | in | km | mi | mm | um | yd

Details

Ball Diameter, .

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

10.0 mm

Program usage name

ball_diameter

Evaluatable

Yes

# Rod diameter (opposite to seat) — stem diameter on the opposite side to the seat side
m | cm | ft | in | km | mi | mm | um | yd

Details

Stem diameter on the opposite side of the seat, .

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

0.0 mm

Program usage name

rod_diameter_at_seat_opposite_side

Evaluatable

Yes

# Rod diameter (seat side) — stem diameter at seat side
m | cm | ft | in | km | mi | mm | um | yd

Details

Seat side stem diameter, .

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

0.0 mm

Program usage name

rod_diameter_at_seat_side

Evaluatable

Yes

# Turbulent effective pressure area factor — effective pressure area factor

Details

Effective pressure area factor, .

Dependencies

To use this parameter, set parameter Flow force model value Corrected by effective pressure area factor.

Default value

1.0

Program usage name

effective_pressure_area_factor

Evaluatable

Yes

# Lift corresponding to zero displacement — lift corresponding to zero offset
m | cm | ft | in | km | mi | mm | um | yd

Details

Lift corresponding to zero offset.

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

0.0 mm

Program usage name

lift_offset

Evaluatable

Yes

# Lift corresponding to minimum area — rise corresponding to the minimum area
m | cm | ft | in | km | mi | mm | um | yd

Details

Lift , corresponding to the minimum area of the passage opening.

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

0.0 mm

Program usage name

orifice_opening_at_min_area

Evaluatable

Yes

# Lift corresponding to maximum area — rise corresponding to the maximum area
m | cm | ft | in | km | mi | mm | um | yd

Details

Lift , corresponding to the maximum area of the passage opening.

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

Inf mm

Program usage name

orifice_opening_at_max_area

Evaluatable

Yes

# Volume at port A corresponding to zero lift — volume in port A corresponding to zero lift
l | gal | igal | m^3 | cm^3 | ft^3 | in^3 | km^3 | mi^3 | mm^3 | um^3 | yd^3 | N*m/Pa | N*m/bar | lbf*ft/psi | ft*lbf/psi

Details

Volume at port A corresponding to zero lift.

Units

l | gal | igal | m^3 | cm^3 | ft^3 | in^3 | km^3 | mi^3 | mm^3 | um^3 | yd^3 | N*m/Pa | N*m/bar | lbf*ft/psi | ft*lbf/psi

Default value

0.0 cm^3

Program usage name

V_a_lift_offset

Evaluatable

Yes

# Volume at port B corresponding to zero lift — port volume B corresponding to zero lift
l | gal | igal | m^3 | cm^3 | ft^3 | in^3 | km^3 | mi^3 | mm^3 | um^3 | yd^3 | N*m/Pa | N*m/bar | lbf*ft/psi | ft*lbf/psi

Details

Volume at port B corresponding to zero lift.

Units

l | gal | igal | m^3 | cm^3 | ft^3 | in^3 | km^3 | mi^3 | mm^3 | um^3 | yd^3 | N*m/Pa | N*m/bar | lbf*ft/psi | ft*lbf/psi

Default value

0.0 cm^3

Program usage name

V_b_lift_offset

Evaluatable

Yes

Jet Force Evaluation

# Jet force coefficient — hydrodynamic force coefficient

Details

A hydrodynamic force coefficient which, at a value of 0 (by default) turns off the hydrodynamic force and at a value of 1 turns it on. If experimental data for this coefficient is available, you can adjust the model to this data.

Default value

0.0

Program usage name

jet_force_coefficient

Evaluatable

Yes

Flow Coefficient Law

# Maximum flow coefficient — maximum flow rate

Details

The maximum flow coefficient affects the flow/pressure drop characteristics of the orifice. This value can be left by default for most applications.

Default value

0.7

Program usage name

C_q_max

Evaluatable

Yes

# Critical flow number — critical flow coefficient

Details

The critical flow coefficient affects the flow/pressure drop characteristics of the orifice. This value can be left by default for most applications.

Default value

100.0

Program usage name

critical_flow_number

Evaluatable

Yes

Initial Conditions

# Initial rod displacement — initial stem displacement
m | cm | ft | in | km | mi | mm | um | yd

Details

Initial stem displacement.

Units

m | cm | ft | in | km | mi | mm | um | yd

Default value

0.0 mm

Program usage name

rod_displacement_start

Evaluatable

Yes

Literature

  1. N.Mittwollen, T.Michl, R.Breit "Parametric hydraulic valve model including transitional flow effects", 2nd MATHMOD Vienna 1997 (IMACS).

  2. N.Mittwollen, "Hydraulic simulation of cavitation induced pressure fluctuations with peculiar periodicities in a fluid power unit", 8th Bath international fluid power workshop, September 1995.

  3. A. Clavier, M. Alirand, F. Vernat, B. Sagot, "Local approach to improve the global approach of hydraulic forces in ball poppet valves", 4th Int. Symposium on Fluid Power, Wuhan, China, April 2003.