(1) Field of the Invention
The present invention relates to a device for measuring a mass flow with a guide means having a surface shaped as a circular arc, over which the mass flow can flow during the measurement, and a force sensor.
(2) Description of Related Art
The German published application DE 18 02 213 discloses a device of this type. The guide means of the device is pivotally supported and has an extension arm which operates on the force sensor when the guide means performs a pivoting motion. During the flow across the guide means, a mass flow flowing across the guide means experiences a centripetal force that is proportional to the moving mass. A force in the opposite direction counteracts the centripetal force applied by the guide means on the moving mass, which in conjunction with the friction forces generated by the mass particles produces a pivoting motion of the guide means about its pivot point. The torque of this pivoting motion is transferred to the force sensor by the extension arm of the guide means. The force sensor generates from the torque a sensor signal which corresponds to the force exerted by the force transfer point on the extension arm on the pivot point where the force sensor is located.
The location of the pivot point of the guide means can be defined in a manner described in the published application, which discloses that effects, which are produced by the friction of the mass particles during their flow along the guide means, are substantially compensated with the predefined location of the pivot point of the guide means. However, the method disclosed in the printed application for determining the pivot point is only qualitative. A quantitative method for determining the pivot point that is mathematically or mechanically founded is not disclosed. Compared to the conventional methods for determining mass flow, the device disclosed in the published application is superior, but does not satisfy the requirements for an exact measurement of the mass flow, where all effects caused by friction need to be compensated.
It is therefore an object of the invention to design a device of the aforedescribed type so that the mass flow can be measured with greater accuracy than before. In particular, effects caused by friction between the mass particles and the guide plate are compensated.
This object is attained by the invention in that guide means are pivotally supported via the force sensor, and that the support occurs on a straight line which extends through an endpoint of a radius vector of a resulting friction force operating on the mass flow and in the same direction as the resulting friction force operating on the mass flow. The point where the guide means are supported is therefore determined depending on the friction force. The friction force can then be compensated so that the force measurement of the centripetal force is unaffected by the friction force, and the mass flow can then be determined from the friction force. Material-dependent quantities, such as the friction coefficient, are taken into consideration when computing the friction force.
The resulting friction force represents the entirety of the friction forces generated when the mass particles flow along the surface shaped as a circular arc. These partials forces are added and yield the resulting friction force.
If the support point is located on the line of the effective force and if the direction in which the force sensor is able to measure forces is perpendicular to the resulting friction force, then the resulting friction force has no effect on the measurement by the force sensor. The resulting friction force is therefore irrelevant for this measurement.
The line on which the guide means are supported can be inclined by an angle η of
with respect to the horizontal, wherein the radius vector TO is representative of the resulting friction force operating on the mass flow. For a friction coefficient of μ=0.1 of the flowing mass, the angle η can be about η=48.48°. For a friction coefficient of μ=0.2 of the flowing mass, the angle η can be η=48.70°. For a friction coefficient of μ=0.3, the angle η can be preferably η=48.88°. In a particular embodiment of the device, the radius vector TO of the resulting friction force F can be oriented horizontally. In this case, the resulting friction force F would be vertical which results in a corresponding support of the guide means.
Preferably, the support is located at the endpoint of the radius vector TO of the resulting friction force F operating on the mass flow.
The force measurement direction of the force sensor, i.e., the direction from which the force sensor can measure forces, is preferably along the direction of the radius vector TO of the resulting friction force F acting on the mass flow. Because of the radius vector TO is perpendicular to the resulting friction force F, the force measurement directions is also perpendicular to the resulting friction force F The resulting friction force F is therefore not a factor in the measurement of the force sensor.
The guide means can be supported on the force sensor, i.e., the guide means is preferably attached to a force-sensitive or to the force-receiving surface of the force sensor. Alternatively, the guide means can be rigidly connected with the force sensor and an assembly which includes the guide means and the force sensor can be supported on a holding means. The support then also occurs on the force-sensitive surface of the force sensor.
The guide means of the device of the invention can be a curved tube, a measurement chute, a slide, and the like.
The device may include a supply means which is suitable and configured to supply the mass flow to the guide means. Such supply means can include one or more elements for uniformly distributing the volume flow over a cross section through which the volume flow flows. The resulting tangential force can only be computed in a simplified manner by assuming a uniform distribution of the flow height of the volume flow in the depth of the guide means. An element for uniformly distributing the volume flow may include, for example, an inclined plane across which the volume flow is guided. Alternatively, the element for uniformly distributing the volume flow may also include a nozzle.
In a particular embodiment, the device of the invention may include shut-off means for shutting off the mass flow. The shut-off means may be configured so that the magnitude of the mass flow can be adjusted. The shut-off means can be arranged in the flow directions either before or after the guide means.
The basic features of the invention will be described first with reference to the drawings, followed by a more detailed description of exemplary embodiments of the devices of the invention.
a shows the forces operating on a mass particle,
b shows the forces acting on a guide means,
A tangent t is indicated at a point P of the path of the mass particle. The normal on the tangent t is indicated with n.
The forces indicated in
According to the concept of the invention, the measurement chute 4 is supported so that the force measurement direction of the force sensor is oriented in the direction of the resulting centripetal force and perpendicular to the direction of the resulting friction force of all particles of the mass flow. In order to properly align the force sensor and to support the measurement chute, for example, in the corresponding direction on the force sensor, the direction of the resulting friction force of all mass particles of the mass flow needs to be calculated. The radius vector of the resulting friction force can be determined using mechanical and mathematical principles. From this radius vector, the following quantity is computed:
The tangential force can be computed by numerical integration. The moment T0 also follows from the following equation through integration:
Because the radius vector of the resulting friction force can be computed, the direction of the friction force can also be determined from the radius vector due to the established orthogonality of the radius vector to the friction force . It follows that the direction of the friction force is inclined with respect to a horizontal by the following angle:
The angle of inclination η can be determined by numerical computations.
The mass flow is indicated in
Conversely, in the exemplary embodiment illustrated in
Number | Date | Country | Kind |
---|---|---|---|
10 2008 011 564 | Feb 2008 | DE | national |
Number | Name | Date | Kind |
---|---|---|---|
1883017 | Sholtz | Oct 1932 | A |
5002140 | Neumüller | Mar 1991 | A |
6471032 | Busschaert et al. | Oct 2002 | B2 |
6616527 | Shinners et al. | Sep 2003 | B2 |
Number | Date | Country |
---|---|---|
0753720 | Jan 1997 | EP |
0851216 | Jul 1998 | EP |
0877234 | Nov 1998 | EP |
Number | Date | Country | |
---|---|---|---|
20100011881 A1 | Jan 2010 | US |