The invention relates to a linear drive unit
A corresponding drive unit is deduced from JP 2002-031054 A.
Corresponding drive units are used in particular to set pump plungers of compressors in linear oscillating motion. The system comprising such a compressor and a linear drive unit is therefore also designated as a linear compressor (see the JP-A specification mentioned initially).
In corresponding known linear compressors, the armature part provided with leaf springs which are generally circular-disk-shaped (see the JP-A specification mentioned initially) forms a spring-mass system with a certain characteristic oscillation frequency. If the linear compressor is to oscillate at 50 Hz (i.e. at the mains frequency), according to the conventional prior art, the spring constant of the two leaf springs would be designed in conjunction with the armature mass such that the characteristic frequency of the spring-mass system is 50 Hz. Furthermore, the rest position of the springs corresponds to the centre position of the desired armature oscillation. During operation a linear compressor thus designed delivers only a limited efficiency and displays a relatively slow start-up behaviour.
It is thus the object of the present invention to improve the linear drive provided with the aforementioned features such that it has a comparatively higher efficiency compared with the prior art and allows easier and more rapid start-up.
In order to achieve this object, the linear drive unit comprises the features specified in claim 1. Accordingly, in the centre position of the armature part, the point of application of the spring on the armature part is displaced axially by a predetermined distance in relation to its clamping position. The centre position of the armature part is understood in this case to be the position of the armature part which this adopts during its oscillation phase between its two maximum lateral deflections.
When the armature part is located in its rest position, this is then displaced towards one side compared with the centre position as a result of the given pre-stressing of the spring.
The advantages associated with this embodiment of the drive unit are seen in particular in the lower electrical losses, a higher efficiency, and the fact that the armature movement is easier to control and regulate. In addition, the start-up properties of the drive unit are thus improved.
Advantageous embodiments of the drive unit according to the invention are deduced from the dependent claims. At the same time, the embodiment according to claim 1 can be combined with the features of one of the dependent claims or preferably with those of a plurality of dependent claims. Accordingly, the following features can additionally be provided for the drive unit:
Further advantageous embodiments of the drive unit according to the invention are obtained from the claims not discussed previously and the drawings.
The invention is explained in detail hereinafter with reference to the drawings. In the figures:
Springs known per se, which act in the direction of oscillation/movement of its armature part can be used for the rive unit according to the invention. It appears particularly suitable to use at least one spring, preferably two leaf springs. These leaf springs are selected for the following exemplary embodiment. They make it possible to nevertheless achieve sufficiently good lateral stabilisation or retaining of the oscillating armature part perpendicular to its direction of movement with a low stiffness or spring constant k in the direction of oscillation/movement perpendicular to the plane of the spring. Naturally, other types of springs such as helical or coil springs can also be used. Bearings can also be provided in a known manner for lateral guidance.
As is further indicated in the figure, the two leaf springs 2 and 2′ which act on extended parts of the armature 15 at points of application A or A′ on both sides of the centre position Mp should be fixed such that they exert a force in the x-direction in the centre position of the armature 15 shown. Here x0 and −x0 designate the (initial) positions of the points of application A and A′ of the springs 2 and 2′ under the formation of pre-stressing which are obtained in a symmetrical arrangement of the armature part 15 with its two magnet parts 9a and 9b with respect to the centre position Mp. The spring constant k of the at least one spring is advantageously dimensioned such that the characteristic frequency f0=
of the drive unit in cooperation with the entire oscillating mass m is lower than the frequency of the driving magnetic force to be produced by the exciter winding. The value of k can be determined by means of computational methods.
In the drive unit according to the invention, the rest position of the armature in which the spring forces are removed, is displaced by a predetermined distance Δx towards one side. The associated pre-tensioning force should act laterally in the x-direction where a compressor V or its pump plunger is located. For this purpose, at least on one side the armature 15 goes over axially into a lateral extension part 16, not embodied in detail, which is rigidly connected to the pump plunger of the compressor V. Corresponding compressors of linear compressors connected to linear drive units and their individual parts belong to the prior art (see, e.g. said JP—2002-031054_A or U.S. Pat. No. 6,323,568 B1). Thus, these will not be described.
For the diagram in
Principles of Spring Design of a System Comprising Drive Unit and Compressor
For the following analyses, a linear drive unit 10 is assumed, its armature 15 being connected to a pump plunger of a compressor V. For simplicity it is assumed that
L1=L2=L.
The magnitude of the electromagnetic force acting on the armature
Fel
should either be zero or have a fixed value, the sign of the force always being selected so that the force acts in the direction of movement. The electrical force
Fel
is only non-zero for a fraction
a
of the distance (
0<a<1
;
a is hereinafter designated as “duty cycle”). Let
k
be the sum of the spring constants in the direction of movement and
x0
the rest position of the spring with respect to the centre position of the armature.
For
which corresponds to the return travel away from the compressor, the energy supplied electrically to the armature is given by
Table 1 Eq. 1
and from the armature dead-centre point
x=+L
to the armature dead-centre point
x=−L
the potential energy of the spring varies by
Table 2 Eq. 2
Both energies must be the same, i.e.
Table 3 Eq. 3
For
which corresponds to the forward travel towards the armature, the energy supplied electrically to the armature (in turn) is given by
Table 4 Eq. 4
and from the armature dead-centre point
x=−L
to the armature dead-centre point
x=+L
the potential energy of the spring varies by
The total electrical energy supplied within an oscillation for a constant oscillation amplitude
L
and negligible friction must be equal to the energy used in the compressor
Ecomp.
The electrical force (assumed to be constant) is thus obtained as
Table 5 Eq. 5
If the spring constant
k
and the electrical energy
Eel−
(i.e. the electrical force
Fel
the oscillation amplitude
L
and the duty cycle
a
) are given, the required spring rest position can be calculated by substituting Eq. 1 and Eq. 2 into Eq. 3:
Table 6 Eq. 6
From Eq. 6 it can be seen that:
The spring must always be pre-stressed in the positive direction and the pre-stressing distance is shorter, the higher the spring constant
k.
Method for Spring Design
The spring should be designed to that the armature oscillates symmetrically in the yoke with respect to
x=0
(i.e. between
x=−L
and
x=+L
), wherein the frequency
f
of the armature oscillation approximately corresponds to a target value
ftarget.
For a given armature mass, oscillation amplitude
L
and compressor characteristic, the oscillation frequency
f
is only dependent on two quantities: the spring constant
k
and the duty cycle
a
It holds that:
The spring can be designed as follows:
Example Calculations
The example calculations relate to a known compressor with a stroke of
2L=20
mm and standard pressure conditions (
pmax−pmin=(7.7−0.6)
bar). Since the dead volume is assumed to be vanishingly small, it produces no restoring force. The mechanical work performed per oscillation in the compressor under these conditions is 0.7753 J. If the mechanical power should be 40 W, an oscillation frequency of 51.6 Hz is required.
In the simulation block diagram according to
m
(mass) and
c
(coefficient of friction) have values of 90 g and 0.336 Ns/m.
In the following table the duty cycle
a
and the spring constant
k
should be considered to be initial quantities whereas the electrical force
Fel
, the spring rest position
x0
and the oscillation frequency
f
are the results of the calculation.
Number | Date | Country | Kind |
---|---|---|---|
10 2004 010 849.8 | Mar 2004 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/EP05/51007 | 3/7/2005 | WO | 5/21/2007 |