in the following , the various exemplary embodiments of the invention are described . although the present invention is applicable in a broad variety of mechanical applications it will be described with the focus put on a micromechanical application . [ 0034 ] fig1 shows a schematic illustration of a first embodiment . a nearly frictionless device 1 comprises a first object 10 that here is a substrate 10 and a second object 20 that here is a spinning disk 20 . the substrate 10 has a first surface 11 and the spinning disk 20 has a second surface 21 , whereby the surfaces 11 , 21 facing each other . the substrate 10 is arranged on an oscillator 30 that here is a piezoelectric oscillator 30 . the spinning disk 20 is separated from the substrate 10 by a plurality of spacers 2 . here , the spacers 2 are cantilevers with a tip mounted to the substrate 10 . the spacers 2 ease the lift off of the spinning disk 20 . on top of the spinning disk is a spindle 50 arranged in order to apply a small force to the center of the spinning disk 20 . the spindle 50 is mounted on a spring 52 , that is deformed when the spinning disk 20 lifts off . the spinning disk 20 lifts off when the medium , e . g . air , between the spinning disk 20 and the substrate 10 oscillates in such a way that an air bearing 40 occurs that has a thickness and the pressure such that the spinning disk glides on it . the piezoelectric oscillator 30 oscillates the substrate 10 in a direction perpendicular to the first surface 11 . this is shown by an arrow and the dotted lines indicating the edges of the oscillating substrate 10 . the air in the gap , i . e . the air in - between the surfaces 11 , 21 of the substrate 10 and the spinning disk 20 is actuating as a hard spring , because the air cannot come out on the side of the gab . this works around resonant frequency and through the air there are nearly no linear effects . a relative movement between the substrate 10 and the spinning disk 20 can be achieved by several driving means or techniques . the movement , for example , can be generated by a capacitor , an electromagnet , an electrostatic element , or an airflow . the rotation of the spinning disk 20 can be initiated by any one of the aforementioned means or techniques . as a driving means is shown an airflow generator or fan 22 to create an airflow which drives the spinning disk 20 . [ 0038 ] fig2 shows a second embodiment , whereby the same reference numerals are used to denote the same or like parts . the device in fig2 comprises the substrate 10 on the piezoelectric oscillator 30 separated from the spinning disk 20 by cantilevers 2 . on top of the spinning disk 20 is a plate 60 arranged such that the spinning disk 20 is sandwiched between the substrate 10 and the plate 60 . both 10 , 60 are equipped with cantilevers 2 , 62 . an axis 54 is arranged at the center of the spinning disk 20 to hold the spinning disk 20 at its position . here , the plate 60 , equipped with the cantilevers 62 , is used to transform a stepwise rotation as a kind of “ linear ” motion into a continuous rotation . this represents a motor . [ 0039 ] fig3 a shows a third embodiment in cross - sectional view where the spinning disk 20 is positioned and fixed in a three dimensional nearly frictionless setup . the same reference numerals are used to denote the same or like parts . the substrate 10 has a recess 12 for the reception of the spinning disk 20 . here , the spinning disk 20 has an enlarged surface to achieve a better centering . also sliders mounted on or attached to the spinning disk 20 would improve the centering . for the sake of simplicity , such sliders are not shown in the figure . moreover , a capacitor structure 24 , short capacitor 24 is arranged on the substrate 10 and the spinning disk 20 . the spinning disk 20 is activated to rotate by the capacitor structure 24 or other suitable driving means . if the substrate 10 is activated by oscillation through the piezoelectric oscillator 30 and the air bearing 40 is generated , the spinning disk 20 is lifted off and centered by the air vibration . in the third dimension , i . e . in the z - direction , the disk might be trapped by another oscillating disk like shown in fig2 . resulting in a three dimensional air cushion . a nearly frictionless high speed motor can be provided . [ 0040 ] fig3 b shows a forth embodiment which is similar to the embodiment described with reference to fig3 a . the same reference numerals are used to denote the same or like parts . fig3 b shows a nearly frictionless bearing with a rotating hard disk 20 , whereby additional parts can be mounted on the hard disk 20 or the substrate 10 . during gliding on the air bearing 40 the hard disk 20 centers itself . [ 0041 ] fig4 and 5 show a fifth embodiment in cross - sectional and top view where the spinning disk 20 is surrounded by three guide elements 60 . the same reference numerals are used to denote the same or like parts , whereby the substrate 10 has no recess . each of the three guide elements 60 can be seen as a wall oscillating perpendicular to the direction of the oscillator 30 . such a wall can be made of piezoelectric material . the oscillation of the guide elements 60 into the direction of the center of the spinning disk 20 additionally supports the air bearing and thereby the gliding of the spinning disk 20 . the oscillations are indicated by the arrows and the dotted lines indicating the edges of the oscillating substrate 10 and guide elements 60 , respectively . the rotation of the spinning disk 20 is initiated by electromagnetic elements , which for the sake of clarity are not shown in the figure . [ 0042 ] fig6 shows a top view of a further embodiment comprising sliders 80 . the spinning disk 20 is arranged within a tube 70 , whereby this tube has three sliders 80 arranged at its inner side towards the circumference of the spinning disk 20 . the sliders 80 are formed such that the medium between the tube 70 and the spinning disk 20 is compressed in a defined way . the sliders 80 could be arranged as well as on the spinning disk 20 . it might be additional advantageous if the radius of the tube 70 varies by oscillation , as described with reference to fig4 and 5 . furthermore , the spinning disk 20 might have an imbalance or unbalance . [ 0043 ] fig7 shows a schematic illustration of a guided spinning disk 20 by guide elements 60 . here , three wheels 65 are arranged at the circumference of the spinning disk 20 . each wheel 65 is fixed at its center . the spinning disk is guided on its outside by the wheels 65 instead of the center . referring still to fig8 where a schematic illustration of an embodiment with several moving objects 20 is shown . the moving objects 20 are micro - robots 20 which can move individually in x - and y - directions , as indicated by the arrows , on the oscillating substrate 1 . the individual movement is achieved by the different resonant frequencies of each micro - robot 20 . an individual control of a lot of micro - robots 20 can be provided . as shown , the micro - robots 20 have different shapes . they can also have different weights or spacers 2 . the spacers 2 , e . g . cantilevers , can be on the side of the substrate 1 or on the side of each micro - robot 20 depending on the application . by using the air bearing 40 , a very precise distance control between the first object 10 and the second object 20 is provided . the working range in an experiment was around 2 - 4 micrometer in z - direction . the resonant frequency was around 8 khz , stable , and reproducible . a nearly frictionless movement in the z - direction and also in the x - and y - directions by activating a movement in these directions can be guaranteed . the motion of the moving object 20 in x - and y - directions can be linear as well as rotational by actuators or driving means 22 , 24 . this driving means 22 , 24 can be external or internal . internal means , the cantilevers by themselves can initiate the movement of the direction by special actuation . the distance of move can be defined by a periodic stimulation of a single pulse . moreover , the movement in the z - direction can be phase locked to the z actuation . that means , nearly frictionless movement in x - and y - direction is only possible if a defined distance between the first object 10 and the second object 20 is provided . the nearly frictionless movement in x - and y - direction can be achieved in x / y resonant or non resonant mode . any disclosed embodiment may be combined with one or several of the other embodiments shown and / or described . this is also possible for one or more features of the embodiments .