Short communicationFollowing the motion of a charged conducting sphere by electrostatic induction in a parallel plate capacitor
Introduction
There are several non intruding methods to trace the motion of a small object. E.g. various schemes of optical detection are widely used. However, if the experiment is confined to a non transparent housing other techniques are required. This may be achieved by monitoring induced charges if the object to be studied carries an electrostatic charge. The current generated by a transient image charge has been described for a particle moving in the vicinity of an electrode [1,2]. Different arrangements of electrodes are conceivable, e.g. tubes [3,4], parallel plate capacitors or a coaxial set of three electrodes [5]. Amongst others experiments were performed e.g. for projectiles with high speed [[6], [7], [8]].
Recently, we have shown that using electrostatic detection it is possible to follow the motion of a weakly charged object in all three dimensions with an excellent temporal resolution which exceeds the one of conventional high speed cameras [9]. The detection relies on the charge induced in an electrode which can be measured by a charge sensitive amplifier. In many cases a satisfactory agreement between the real trajectory and the one deduced from the measured charge is obtained assuming a point charge instead of an extended charge distribution. In the present paper we will consider in detail, how the induced charges vary with distance when a conducting sphere comes close to the surface of the electrode. As will be shown an almost accurate description can be given for distances down to less than a hundredth of the radius of the sphere.
Section snippets
Principle of the experiment
Fig. 1 displays the basic scheme of the experiment. The detection of the motion and of the charge of the sphere are based on electrostatic induction. The sphere is falling through a small hole (not shown in the sketch) into a parallel plate capacitor. The lower plate is grounded by connecting it to a very sensitive charge amplifier. The charge of the sphere induces image charges on the upper and lower plate of the capacitor, both of opposite sign. If one assumes a point charge instead of the
Method
For the presented study it is important to know the trajectory and the charge of the sphere. To obtain a well defined motion in the vertical direction, the free fall of a sphere is studied.where g is the gravitional acceleration, and are the initial conditions for the velocity and the height at . If the sphere bounces from a horizontal plate, and may be easily determined for each section. If and are the successive times when the sphere touches the
Results
The lower part of Fig. 3 displays the measured charge on the lower plate of the capacitor while a stainless steel sphere is bouncing on the lower plate. The full dataset including simulations using formulas (1) and (4) is available in Ref. [14]. The moments of mechanical contact, indicated by the vertical dashed lines, are clearly visible. The data are slightly complicated because the charge of the sphere changes at each contact to the plate. Due to the conservation of charge, the charge
Summary
The induced charges in a parallel plate capacitor may be used to accurately determine the position of a charged sphere in the direction normal to the plates. However, when the sphere approaches one of the plates the motion of the charge on the surface of the sphere has to be considered. Based on known formulas for the mutual capacitance between a sphere and a plate a formula is given which provides an accurate description of the induced charge. The comparison to the data measured for a charged
Declaration of competing interest
The authors declare that there is no conflict of interest.
Acknowledgement
The work was funded by the Elstatik Foundation, Germany (Project No.: 440701010750005).
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