APPARATUS FOR CAPACITIVE ELECTRICAL DETECTION

Abstract: Apparatus for capacitive electrical detection or measurement relating to a medium, comprising at least one electrode (10) having a given surface extension (10A, 10B) and an oscillator circuit (15) the output frequency of which is a function of the capacitance being associated with the electrode and the dielectric constant of the medium, and is taken as a basis for the detection or measurement. The effective spacing of the electrode (10) from a counter electrode or frome earth is of the same or a substantially higher order of magnitude as seen in relation to the surface extension (10A, 10B) of the electrode (10). A conductor (11) connecting the electrode (10) to the oscillator circuit (15) has a length that is a small fraction as seen in relation to the surface extension (10A, 10B) of the electrode.

Description: APPARATUS FOR CAPACITIVE ELECTRICAL DETECTION The invention relates to an apparatus for capacitive electrical detection or measurement with respect to a medium, substance, material or object in a solid or fluid form. In many practical applications the media of interest comprise water, e.g. in the form of moisture in the substance or material concerned. The apparatus is of the type comprising at least one electrode having a given surface extent and an oscillator circuit the output frequency of which is a function of the capacitance being associated with the electrode and the dielectric constant of the medium, and taken as a basis for the detection or measurement. There is here the question of a measurement principle being well known per se, as will appear e.g. from the book "Instrumenteringsteknikk" by Odd Arild Olsen, Tapirs forlag, 1988, pages 141 and 245. Examples of specific applications are given in McGraw-Hill Encyclopedia of Science & Technology, 7ht addition, volume 10, page 35 and volume 14, page 278. There exist various earlier practical proposals and applications based on the known principle, where there is provided a capacitor in a relatively conventional sense, usually with plate-shaped electrodes between which there is received a dielectric in the form of the medium, substance or material concerned, that is subject to detection or measurement. In this connection there is reason to note that different media can have rather different dielectric constants, e.g. water having the value 80, oil the value 3 and air the value 1. The object of this invention is to provide a novel apparatus being based upon the above principle, but having substantially expanded fields of application as well as an increased accuracy and sensitivity, as it is required when measuring e.g. pollution or moisture and likewise in demand- ing level measurements. As regards detection or measurement of pollution there can e.g. be the question of oil in water or water in oil. Also when level measurement is concerned the two media water and oil are of much interest in this connection. As will appear from the following description there is φ. ω ) to to I- 1 H o LΠ o LΠ o LΠ o LΠ 3 H Φ rt ft ) to g; 0 μ- hf l- 1 Φ 3 φ ft ) ø rt CΩ O CO μ- tr LQ φ 0 PJ TJ M o CQ ft CQ tr μ- 0 ) tr ft H φ ft ) μ- 3 tr hi H Ω φ Ω tr hi CΩ Ω O o Ω 3 3 rt Φ CQ rt tr CO Φ 0 ø Ω tr rt 0 Ω ft ) LQ 0 Φ 0 0 ) Φ M hi CΩ ft ) O (t Φ tr φ ft ) 0 ft rt Φ μ- 3 TJ μ- Φ N hi φ ft ) P. ft 0 Hi hf 0 Φ hi _-> ω OJ to to μ> μ> o LΠ o LΠ o LΠ o LΠ hf Φ Ω hh 0 < hf 01 <! £ μ- ft Ω TJ 03 ft ) CQ it Hi Ω « 0 H Hi TJ It 0 ø ft ) hi 01 ft P. HI TJ Ω rt o ft ) 1 0 ) 0 TJ ft ) ft ) φ ft ) 0 ) rt tr O φ rt 01 Φ μ- O O Φ Hi O hi hi tr hh rt Pi Φ ø tr φ hf ø OJ tr ft ft hi o 0 ft 0 μ> ft Φ 3 0 ft ) 0 o hi 0 O Φ Φ Φ μ- P. Ω hi Φ 01 O rt 0 Φ tr Φ 0 μ- ø rt 0 01 0 φ Ω TJ P. ø Pi It ø ft Hi Λ hh μ- h- 1 μ- O φ μ- 3 φ Φ P. P. tr rt ft ) 01 μ- Φ hi ft ) 3 Φ Φ rt μ- CQ Φ S Φ 0 S 0 Φ 3 0 μ- rt hi 3 Ω hf H ft o hi μ- hi tr OJ LQ rt ø μ- ø ø - 01 i ft ) 0 0J 0 tn Φ hi Φ ft > N μ- P. φ o φ rt - 0J 03 3 ft ) Φ ft Φ ft ) μ- 3 μ- μ- Ω 03 rt Ω Λ • It ft P. P. N ø hi P. φ 01 ft ) O μ- 0 P. tr Ω J Φ Φ ft O Ω <! o 03 03 tr hi 0 ) μ- ø 0 Φ ^ 0J 0 ) • Ω φ μ- hi rt ø ø ft TJ Φ φ Φ μ- 0 ø μ- Φ o 0 Ω μ- 0 Φ O rt ft ) ø 01 μ- > hf TJ 3 *< P. ø Φ ft ) μ- ft ) LQ 0 TJ μ> hf LQ rt o μ- 1 0 01 O rt LQ 0J OJ TJ φ ø 01 rt CQ S rt φ TJ 3 CQ o 01 ft hi o LQ TJ μ> TJ 01 0 Φ φ hf ^ tr tr 3 hf p. TJ φ φ tr tr φ ø hi O ft ) ft hi ø O μ- φ O 03 • ft ) O Ω Ω CL ft 0 0 φ O OJ ft ) P. W 0 ) μ- P. It Φ Hi Ω o Φ • P. hi LQ hi Ω Ω ft j rt 01 s: t, rt a- ft ) μ- ft ) tr 0 0 0 Ω ft j H ft ) 0 01 Ω 0 ) hh Ω hi Ω ft ) ft ) 0 ~ Φ μ- ft ) Ω O Φ tr tr μ- hf 0 ) 0 ø Φ rt rt ft Φ 01 Ω rt ft ) o tr hh Φ ft O ft ) P. rt P. ft ) 01 M Φ hf 01 φ φ rt O ø μ- LQ P. μ- 03 O Ω μ- tf P. s 0 ) O hf tr hi O 0 • <: μ- h- 1 ft 03 TJ 0 hi tr P. Pi tr μ- it* oo o 03 O Ω O μ- 0 μ- hi hh 0 ) Φ Pi tr 03 tr μ- 0 ) π Ω ft Φ φ hi rt LQ 3 O o ø O Hi hf ø < Hi TJ 01 hf tr μ- μ- 3 TJ TJ ft μ- 0 rt μ- μ- tr «. 0 ) ft ) o O ► 5 φ hf o P. φ hh ft hi 0J Φ o 0 φ ø φ hf tr 01 LQ O rt hi ft ) Φ 01 0 ) μ- ft O o 0J 0 ) P. hf μ- ft ) • φ tr o hi Λ * 01 LQ Ω ø O ft ) ft ) hf rt tr Ω ø < φ rt OJ h{ μ- rt P. h{ ft ft O ø hf hi Φ 0 φ tr 0 Ω It 3 rt Ω "< rt p. O tr 0 Φ <! Φ 0 O tr rt tr hj ft LQ > φ 0 h- 1 μ- φ tr μ- ft ft ) μ- φ Φ Hi Ω ft j ft ) μ- rt M φ hf Pi 0 ) ø φ 3 ft ) 0J 0 ) Φ tr hh 01 0 - 0 OJ LQ 0 Φ 1 O Ω ø O 03 P. Ω 1 μ- rt Q 1 rt tr hf ø Φ ø hi Ω μ- rt O It o 0 rt tr Ω It 1 O *< ø 03 φ ft ) μ- ft hf <! Φ 3 OJ OJ 0 ) p. O μ- ft ) rt ft ft Φ O 01 O hf ft ) 01 Ω φ *< * ft ) rt 0 Φ μ- < ø <! tr Ω 0 ) ft ) ft ) φ H 1 01 rt hh ø 01 Φ φ 3 φ 01 φ Pi 01 Φ rt tr Ω Ω P. 0 μ- φ Φ 0 h- 1 ø 01 Pi OJ TJ <J 0 Hi 3 3 rt TJ tr ft £ 01 hh P. Φ It Φ o φ Φ ft ) LQ Ω rt hf μ- 03 rt μ- 01 01 OJ rt hi ft φ hf Φ Tl TJ tr 0 *< tr ft ) O hh Hi rt ø tr ø hf h( CQ ft ) φ tr 01 01 rt 0 0 ) 3 hf 0 φ tr φ tr ø μ- ft ) Φ φ 0 ) ft Φ ft Φ ft ) 3 o 03 Φ μ- 0 Φ tr hh • Φ μ- • LQ φ φ hi TJ Pi Φ Hi Φ ft ø ft hf hi rt Φ 3 Φ 3 Ω Ω μ- μ- H Ω ø Φ 01 0 O ø ft ) LQ hi φ ø Ω Φ OJ μ- φ μ- LQ 0 ft j ft ) hi φ μ- hi φ It It ø rt It ft ) LΠ μ- < Pi < hf cn 0 n φ rt ft 3 hi Φ o hi 0 0 hf ft ft rt 0 ) ø •• ø O μ- tr μ- TJ h{ φ • Ω Φ ø tr hi 0J ø Ω μ- μ- φ ft ) rt OJ 01 ø hi Φ 0 0 tr 3 ø <! rt Hi hi 3 Φ < J ft ) Ω ø O - ft ) Ω Φ Φ tr φ ø 0 ft 0 ft Φ tr tr Ω Φ 01 hf hi Φ Φ 01 φ μ- μ- hi ø μ- p j ø 0 rt M 3 0 * 01 01 03 μ- ø φ ft φ Ω Φ μ- 01 Φ Φ 0 ø 03 O O μ- 3 hh tt hf P. μ- μ- 0 J 3 hh Ω 0 φ <J 0 ) Φ rt 3 rt hf > 0 Ω P. ft o rt ø 3 0 0J *< ø j rt o hi φ ft ) P- o μ- Λ Φ p. •S μ- φ hi tr h- 1 O O O μ- μ- hh μ- <! φ 0 ) Ω It ω ø 01 μ- ft ) <! φ ø rt ø ø 03 3 Φ 01 H μ- tr CL ft ) Φ ft 0 hh hh Φ o O φ P. It It It rt £ 0 o μ- 0 01 01 O < <J μ- Φ μ- ft j hf φ Ω ft j hf rt hf 01 it H ø 01 ø hi tr tr μ- 01 01 It Ω φ 0 0 μ- Φ ø It ø ft Ω tr ft ) Ω Ω ø > < o Φ hf + + Φ Φ 0 • <; rt Φ μ- ft ft rt S tr tr hf hi Ω ^ LQ tr rt tr hf o It 0 ft Hi p. hi tr μ- 00 to Ω P. μ- μ- tr 01 tr tr tr £ K s: ft ) s: Φ ft ) φ Φ Φ Φ o < 0 ø hi 0 OJ μ- ^ tr O LΠ rt • rt rt ft Φ p. Φ 0J μ- N μ- rt OJ ft j 3 tr CQ P. P. It TJ Φ hf rt 0 hi TJ μ- hh 01 ø 0 0 n n hf OJ φ μ- Ω rt hf • rt TJ rt φ M φ 3 O 0 hf . Φ φ P. hf hi hi 3 rt μ- *1 tr μ- 3 Pi φ 0 h Φ tr rt Tl Φ ø Φ Ω rt It μ- 0 O 3 Φ ft Φ Φ μ- φ μ- Ω 0 M 01 TJ μ- M 0 hi It 03 μ- tr M hi rt ft ) 0 φ Ω OJ ft Ω cn Ω J 01 tr h ft ) Λ ø ft ) ø hi φ φ φ φ 0 Φ tr TJ tr ft ø Φ μ- CΩ TJ 0 Ω hi TJ Φ 0 O H φ φ CQ 0 < ø LQ tr Ω TJ hf H Ω φ a Φ Φ φ Ω o hi ft ) It o 03 ø 03 Ω 3 OJ ft ) hi φ o 01 μ- 3 Φ 0 J O ft ) φ rt Ω 0 Ω 01 rt Hi PJ hi O Φ ft ) 0 μ- TJ 0 ft 0 tr J ft hi φ OJ ft ) 0 rt hi 0 hf CΩ ft Ω hi It Φ M ft J 0 tr 0 It hi CQ M O hf μ- O Φ Φ Φ h- 1 tr Ω <! O o 03 H 0 03 Φ 0 rt μ- μ- 0 0 ft ) Ω Φ ø μ- 3 Φ 03 ft ) ø 0 rt Hi hf 0 ø P. φ P. ^ φ hh ft ft ) 0 Ω μ- hi hi Ω O Ω 03 It hi tr P- O o P. 0 O H Ω ft ) hi ft 01 μ- Ω ^ μ- P. ft ) Φ ft 03 OJ 03 Φ tr Φ μ- ø μ- 03 O It hi ft j ø μ- ft ) O Φ tr Φ O μ- ft ) 0 rt φ tr ft 0 rt 03 Ω Ω Φ μ- ft ) ft ) 3 03 01 rt ft ) Ω hi hi 01 Λ hi M It 01 Ω hi OJ 0 ) ft ) tr tr ft ø ft hf CQ φ P. 0 hj 01 hh £ Ω ø φ rt Φ ft O 3 01 φ 0 μ- μ- 0 0 0 φ cn ø Φ μ- OJ μ- φ Ω tr 0 Φ 0J 0 ) ø Ω LQ ø μ- 0 Ω μ- 3 3 O Φ Ω M O Ω H P. 0 Ω φ LQ hh ft tr Φ rt rt hi rt Φ 0 ft c o 01 TJ 3 Ω It h- 1 O TJ φ H ft ) 0 O ft ) ø tr TJ Φ ft rt P. ft ) ft ) tr O μ- LQ o ø rt hi φ It Φ ft ) 0 ft ) φ μ- ø hi ft ) ø Ω 3 rt 0 tr hi Pi TJ hf O ft ) Φ ø O hf hi μ- μ» - 1 μ- O μ- O i • <: μ- 0 Φ μ- 1 TJ ø μ- ø hi h J Ω o 01 μ- ø o 01 hf O hh H hi Ω 0 ) 0 rt *< Φ ø hi φ ø ft rt μ- Ξ o Pi tr ft ) ft ) * * μ- Hi Ω Ω Ω TJ J 0 ) TJ It CQ tr TJ 3 rt hf s; ft ) hf tr P. ft ) OJ 0 Ω φ Hi 3 hi ø ft ) tr Φ Φ ø Ω μ- ø 0 O tr O 0 M Ω hi 0 ) Φ ft ) O φ tr ft ) tr o> Φ Φ ø ft 03 O 0 ) hi μ- It rt rt Φ P. Ω ø < hf ft ) ft ) 3 It ft! Ω o 0 hi ø φ It o hi It 03 Φ Ω hi Ω Φ μ- Ω φ φ 0J Φ ø 0 P- φ 3 ft ø TJ Φ Ω O tr 03 Φ It It hi 0 - 1 Φ 0 TJ Ω μ- P. μ- hi tr Λ Ω ø hi μ- Ω tr hf ø μ- LQ O K φ 0 Φ hh μ- ft ) μ- φ 03 Φ TJ 01 hi H. ø Φ 0 h_ 0 ) TJ It ø ft TJ μ- ft ) CO It H o ø φ ø H • 0 hi rt < ø O • Φ 0 μ- It O M Ω 03 φ tr h- 1 0 μ- μ- μ- o LQ Ω rt μ- tr Hi LQ 01 Φ tr tr It μ- Φ μ- 0 ) It ø μ- o ft ) tr <i TJ Φ 01 ft ) It φ 0 Φ £ o ø 3 o 01 0 * " 0 ) O Φ ø μ- *<: ø Λ <! hi - φ CΩ H TJ It ft ) μ- rt LQ Ω It TJ Ω φ Φ ø φ ø 01 M rt ø hh rt μ- rt 03 ft ) ø μ- ^ P. 0 Φ Φ 01 P. μ- hi μ- O Hi ft! • <: μ- hf O ft μ- ^ μ- φ 0 ) O tr ø 01 0 ft ) Φ rt μ- 01 μ- hi Pi φ O ft ) M hi O hf ø 5" tr μ- 01 o tr ø P. 3 tr ø ft ) 0 ) ft! 0 P. 0 ^ ø μ- ft ) ø TJ 0J tr P. ø M hf ft ) Ω < o ft ) 0 hj H P. ft ) o H It It LQ μ- Ω Ω LQ ø tr Ω 0 ) It ft ) Φ ^ ft ) Ω It ft ) φ i 0 01 . hf φ μ- P. tr *" <; μ- tr μ- 03 rt Ω O ft ) Ω 0 o hi μ- ø Φ hh 0 ft μ- < φ ø μ- 0 ) φ 3 hh φ Φ φ Φ ø tr Φ ø o ft ) O 3 JT ø TJ Φ <! hi It o Pi ø 0 rt 0 o hf 0J μ- rt 3 3 It 2 3 φ μ- Hi It hi LQ ^ LQ tf hf TJ P. hj Φ J μ- ø hf tr μ- hf Ω hf φ tr μ- Φ Φ tr O φ ft ) ø φ φ Φ μ- P. • TJ Ω hi ~ > o Φ - O Ω 0J ft ) TJ Φ rt 0 μ- M hi 0 ø Φ h{ ø 01 hf Ω rt μ- ft ) h{ μ- o φ Φ φ h- 1 It TJ ft ) hi ø Pi ø ft ) hf • Ω μ- 0 ) Φ ft ) ø rt < φ It 0 Tl Φ rt 03 ø 0 ø 3 Ω It φ φ Ω Ω ft ) ft ) It φ μ- rt rt Ω ft 01 ft ) O 01 hj hi 0 μ- tr TJ Ω Pi TJ TJ TJ It φ 3 hf - ft ) It 0 ) ft TJ 01 > hf 03 μ- It μ- 0 ) . ft ) P< <! Φ ft ) It O ft ) O ø φ rt hi hf Φ 01 J ft M Φ hf μ- It μ- μ- Ω 03 Ω O h{ o 01 rt Φ 0 3 Ω ø <! 03 03 tr hi tr μ- O L TJ 0 Φ μ- φ μ- P. 3 μ- ø 3 ft ) 0 0 O ø o> hi hh φ It ft ) μ- 03 03 ^ It Φ 03 LQ Ω hi φ h- 1 tr μ- φ < It μ- 0 μ- μ- 01 03 P. -3 It ø ø μ- TJ 0 ) ø μ- Φ μ- φ hf Hi 0 ) tr 0 ) 01 φ hi ft ) ø Φ O rt rt o Φ S φ tr rt ft ) rt Ω J 0 LQ tr Pi Ω φ 0 CQ ft ) O 0 ft Ω ft ) o ft ) 3 μ- • μ- Φ ft ) It CQ . φ μ j P. ft ) 01 01 3 hi It hh 0 O rt It 0 It hi Ω O hi O £ μ- It ø M LQ * μ- ft j φ ø Ω Ω 3 ft ) hi hi hi μ- 0 tr ft ) TJ hf μ- ø tr M o Φ φ 01 1 S Ω 3 03 o μ- ft! μ- P. O Ω Φ O o Φ H" Φ Ω Φ ft ) Ω 0 OJ hf 3 O μ- ft ) Φ tr rt Tf ft ) hh h- 1 - ø 0 hi ft TJ P. ø μ- μ- hf ft ) 0 It It O tr 01 p. O ft ) ft ) hi rt It ft ) μ- O Φ it μ- LQ hi O Ω ft ) Φ Φ Ω hh tr ft ) tr 3 hh Φ Φ hh TJ tr μ- 01 LQ Ω rt It 0 ) tr μ- 01 H O hi ft ) hi ft ) φ hi rt μ- φ ft ) μ- rt TJ 0 ) 0 ) hf TJ h- 1 Φ o ø tr TJ μ- ft ) tr rt hi o 0 *< 01 Φ ft ) O 01 03 ft ) μ- tr hi M 01 tr O Ω TJ P- Ω ft ) X ø hi hi hh Ω Φ O PJ hh LQ 01 Hi 3 01 O φ It rt O h{ CQ Φ ø It Φ P. O O hj ft ) ft ) ø 01 Φ CO 0 μ- tr h{ rt It rt hh φ Ω Pi hh μ- μ- 0 ft ) ft ) O H Φ hi μ- hh 0 ft ) 3 O 3 Φ < Ω Φ μ- It It φ tr μ- ft μ- μ- o 3 O ft Ω φ Φ ø 03 Hi rt 01 It TJ TJ t, It φ ø μ- It H" Ω O tr tr 3 ft ) Ω φ 01 μ- Hi φ ø μ- Ω ft ) 01 It 0 o μ- 3 0 0 hf h- 1 ø tr ø 03 P. Hi tr φ μ- ø Φ Φ It μ- hi M Ω 0 μ- o O J TJ Φ 03 Ω hi O ft ) 3 01 O Φ ft> rt μ- φ Φ Φ Ω hj Φ 01 ft ) ø P. CΩ o TJ ø ø hf TJ Φ Ω tr ø LQ hh It *• 3 μ- TJ rt ft ) hi rt Ω O 3 Ω s: < 0 rt CQ μ- 0 Hi hi P. φ Ω It 0 φ ft ) 0 ø ft ) O O μ- ft ) ft Φ hi 0 hi μ- ft ) μ- Φ ft O 03 < Ω O J TJ μ- ft! It hf hi Ω P. M μ- LQ Ω hf μ- hf tr ft ) <! J 0 rt O μ- Ω H hi μ- hi Φ μ- tr rt Ω ft ) hi ø hi O ft ) rt Ω ft rt 3 ft ) 01 μ- TJ hf o P. rt Ω hi μ- h- 1 ^ 0 ) rt P. P. tr Φ hf 0 LQ s: P. J M μ- ft ) ø <! o μ- 01 < tt 0 ) Φ - Φ O o tf 03 tr J ø ft j Φ P. rt Ω Hi μ- Φ 0 ) μ- ø C P. φ hf O μ- Φ s ^ hf 01 01 £ 3 J H tr hh hi tr ft ) TJ 0 μ- Φ It hf hf tr P. <! Φ hi P. ø 01 O φ 0 ) TJ μ- TJ hi ft ) φ hi s: hi O Φ μ j Tl 3 h{ Ω CΩ O O M ft ) 0 ) hi μ- OJ • : μ- Hi ø H ft ) ft ft ) o rt Φ O It O Φ φ tr hi ft> φ Φ 0 03 3 0 3 ft < ø O 0 ft ) TJ 0 h- 1 ø 0 Ω 01 01 tr ø Ω μ- It 3 01 φ φ φ hf ft ) M It tr P. Φ rt μ- rt Hi M LQ CQ O Ω It P- 01 Ω 01 0 01 Φ 0 0 ) M TJ 0J 01 P. ft ) tr rt Φ rt μ- P- ft ) μ- 01 ft ) ft ) φ O μ- Ω It ft ) 01 ø tv TJ Φ μ- £ φ It 0 0 hf tr Φ tr It Φ 0 ø Q H rt It O 01 TJ tr 01 0 ) 01 hf tr tr μ- rt 01 - φ hi ft ) Ω ø μ- Ω ø h{ hf Φ Φ It tr hf ø ft ) Φ rt 0 - μ- ft ) μ- P. 3 μ- O 0 O 03 rt μ- It CΩ μ- μ- μ- ø μ- hf Φ 03 μ< 01 3 j H tr Ω rt < tr 0 μ- ^ OJ φ O hi rt tr rt " hi ø ø ø ø Hi φ :> H ≤ φ ft o\° H μ- tr ft ) μ- hh 0 01 ø tr μ- Φ hh tr μ- O s: LQ LQ rt <! 0 ft ) 0 ) 0 μ- ^ ft ) tr φ rt Φ hi LQ LQ μ- ft ) O ft ) ø 0 o tr P. tr Hi tr φ M It 01 hh > 0 μ- Φ φ O μ- hi μ- tr ft ø tr ø hh hi It It It 0 It H Φ Φ Φ ft ) It O Φ ø > Φ 03 H Hi Pi ø hh rt <! It o tr It *< Pi O O o P. tr μ- 1 CQ hf TJ tr hi rt 0 Pi o It 0 Φ O φ o 0 Φ O rt hi Ω It ft ) *<; μ- Φ TJ φ 3 ft ) μ- s: Ω tr ft ) h{ Ω 01 tr O ft ) 3 It 3 ft! ft ) TJ O μ- ft ) μ- φ ft Φ 3 φ 0 Ω O TJ ø ø 01 tr φ ø hh PJ LQ O Φ 01 0 particular embodiments thereof, will be explained more closely in the following description with reference to the drawings, in which: Fig. 1 shows an electrical circuit diagram in partial block form, according to an embodiment of the invention, Fig. 2 schematically shows an exemplary embodiment of an apparatus according to the invention being particularly intended for measurement of moisture in bulk goods or continuous materials, Fig. 3 in a corresponding schematic manner shows an embodiment particularly intended for measurement on a liquid or mass received in a measurement vessel, Fig. 4 shows an example of an apparatus in the form of a spear-like tool for measuring moisture in bulk goods, Fig. 5 shows a block diagram of an embodiment with three electrode-oscillator probes in a system, e.g. intended for level measurement, Fig. 6 in cross sectional view shows a level measurement apparatus based on a tubular structure, e.g. for the measurement of tank levels, such as at gasoline stations, Fig. 7 shows a schematic vertical section in the form of a separation or sedimentation tank in which there are installed three separate rows of electrode- oscillator devices according to the invention for measuring interface levels between different fluids in the tank, Fig. 8 additionally shows a specific embodiment of the apparatus according to the invention in vertical section, for the purpose of measuring a level or an interface between two surrounding fluids, Fig. 9 shows a cross-sectional view of the apparatus of Fig. 8, Fig. 10 in block schematic form in a corresponding manner as Fig. 5, shows the electrical measurement system that can be employed in association with the apparatus of Figs. 8 and 9, and Fig. 11 schematically shows an apparatus according to the invention for detection or measurement of flowing fluids. In Fig. 1 the oscillator circuit is generally denoted 15, and it is seen that this is an LC oscillator. There is included an active component in the form of an NPN transistor Q4, whereas the frequency determining components in the first place consist of a coil L5 and a capacitor CIO . In parallel to capacitor CIO there is the capacitance being re- presented by an electrode 10, which is shown here in rectangular plate shape as a typical design. The side edges of the electrode are denoted 10A and 10B, respectively. Coil L5 is an air core coil, i.e. without any other core material than air. This is a great advantage in view of the desired high stability being required in this connection. The capacitance of capacitor CIO shall be as constant as possible, whereas in contrast the capacitance being represented by the electrode 10 in parallel with capacitor CIO, will vary depending upon the medium that may be present as a dielectric for electrode 10, namely in this case between the electrode and ground. In other words Fig. 1 does not show any other counter-electrode than ground with respect to electrode 10. This additional capacitance or measured capacitance being parallel to capacitor CIO, will have an influence on the output frequency of the oscillator circuit, and it is this variation of the output frequency that is utilized for the intended detection or measurement. Other components incorporated in oscillator circuit 15 are of conventional type and function, among other things for applying required operational voltages to transistor Q4 , whereas in contrast component RT3 is a temperature-dependent resistor, such as a so-called NTC resistor. This is physically located in close thermal contact with air coil L5 , primarily for the purpose of providing for temperature com- pensation in oscillator circuit 15, so that the output frequency thereof to the extent possible is independent of the ambient temperature. Accordingly one of a number of sources of error are eliminated to a substantial degree. At 15F there is indicated an output unit for the oscil- lator frequency, that is converted in a following counter 19 >» ω LO to to H μ> o LΠ O Ul O Lπ o LΠ ft ) Φ o Hi μ- μ- μ- 3 hi ft μ- ft s: 01 *] It Φ Ω It rt rt H Λ μ- tr Φ ft rt rt P. It 01 tr P. ft O μ- M hh 01 M rt ø φ ø Φ o Φ 0 tr μ- μ- μ- ø 1 h- 1 O Φ tr hi Π f_ 01 Φ ø tr tr tr hi μ- μ- 0 ) μ- μ- Hi 01 03 Hi Ω 0 LQ Ω It & 0 hf ft Φ ø LQ LQ hi Φ 0 3 Φ O Φ Ω Φ φ ft ) 0 ) 0 LQ J 3 o 0 Φ μ- φ μ- It φ μ- 0 0 φ P. ø O Ω < TJ P. 0 ø w φ rt s: 0 0 φ Φ ø ft φ Ω 0 01 ø 0 p. ft ) hf $. 0 ft ) 0 ft Φ Φ PJ Φ Ω o Φ Ω μ- μ- 01 ø Φ 2 > M H LQ hi hi hi Ω ι Φ TJ 0 ft ) ø μ- ø 0 03 i S 01 ft ft μ> Ω ^ s; P. 3 μ- μ> 0 ft ) 0 ) CΩ 0 ft ) Φ Ω hf μ- φ ø ft ) ø - tr μ- rt ft ) rt to μ- hi It ø TJ rt ø LQ hh 0 ) μ- μ- φ 3 It O P. o LQ 03 H M to TJ Ω Φ It 0 o LQ O μ- ft ) φ 01 ft μ 1 O tr Ω ø 03 μ- o ft φ 3 " hi 03 0 03 to φ hf Ω 0 0 ) hi 0 ft ) • Hi cn i It Ω hi rt • Φ Φ ø Φ 0J rt 0 rt hf tr 0 ) 3 hf 03 01 O ft ) 0 - hf rt r ø tr μ- ø tr ft ø 01 hi μ- 3 tr Φ h{ rt tr φ o hh 0 O o 01 Ω 0 μ- h- 1 to Φ tr t ft μ- Φ tt ft ) Φ H tr LQ Φ ft ) Φ Ω tr 0J 0> tr μ- ft ) hi hh hh φ Φ rt *< co o hi tr o rt o μ- 1 0 O μ- ft to • • P. hj μ- Φ ft φ < 01 Ω Hi 0 01 Ω 03 O 01 φ Hi φ o hi ft ) P. 01 tr X μ- P. Φ hf tr Φ 0 φ Φ Φ ft ) Φ Φ ft 01 φ t Ω O Ω 0 tr 01 ø Ω Ω rt μ- LΠ H 3 OJ φ 03 Ω Φ 0J LQ hi Ω . Ω 0 μ- μ- μ- ft ) VO O μ- 3 μ- LQ 0 Φ 03 01 It π O rt tr 3 TJ o tr φ Ω LQ TJ 0 Ω rt φ 0 ) φ ft ft Φ Ω φ ft ) 0 P. 0 03 TJ μ- 1 tr s: o tr TJ μ> 0 0 μ- φ O hh Ω Φ ø Ω hj φ μ- ft 0 3 rt tr ft ) Ω M iQ It P. Φ 01 μ- 0 o ø o 0 ft ) 01 ø μ- 3 01 O Φ Ω rt hf o 3 LQ φ to tr Φ O J rt It tr ø tr ø ft ) ft ) ø hf hf ft Φ rt ø to 01 μ- hf Φ ft μ- tr Φ hi ø Φ hf hh 01 hf hh ft ) O ft ) Ω o 03 rt OJ rt Ω ft ft ) Ω Ω 01 rt ft ) 0 o P. to Ω l_l. rt O It Ω Φ 0 μ- Φ ø rt rt 0 0 ) o CΩ ø φ Φ Hi ø It O O 3 ø hj ø μ- Tl ft LΠ ft ) φ hf 0 O hi o £ M Ω ft ) P. ft ) μ- 01 It hi tr hi 03 0 ) hi p. μ- 01 ø μ- Ω 3 P hh 0 ) ø o Ω μ- 0 O 0 Φ hh μ- ft 0J ft μ- <! φ μ- o Φ 0 0 Φ o Ω ø 0 ) 0 ) LQ ft ) μ- ft Ω P. hi Ω LQ ø ft 0 TJ 3 ø Φ P. o Ω hi g ft ) o P. Λ Ω ø μ- φ 0 rt Ω "< LQ 01 hh 0i Φ μ- μ- P. μ- H hi hi μ- ø μ- ft CT -> hh 0 o 01 M Ω ø 3 tr Φ hi ft hi μ- to Ω P. hj o 03 o o < Φ φ Ω 01 3 μ- hj o 01 Φ μ- M ft 01 tr o Φ Φ O ft O ft ) φ O φ 0 ø € ø 01 hi μ- ft ) ø Ω Ω Ω P. Ω Φ ft 0 μ> tr ft! μ- ft Φ hi O - 1 tr ø Ω M rt hi 0 ft Φ ft ) ø O φ O 3 It μ- ø O μ- O hf 0 ) Ω Φ It o hi Φ Ω Hi 0J rt Φ 0 rt P. O φ 0 φ P. Pi to to O Hi 0 TJ μ- Φ 0J hi μ- 0 3 0 hf tr T^ tr 1 It o ø 0J hh o ft tr Pi μ- H Φ Ω 03 ft ) t |J ø It hi M hf ø Ω rt P. φ 0 O LΠ s: hi ft O i ø Φ μ- φ h{ <J tr ft ) ft ) Ω ft TJ Tl - • 1 ft ft ) O PJ μ- 0 ø ø Φ hi φ - Φ μ- Φ ø Φ P. o 0 ft ) φ rt rt μ- μ- ft ) ft Ω tr It Ω hi 0 ) Φ μ- to Ω rt Ω H Φ Ω rt Pi 0 ft 0 φ ø μ- h- 1 Φ rt μ- 01 μ- μ- 0 03 Ω φ £ Ed O Φ μ- Φ μ- ø rt LΠ ft ft s: μ- tr hi ø μ- & ft ) Ω Ω 01 ø Φ 0 φ ø ø o O 0 Φ P. tr M 0 O 01 rt • Ω O s: μ- O ø Φ Φ hi μ- μ- μ- ft ft ' < Ω Pi LQ tr ø ø Φ Φ P. 01 ø 01 ^ 01 t tr hi tr 0 hf 01 01 rt Ω 03 ø μ- O hi μ- φ o ft ) 01 01 o O ft H Ω 0 rt O o Tl -0 ft ) Φ ø It ? Φ TJ tr 0 ø 01 hi O TJ ø Hi TJ Pi rt tr 0J H Ω hi o φ It Ω hi hi It 0 CQ <! M hi 01 tr ø φ Φ μ- 0 ) rt P- 03 It 01 H 0 0 ) μ- 01 0 ft! ft ) h{ ft 0 o ft 0 0J μ- Φ Φ 0 Ω Ω ft H tr rt hi φ μ- ft ) 0 0 φ 0 TJ ft TJ tr 03 O μ- Ω O TJ h- 1 ø ø ft ) μ- 3 £ 0 It l_l. 01 Φ tr Φ φ ft o ft 01 μ- TJ φ O φ Pi <! ft h{ rt ø ft ) P. LQ Pi 0 ) ø Φ ø ø μ- 0 μ> 0 Φ LQ ft ) μ> tr 0 Ω 0J ft ) ft μ- ø hf i CQ ft Φ φ 0 tr ft It ø ø <; 0 Ul 0 ft ) P. o Φ 0 ft P. 0 OJ ft ) Pi 0 ) μ- φ tr hi Ω φ μ- OJ ft ) to TJ O It £ Φ φ Ω 01 rt hh hf 0 μ- P. μ> TJ μ- Ω o rt X Φ to 3 Φ O 01 0 ø 0 μ> " 01 μ- 0 ) Ω ft rt μ- tr 0 P. H rt Hi 0J 0 O μ- φ TJ Ω ft hf μ- TJ o 0i 3 ft ) μ- ø ft ) Ω o > < ft μ- tr LQ h- 1 ft ø rt H P" ft ) ft ) μ- O ^ Φ μ- H s o 0 0 o ft μ- TJ hi LQ ft ) ft ) Ω rt μ- ø CΩ μ- o Φ ø hf H 0 M P. φ μ- Φ φ hi It Ω Ω ø 03 TJ μ- Φ ø 0 hi 0 o ø CQ o Φ μ- >• O ø μ- O iQ ft μ- hj t O Ω LQ Φ φ φ O φ TJ 01 hi It ft ) OJ hi ft ) 03 O 1 M ø ø tr Ω Hi Hi s: Ω 0 ft ) 1 ( ) ø ft hf ø P. 0 S Pi o μ- j φ ø μ> M O TJ 01 0 ) iQ 01 01 ft ) 3 ft ) μ- μ- μ- TJ ^ 0J z 03 Φ hi Φ rt 03 < tr 03 0J ftl μ- hi LQ CQ 03 O Ω Φ tr ft - O 01 Φ J Ω LQ ø hf μ- μ- s: rt O Φ μ- 0 Φ Φ ft μ- TJ H iQ φ Ω LQ μ- hi ft ) o tr ø ft ) 0 ) 0 LQ 0J Ω ø ft ) Φ μ- 0 P. hh ø Ω * hf o rt TJ • hh 3 0J hi 1 ft ) ft ) TJ hj ft ) rt 0 ft ) rt Ω ø hf Ω 0 ) ^ LQ 0 Ω Φ S hf tr Φ Φ Φ H μ- O φ hi Φ Pi rt rt Φ CQ tr s: ø μ- μ- rt Φ P. ft M ft M rt μ- O rt P. ft μ- ø to hi 0 Φ Φ μ- φ Φ Pi Ω Φ o rt 01 Φ μ- Ω μ- φ hi tr to 3 tr 0 ) It tr ft ) φ ft 0 LQ Pi 01 μ- 0 ) It <! μ- ø 0 ) rt 01 Ω ^ OJ 03 X 0 tr μ- O Φ ø hh tr Φ ø Pi O μ- hh It μ- Φ hj Φ ø φ ø 0 O Ω 0 ) 0 ft ) P. φ 01 n_ O Φ Pi ø 01 0 0 ft! to rt Ξ M Ω Ω rt hf h P. Ω Hi hi H Ω 3 3 Φ hf £ μ- μ- p. 0 hi 03 rt φ hi hh w φ> ft j μ- Φ 0 O tr φ 0 μ- ft ) tr φ J * φ tr ø iQ hi tr 0 Φ O ft ) It φ H rt Ω μ- 0 Φ 0 ft ) 0 TJ Pi 0 Φ Φ 1 ft ) 1 ft ø H hf X O tr 0 O tr rt 01 hi Ω ø O It Φ Φ H ø tr 1 1 OJ Hi φ hh Φ Φ ft ) P. Hi φ 1 t o ft I Φ ø hi 1 0 hh φ. ω OJ to to H H o LΠ o Ul o LΠ O LΠ Ω < 0 O o 0 ft ) It X ft TJ μ- ft ) 0 fti LQ rt M Φ ft 01 tr Ω hh μ- o ft ) O LQ 0 tr hf ø LQ ft j tr φ rt M . tr 01 *1 Φ μ- hh LQ Ω hi μ- O h{ 3 to Ω 0 It P. μ- tr o rt φ φ CQ 01 ft j Ω TJ 0 ft ) TJ o 0 ft ) ft h{ tr ft ) μ- φ It ø 0 01 03 P. 0 . φ Tl rt TJ > ft ) μ j μ- μ- 03 μ> φ o . CQ It tr It tr 0 tr Φ £ hi o o rt ø TJ tr LQ Φ Φ tr hf ft ) 3 rt rt o tr μ- hi Φ O Φ ø 01 ft ) Ω ft ) μ> 3 0 φ O 03 n Φ 1 ly integrated structure of oscillator circuit 25 with associated electronic circuits, in particular circuit 27 for temperature compensation, and electrode 20, it is obvious that these components can be assembled in such a manner that they have a relatively good thermal contact with object 2. The temperature of at least the adjacent surface of object 2 can then in many cases be sensed by the apparatus . In the embodiment of Fig. 2 the accuracy of such sensing will also depend on window 22. When in this manner the oscillator circuit has a good thermal contact with the medium, substance or material concerned, the output signals to the microprocessor can make it possible for the processor to correct also with respect to the temperature variation in the dielectric constant of the object, e.g. when there is a water content or moisture in object 2. Embodiments to be described in the following description can also be more favourable for the purpose of the correction discussed here. Advantageously the embodiment of Fig. 2 as well as other embodiments described, can be subjected to frequency calibration in the first place with air as a dielectric for the electrode, and besides preferably with water as a dielectric. This form of calibration is suitably performed during the running production of such apparatuses, because component values and other factors usually will lead to individual variations, so that the nominal output frequency must be determined individually for each electrode-oscillator probe under standard conditions. Fig. 3 shows an embodiment where a bottle-like measurement vessel 33 is adapted to receive a liquid or a mass to be subjected to measurement. Measuring vessel 33 can expediently be made of a plastic material. A cylindrical part 32 has an internal cavity for receiving the measuring vessel 33, and an electrode 30 in ribbon form is provided outside cylinder 32 around the circumference thereof. Accordingly, cylinder 32 consists of an electrically non- conductive material, such as teflon. When the measuring vessel 33 with a liquid or bulk goods filled in, has been introduced into cylinder 32, the electrode 30 will surround the measuring vessel at the level of the contents therein. Concentrically around cylinder 32 there is shown a screen 34 of electrically conductive material, e.g. aluminum. The geometrical relationships and dimensions are so chosen that the distance radially inwards from electrode 30 to the medium being subject to measurement, is much smaller than the radial distance outwards to screen 34. Nevertheless the capacitance between electrode 30 and screen 34 will be incorporated in the total capacitance that determines the oscillator frequency, namely as a parallel capacitance to that which exists radially inwards of electrode 30 in the cavity of cylinder 32, where the medium 3 in vessel 33 constitutes a dielectric. Depending on the properties of the medium this dielectric will represent a variable capacitance contribution that leads to variation in the output frequency of the oscillator and accordingly an output signal from the apparatus as in the embodiment of Fig. 2. Relatively schematically in Fig. 3 there is indicated an oscillator circuit 35 having a short conductor lead 31 to electrode 30 and besides a temperature circuit 37 and an analog-digital converter 38. Circuit 38 in this case is located outside screen 34 in a screen box 34A which is also provided with an output connector 39 for e.g. a coaxial cable . As mentioned above it is contemplated that the practical embodiment according to Fig. 3 can be based on a printed circuit board having the electrode 30 at one side and the oscillator circuit 35 with associated electronics at the other side. Circuit boards of such structure, that can be formed in an arcuate or circular ribbon-shaped configuration are available according to present-day technology. In particular for measuring moisture in bulk goods there is shown a spear-like embodiment in fig. 4. There is incorporated a rod- or thread-shaped electrode 40 which extends from oscillator circuit 45 forwardly in a front part 42 of the apparatus. Advantageously this front part is some- what pointed in order to facilitate penetration into the bulk goods, that can be e.g. bales of collected waste, such as paper waste. Whereas the front part 42 mentioned, in the principle should consist of electrically non-conductive material, the remaining part of the tool is based on a sur- rounding enclosure 44 of tubular shape and consisting of an electrically conductive material, e.g. aluminium. This part therefore constitutes a screen for oscillator circuit 45 and an associated electronics circuit 47 for temperature compensation as explained previously, as well as an analog-digital converter 48. At the rear end of this tool there is shown a rear wall 43 with a lead-through for a coaxial connector unit 49. Also in this embodiment there can in part be considered to exist a form of counter-electrode, namely in the form of the screen enclosure 44. It is more essential how- ever, that the object or bulk goods 4 being subject to measurement, to a high degree will have influence on the capacitance of electrode 4, among other things because the goods 4 as indicated, will normally have a good ground contact. In this case there is not at all any indication of a specific conductor lead between electrode 40 and oscillator circuit 45, since the electrode can extend directly up to a point of connection in the oscillator circuit itself. When there is the question of measuring a liquid level in a tank or the like, it is highly relevant to employ a number of electrodes being located in a preferably vertical row in order that a varying liquid level can be detected or measured with a desired resolution. Such an embodiment is shown schematically in Fig. 5, where there are shown three such electrodes 50A, 50B and 50C. These electrodes are shown in the principle with a rectangular plate shape and with closely connected oscillators 55A, 55B and 55C, respectively. For each such electrode-oscillator probe there are taken out two leads as shown e.g. at 55T and 55F for electrode 50A. Thus, there is also here a frequency output signal 55F and a temperature output signal 55T, and correspondingly from the other two probes. For controlling or activating the probes according to a desired program or a measurement procedure, there are provided two selector circuits 51 and 52 for handling the frequency signals and the temperature signals respectively, and convey these to an output unit 56 with an associated connector 59 in similarity to the preceding exemplary embodiments . As in the preceeding examples there is included for the temperature signals, an analog- digital converter 58 in the block diagram of fig. 5. There is not shown any specific microprocessor or com- puter in Fig. 5, but unit 56 can possibly be considered to incorporate a microprocessor. A microprocessor or computer can particularly in such an embodiment be adapted to provide for frequency calibration with respect to the individual electrodes 50A, 50B, 50C having each an associated oscillator circuit, based on suitable programming of the microprocessor or computer, including the possibility of adaptive calibration or adjustment during the operational time of the apparatus. Such calibration can suitably be performed de- pending upon whether the electrode concerned is fully immersed in the liquid in question or is located as a whole above the liquid level. In most cases it will be simple to decide in an unambiguous way whether or not a given electrode is fully immersed. Fig. 6 shows an embodiment being developed particularly for measuring tank levels in gasoline stations and the like. For such purposes there is employed an arrangement having av vertical row of electrodes as in Fig. 5, but preferably with a still higher number of electrodes. The practical embodi- ment of Fig. 6 is shown in the form of a cross-section through a tubular structure adapted to be inserted down into and installed in a tank. Existing gasoline station tanks will often be equipped with vertical ducts or tubes, among other things for conventional level determination, and the apparatus according to the invention as in the embodiment of Fig. 6, can be adapted with advantage to be introduced into such existing tubes or ducts. The apparatus will then still make possible conventional level determination as just mentioned. The cross-sectional view of Fig. 6 shows an outer or surrounding protective tube 64 of steel, i.e. an electrically conductive material. Inside this there is shown a non- conductive tube 63A, 63B having an internal partition 62. Preferably this is substantially planar as will appear from Fig. 6, but apparently can have other geometrical shapes when seen in cross-section. The major part of the tube cross-section within the wall 63A is here adapted to receive the liquid 6 the level of which is to be measured. With fluid-tight separation therefrom by means of partition 62 in the other part of the tube cross-section, there is provided Φ 1 0 03 4 φ MH rl 1 A! 1 o Φ rH £ rH i TI 0 Φ CQ O ϋ -H rl 40 -H 1 1 XI id CQ SH -H SH 0 A SH φ 40 o 40 J r- © ϋ ■ H CΛ vo 00 Φ 03 VO Ov rH 40 o Φ 40 J -H 0 SH ø H Φ Φ rd ϋ υ A O 0 SH 40 id A -H -r-i ϋ 40 TJ 40 rd rd -H Φ ■0 0 SH 40 φ υ ø A 40 o 40 -H id CQ ϋ SH A Φ CΛ 40 MH VO -H O & £ S φ T) Φ 40 rl 40 TI id ϋ -H 0 0 id CQ fd A 40 in 0 Φ TJ 40 O 40 0 -H ϋ -H rd 0 CQ o 0 0 in rl -H L VO -H Pl O H O SH O O id Φ 40 0 ,0 rd 0 40 40 rH o rH Φ 40 -H o CQ < ϋ O o CQ r-i • O φ V CN J VO 0 o TJ id SH Φ 0 40 40 o 0 o rd -H SB φ ϋ 40 o r- H O -H A φ rH 40 CQ SH 00 0 CQ rd CQ id -H Pl -H rd 1 1 Oi 1 . Tl 1 x-i 1 1 | Φ 1 1 φ -H XI ι rH 1 O . Φ X! , Φ SH MH Φ H xi • ti 4θ • n 40 • rH CQ rd υ 40 1 40 tn 40 Oi Ol > Φ 0 • ti O 40 IΛ 0 0 Oi 0 Φ tn H 0 0 Φ SH 0 -H Φ 0 -H cα O CO r-i -H Φ • -H X! Φ -H rd -H « Φ O • ti r-i Xi -H o fa 0 XI -H Φ 40 0 H 0 SH MH MH r-i Tl ^ r-l tn 0 01 o 0 CQ o 0 id Φ -H 03 . 0 id -H -H 0 T) 0 Φ Φ SH X! 0 tn CQ 0 O • 0 r-i fa 0 -H Φ 0 SH -H -* td <tf υ -H Φ 5 XI φ 40 tr φ 0 40 -H Oi Oi 0 id Φ • ti MH O N Φ

Claims: C l a i m s 1. Apparatus for capacitive electrical detection or measurement with respect to a medium, comprising at least one electrode (10) and an associated oscillator circuit (15) the output frequency of which is a function of the capacitance associated with the electrode and the dielectric constant of the medium, and is taken as a basis for the detection or measurement, c h a r a c t e r i z e d in that a conductor (11,21,31,- 61) between the electrode (10,20,30,40,60) and the oscillator circuit (15,25,35,65) is so short that the conductor (11,21,31,61) represents a substantially smaller capacitance than the capacitance of the electrode (10,20,30,60). 2. Apparatus according to claim 1, c h a r a c t e r i z e d in that an electrically screening encapsulation constitutes a counter-electrode (24,34,44,104) having a shape different from the shape of the electrode (20,30,40,100) and that the configuration of electrode and counter-electrode is adapted to be influenced by the medium (2,3,4) during measurement or detection in such position that it is located essentially displaced from the space directly between the electrode and the counter- electrode . 3. Apparatus according to claim 1 or 2, c h a r a c t e r i z e d in that the oscillator circuit (15) comprises a temperature sensing element (RT3) for temperature compensation of the oscillator circuit (15) . 4. Apparatus according to claim 3, c h a r a c t e r i z e d in that the oscillator circuit (15) is of the LC-oscillator type where there is included an air core coil (L5) and that the temperature sensing element (RT3) has a good thermal contact with the air core coil. 5. Apparatus according to claim 3 or 4 , c h a r a c t e r i z e d in that a first output (15F) from the oscillator circuit (15) is adapted to deliver the output frequency, that another output (15T) from the oscillator circuit is adapted to deliver a temperature measuring signal derived from the temperature sensing element (RT3) , that there is provided an analog-digital converter (18) receiving the temperature measuring signal and delivering a corresponding digital temperature signal, that the first output (15F) preferably via a frequency counter (19) is connected to an input (16F) of a microprocessor (16) adapted to compute and deliver a resulting detection or measurement signal (16U) , such as to an alarm, recording or display device, and that an input (16T) of the microprocessor further is adapted to receive the digital temperature signal for said temperature compensation in said calculation of the resulting detection or measurement signal. 6. Apparatus according to claim 1, 2, 3, 4 or 5 , intended for detection or measurement with respect to a medium, substance, material or object containing water, c h a r a c t e r i z e d in that the fundamental frequency of the oscillator circuit is within the range 10-100 MHz, preferably between 15 and 30 MHz. 7. Apparatus according to any one of claims 1-6, c h a r a c t e r i z e d in that it is frequency calibrated with air as an dielectric for the electrode, and besides preferably with water as a dielectric for the electrode. 8. Apparatus according to any one of claims 1-7, c h a r a c t e r i z e d in that the electrode (60) is formed at one side of a circuit board (69) and that the oscillator circuit (65) is located essentially on the other side of the circuit board (69) with said conductor (61) arranged therethrough. 9. Apparatus according to any one of claims 5-8, c h a r a c t e r i z e d in that the oscillator circuit (35,45,65) is adapted to be located in good thermal contact with said medium, substance, material or object (3,4,6), and that there is included means for digital compensation of the detection or measurement signal at the output of the microprocessor (16) , also with respect to temperature variation of the dielectric constant of the medium, based on said temperature measuring signal . 10. Apparatus according to any one of claims 1-9, in particular for measuring moisture in bulk goods or continuous materials, c h a r a c t e r i z e d in that the electrode (20) , the oscillator circuit (25) and possibly associated electronic circuits, such as for temperature compensation (27) , are located in a substantially closed, electrically conductive encapsulation (24) , where a window (22) in the encapsulation is formed of an electrically non-conductive material, and that the electrode is plate-shaped (20) and provided at the inside of the window (22) , whereas the outside of the window is adapted to face against the goods (2) or the like the moisture of which is to be measured. 11. Apparatus according to claim 10, c h a r a c t e r i z e d in that the window (22) has a thickness being of an order of magnitude that is comparable to the surface extent of the electrode (20) . 12. Apparatus according to any one of claims 1-9, in particular for measurements concerning a liquid or mass received in a measuring vessel (33) , c h a r a c t e r i z e d in that the electrode (30) is generally annular, but preferably circular, and adapted to enclose the measuring vessel (33) at the level of and at a given spacing from the liquid or mass (3) therein, that the measuring vessel (33) consists of an electrically non-conductive material, and that the electrode (30) at least laterally is sur- rounded by a screen (34) of electrically conductive material, having a distance from the electrode (30) being preferably larger than said given spacing. 13. Apparatus according to claim 12 , c h a r a c t e r i z e d in that the electrode (30) is provided as a ribbon externally of a cylinder (32) of electrically non-conductive material and with an internal cavity adapted to accommodate the measuring vessel (33) . 14. Apparatus according to any one of claims 1-7 or 9, in particular for measuring moisture in bulk goods, c h a r a c t e r i z e d in that the electrode (40) is rod- or thread-shaped and located preferably centrally along the axis of a pointed front part (42) of a spear-like tool, where the electrode (40) is substantially surrounded by electrically non-conductive materials, and that the oscillator circuit (45) and possible associated electronic circuits such as for temperature compensation (47) , are located in an axially adjacent part of the tool, preferably with a surrounding enclosure (44) of electrically conductive material, extending rearwardly from the region at the connection between the electrode and the oscillator circuit, to a rear end (43) of the tool. 15. Apparatus according to any one of claims 3-9, c h a r a c t e r i z e d in that a number of electrodes (50A-C, 711-718 , 801-807) are arranged in a row preferably vertically oriented, for measuring at least one liquid level, and that each electrode has its own oscillator circuits (55A-C, 85A-G) directly associated therewith. 16. Apparatus according to any one of claims 5-9 and 15, c h a r a c t e r i z e d in that the microprocessor (16) is adapted to provide for frequency calibration with respect to the individual electrodes with associated oscillator circuit, depending on whether the electrode concerned is fully immersed in a liquid or as a whole is located above the liquid level thereof. 17. Apparatus according to claim 15 or 16, c h a r a c t e r i z e d in that outputs from the oscillator circuits (15, 55A-C, 85A-G) for the electrodes (10,50A- C, 801-807) are connected to at least one selector circuit (13,51,52,91,92) for controlling the activation of the individual electrodes during a measuring procedure . 18. Apparatus according to claim 15, 16 or 17, c h a r a c t e r i z e d by comprising a tube (63A,63B) of electrically non-conductive material and so designed that the electrodes (60) with associated oscillator circuits (65) and possible associated electronic circuits, such as for temperature compensation (67) , are separated in a liquid- tight manner from the liquid (6) the level of which is to be measured, preferably by means of a planar partition (62) incorporated in the tube . 19. Apparatus according to claim 18, c h a r a c t e r i z e d in that the electrodes (60) lie substantially in engagement with one side of the partition (62) . 20. Apparatus according to claim 18 or 19, c h a r a c t e r i z e d in that the non-conductive tube (63A,63B) is surrounded by a tube (64) of electrically conductive material, such as steel. 21. Apparatus according to claim 15, 16 or 17, for measuring interface levels (7W, 7X, 7Y, 7Z) between different fluids (7A-D) in a tank, in particular for the separation of oil (7B) and water (7A) , c h a r a c t e r i z e d in that at least a number of electrodes (711-718,721,731) with associated oscillator circuits are arranged each in or on a separate carrier tube (71,72,73), and that the number of electrodes for each carrier tube is several times as high as the number of interface levels (7W,7X,7Y,7Z) to be measured. 22. Apparatus according to claim 15, 16 or 17, c h a r a c t e r i z e d in that the electrodes (801-807) are disposed internally in a preferably tubular housing (83) of electrically non- conductive material, that the electrodes are in the form of ribbons lying generally in parallel planes and that the liquid to be detected or the level of which is to be measured, is intended to contact the housing (83) externally. 23. Apparatus according to claim 15, 16 or 17, for detecting or measuring flowing fluids, c h a r a c t e r i z e d in that at least one electrode (100) is provided around the circumference of a pipe length (102) of electrically non-conductive material, through which the fluid flow passes, and that a portion of the pipe length (102) at either side of the electrode (100) with associated oscillator circuit (105) , is surrounded by an electrically conductive screen (104) disposed at a radial spacing outside the pipe length (102) .

Inventors: ENGEBRETSEN BJOERN, HALLERAKER JON MORTEN, ENGEBRETSEN, BJOERN, HALLERAKER, JON, MORTEN
Applicants: ENGEBRETSEN BJOERN, HALLERAKER JON MORTEN, SENTECH AS, ENGEBRETSEN, BJOERN, HALLERAKER, JON, MORTEN
Application year: 1998
Main classification: G01F23
IPC codes: G01F23, G01N27