Wednesday 11 February 2009

A Problem With Ammeters and Measurement of dØ/dt

A Problem With Ammeters and Measurement of dØ/dt
Note that an ammeter cannot differentiate between displacement current dØ/dt and normal current dq/dt. In the ammeter, the sample
dØ/dt will couple to free electrons, producing a normal dq/dt inside the ammeter. The driving of this dq/dt through a precision
resistance, e.g., is measured and the instrument is calibrated to show the dq/dt amperes flowing. One of the major needs of free energy
researchers is the development of a good current meter that will differentiate between dØ/dt and dq/dt, and measure each one. Short
of using a mass spectrometer to differentiate the mass current dm/dt, and comparison of those mass current measurements with an
ammeter's measurements of the "current" dq/dt, and calculating the dØ/dt from that, I presently know of no way to precisely and
simply measure and separate the two current components. I have been thinking of utilizing a multi-channel sampling meter set
arrangement, where one channel uses a dm/dt blocking device such as the Fogal semiconductor in this respect, but have not yet
developed the complete concept.
Better Solution: A Charge Blocking Device
A better solution than the capacitor or capacitive collector is the use of a special rigid solid state "charge blocking device", such as a
Fogal semiconductor, to enable the current separation into two components, blocking of the mass flow component, and passage of the
massless displacement current component. In overunity electrical devices, it is massless displacement current dØ/dt that must be
separately passed down the primary circuit and collected in the collector as an E-field or an H-field. This provides "free" energy that
has been extracted from the vacuum, via the potential difference between the terminals of the source antenna, and collected and
stored in the appropriate field, without work. The collected free energy may then be transferred to the isolated load circuit by a variety
of means, for separate discharge through the load without return of dq/dt through the source.

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