Abstract: A high frequency inductive emf circuit charges storage capacitors, one at a time, from a DC source to a voltage that is higher than the DC output voltage. After each storage capacitor is charged, it is disconnected from the charging circuit and then connected to an output device/regulator that uses the energy in each storage capacitor to provide the desired DC output voltage to a load. While one storage capacitor is being charged, a previously charged storage capacitor is being discharged through an output device/regulator. After being discharged, each storage capacitor is disconnected from its output device/regulator and reconnected to the charging circuit and is charged again. While being charged, the storage capacitors are in a parallel circuit to the inductor in the charging circuit. The inductor in the charging circuit and the DC source are never in a current loop with the load.

Abstract: A high frequency inductive emf circuit charges storage capacitors, one at a time, from a DC source to a voltage that is higher than the DC output voltage. After each storage capacitor is charged, it is disconnected from the charging circuit and then connected to an output device/regulator that uses the energy in each storage capacitor to provide the desired DC output voltage to a load. While one storage capacitor is being charged, a previously charged storage capacitor is being discharged through an output device/regulator. After being discharged, each storage capacitor is disconnected from its output device/regulator and reconnected to the charging circuit and is charged again. While being charged, the storage capacitors are in a parallel circuit to the inductor in the charging circuit. The inductor in the charging circuit and the DC source are never in a current loop with the load.

Abstract: Practically ideal electrical resonance is employed to soley provide armature power, and stator power if desired, to run DC motors. A practically ideal parallel resonant tank circuit (PIPRC) is used wherein the quotient of the “tank current” divided by the “line current” (called the “quality” or “Q” of the tank) is (1) greater than one, (2) large enough to allow the percent efficiency of the electric motor to be equal to or greater than 95%, and (3) removes enough back emf or enough of the influence thereof so that criteria (1) and (2) can be realized throughout the entire operating range of the motor. Only one PIPRC is needed for a DC motor. Recontrolling and/or redesigning is done for two reasons.

Abstract: Practically ideal electrical resonance is employed to soley provide armature power, and stator power if desired, to run DC motors. A practically ideal parallel resonant tank circuit (PIPRC) is used wherein the quotient of the “tank current” divided by the “line current” (called the “quality” or “Q” of the tank) is (1) greater than one, (2) large enough to allow the percent efficiency of the electric motor to be equal to or greater than 95%, and (3) removes enough back emf or enough of the influence thereof so that criteria (1) and (2) can be realized throughout the entire operating range of the motor. Only one PIPRC is needed for a DC motor. Recontrolling and/or redesigning is done for two reasons.

Abstract: Practically ideal electrical resonance is employed to soley provide armature power, and stator power if desired, to run DC motors. A practically ideal parallel resonant tank circuit (PIPRC) is used wherein the quotient of the “tank current” divided by the “line current” (called the “quality” or “Q” of the tank) is (1) greater than one, (2) large enough to allow the percent efficiency of the electric motor to be equal to or greater than 95%, and (3) removes enough back emf or enough of the influence thereof so that criteria (1) and (2) can be realized throughout the entire operating range of the motor. Only one PIPRC is needed for a DC motor. Recontrolling and/or redesigning is done for two reasons.

Abstract: Practically ideal electrical resonance is employed to soley provide armature power, and stator power if desired, to run DC motors. A practically ideal parallel resonant tank circuit (PIPRC) is used wherein the quotient of the “tank current” divided by the “line current” (called the “quality” or “Q” of the tank) is (1) greater than one, (2) large enough to allow the percent efficiency of the electric motor to be equal to or greater than 95%, and (3) removes enough back emf or enough of the influence thereof so that criteria (1) and (2) can be realized throughout the entire operating range of the motor. Only one PIPRC is needed for a DC motor. Recontrolling and/or redesigning is done for two reasons.