A source of this quantity is required in the statement of Norton's theorem, whereas it s not required in Thevenin's theorem. Magnetic field equals mu-nought over 4pi times the path integral of dl cross r-hat times this quantity over magnitude of r squared, according to the Biot-Savart law. A term was added to Ampere's Law to account for the "displacement" type of this quantity. The voltage drop across an inductor equals inductance times the time-derivative of this quantity, and the power supplied to a component is equal to this quantity squared times resistance. For 10
A source of this quantity is required in the statement of Norton's theorem, whereas it s not required in Thevenin's theorem. Magnetic field equals mu-nought over 4pi times the path integral of dl cross r-hat times this quantity over magnitude of r squared, according to the Biot-Savart law. A term was added to Ampere's Law to account for the "displacement" type of this quantity. The voltage drop across an inductor equals inductance times the time-derivative of this quantity, and the power supplied to a component is equal to this quantity squared times resistance. For 10 points, give this quantity measured in amps, which by Ohm's Law equals voltage divided by resistance.
A source of this quantity is required in the statement of Norton's theorem, whereas it s not required in Thevenin's theorem.
electric current