ELECTRONIC PRINCIPLES - OD1647 - LESSON 1/TASK 1
overcoming the emf of selfinduction, which is at maximum
because the rate of change of current is maximum. Thus the
battery voltage is equal to the drop across the inductor, and
the voltage across the resistor is zero. As time goes on, more
of the battery voltage appears across the resistor and less
across the inductor. The rate of change of current is
approached, the drop across the inductor approaches zero, and
all of the battery voltage is used to overcome the resistance of
the circuit.
Thus, the voltages across the inductor and the resistor change
in magnitude during the period of growth of current in the same
way the force applied to the boat divides itself between the
inertia and friction effects. The force is developed first.
across the inertia/inductive effect and finally across the
friction/resistive effect.
When switch S2 is closed (source voltage Es removed from the
circuit), the flux that has been established around the inductor
(L) is essentially equal to Es in magnitude. The induced voltage
causes decay current (id ) to flow in resistor R in the same
direction in which current was flowing originally (when S1 was
closed). A voltage (eR) that is initially equal to source
voltage (Es) is developed across I. The voltage across the
resistor (eR) rapidly falls to zero as the voltage across the
inductor (eL) falls to zero due to the collapsing flux.
Just as the example of the boat was used to explain the growth
of current in a circuit, it can also be used to explain the
decay of current in a circuit. When the force applied to the
boat is removed, the boat. continues to move through the water
before eventually coming to a stop. This is because energy was
being stored in the inertia of the moving boat. After a period
of time, the friction of the water overcomes the inertia of the
boat and the boat stops moving. Just as inertia of the boat
Because of this, even when the power source is removed, the
stored energy of the magnetic field of the inductor tends to
collapses.
(1) L/R Time Constant. The L/R TIME CONSTANT is a variable
tool for use in determining the time required for current in an
inductor to reach a
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