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Welcome to our Physics lesson on Ohm's Law for the Whole Circuit, this is the fourth lesson of our suite of physics lessons covering the topic of Electric Potential Difference (Voltage). Ohm's Law, you can find links to the other lessons within this tutorial and access additional physics learning resources below this lesson.
The battery has its own internal resistance, which we denote as r. We can draw this conclusion when we touch a battery immediately after it has been operating. We can feel the hotness of battery, which indicates the conversion of electricity into heat inside the battery.
In addition, from the previous tutorial, we know that a conductor has its own internal resistance, which depends from the type of material, length and thickness of conductor. This causes a drop in the potential difference at the resistor. Look at the figure below.
We can write for the relationship between potential differences and the electromotive force in the above circuit:
If we write the total resistance of the circuit by Rtot, we obtain (applying Ohm's Law):
Given that RABCD = Rwire, we obtain
or
The above equation gives Ohm's Law for the whole circuit. We can write it in a shorter way as
A 20 m long copper wire of 4 mm2 thickness (ρ = 1.69 × 10-8 Ω ∙ m) is used to build an electrical circuit that contains a 24 V battery and a resistor. The battery has a 0.6 Ω internal resistance. What is the resistance of the resistor if the current flowing through the circuit is equal to 12A? Use the figure shown in the theory as a reference.
Clues:
L = 20 m
A = 4 mm2 = 4 × 10-6 m2
emf = 24 V
r = 0.6 Ω
I = 12 A
R = ?
First, we find the resistance of wire. We have
Applying Ohm's Law for the whole circuit, we obtain
Thus,
You have reached the end of Physics lesson 15.3.4 Ohm's Law for the Whole Circuit. There are 4 lessons in this physics tutorial covering Electric Potential Difference (Voltage). Ohm's Law, you can access all the lessons from this tutorial below.
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