Ohm's Law: Difference between revisions
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==Examples== | ==Examples== | ||
===Simple=== | |||
The most basic example of Ohm's Law in action involves a closed circuit with a single power source and a single Ohmic resistor. | |||
[[File:OhmsLawExample1.png]] | |||
= | For this example the power source will be 12 volts and the resistor will be 4 ohms. To solve for the current, simply plug in the given values to get <math>{\frac{12V}{4\Omega} = 3A}</math>, meaning that the current is 3 amperes. | ||
===Middling=== | ===Middling=== | ||
A slightly more complex example involves a closed circuit with a single power source and two Ohmic resistors in parallel. | |||
[[File:OhmsLawExample2.gif]] | |||
In this case, R<sub>1</sub> is given to be 2 ohms, R<sub>2</sub> is given to be 4 ohms, and I is given to be 3 amperes. The first step is to remember that the R in the Ohm's Law equation represents total resistance, not individual resistors. In this case (Ohmic resistors in parallel), <math>{\frac{1}{R_{Net}} = \frac{1}{R_{1}} + \frac{1}{R_{2}}}</math>, meaning that <math>R_{Net} = \frac{4}{3} \Omega</math> | |||
===Difficult=== | ===Difficult=== | ||
Revision as of 17:44, 5 December 2015
WIP -- Claimed by Max Trussell
Ohm's law is very famous equation discovered by Georg Ohm describing the proportional relationship between voltage and current through some conductor. Most commonly this equation is seen in the form of
, with I representing current in amperes, V representing electric potential in volts, and R the resistance in ohms.
The Main Idea
Stripped down to its most basic, Ohm's Law exists so that either the electric potential, current, or total resistance of some conductor may be found when two out of the three are known quantities. This is possible because of the simple, linear relationship between the three.
A Mathematical Model
While most often represented as [math]\displaystyle{ {I = \frac{|\Delta V|}{R}} }[/math], Ohm's Law may also be represented as [math]\displaystyle{ V = IR }[/math] or [math]\displaystyle{ {R = \frac{V}{I}} }[/math]. Noteworthy is the fact that Ohm's Law depends upon Ohmic resistance and near ideal conductors to be accurate. Fortunately, most simple circuits without capacitance or inductance fit this criteria as the wires offer minuscule resistance when compared to the various resistors in the circuit. Additionally at any given point in time, Ohm's Law applies to both alternating current and direct current. Also worth noting is that V does not necessarily represent the potential difference across a single source of electric potential (e.g. a battery) but rather the absolute value of the potential difference across an entire circuit.
A Computational Model
There are numerous programs to be found that simulate circuits via Ohm's Law, with many allowing for analysis beyond the standard scope of Ohm's Law. One such example is Phet's Circuit Construction Kit, a free, lightweight tool to create and analyze simple DC current circuits. Here is a video briefly describing its installation and use!
Examples
Simple
The most basic example of Ohm's Law in action involves a closed circuit with a single power source and a single Ohmic resistor.
For this example the power source will be 12 volts and the resistor will be 4 ohms. To solve for the current, simply plug in the given values to get [math]\displaystyle{ {\frac{12V}{4\Omega} = 3A} }[/math], meaning that the current is 3 amperes.
Middling
A slightly more complex example involves a closed circuit with a single power source and two Ohmic resistors in parallel.
In this case, R1 is given to be 2 ohms, R2 is given to be 4 ohms, and I is given to be 3 amperes. The first step is to remember that the R in the Ohm's Law equation represents total resistance, not individual resistors. In this case (Ohmic resistors in parallel), [math]\displaystyle{ {\frac{1}{R_{Net}} = \frac{1}{R_{1}} + \frac{1}{R_{2}}} }[/math], meaning that [math]\displaystyle{ R_{Net} = \frac{4}{3} \Omega }[/math]
Difficult
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