Ohm's Law — Core Principles
Core Principles
Ohm's Law is a foundational principle in electricity, stating that the current () flowing through a conductor is directly proportional to the potential difference () across its ends, provided physical conditions like temperature remain constant.
This relationship is expressed as , where is the constant of proportionality known as resistance. Voltage (V) is the 'electrical push,' current (A) is the 'flow rate of charge,' and resistance () is the 'opposition to flow.
' Materials that obey this law are called Ohmic conductors, exhibiting a linear V-I graph. The resistance of a conductor depends on its material's resistivity (), length (), and cross-sectional area () via .
Resistivity is an intrinsic property, while resistance is specific to a component. Temperature significantly affects resistance; for metals, resistance generally increases with temperature. Ohm's Law is crucial for basic circuit analysis but has limitations, particularly with non-Ohmic materials like semiconductors.
Important Differences
vs Non-Ohmic Conductors
| Aspect | This Topic | Non-Ohmic Conductors |
|---|---|---|
| Definition | Ohmic Conductors are materials that strictly obey Ohm's Law. | Non-Ohmic Conductors are materials that do not obey Ohm's Law. |
| V-I Characteristic | Exhibit a linear V-I graph, passing through the origin. The slope ($V/I$) is constant. | Exhibit a non-linear V-I graph. The slope ($V/I$) is not constant and varies with voltage/current. |
| Resistance (R) | Resistance is constant and independent of the applied voltage or current (assuming constant temperature). | Resistance is not constant; it changes with the applied voltage, current, or even the direction of current. |
| Examples | Most metallic conductors (e.g., copper, aluminum, nichrome) at constant temperature. | Semiconductor devices (e.g., diodes, transistors), electrolytes, vacuum tubes, gas discharge tubes. |
| Microscopic Behavior | Drift velocity is directly proportional to the electric field. | Drift velocity is not directly proportional to the electric field, or charge carrier concentration changes with applied field. |