====== Non-linear resistors ====== All resistors examined so far are linear resistors, for which the characteristic $I = f(U)$ is a straight line; see . The resistance of a linear resistor is independent of the current $I$ flowing through it and of the applied voltage $U$. {{drawio>lab_electrical_engineering:1_resistors:Fig-6_Linear-resistors_V1.svg}}\\ \\ For non-linear resistors, there is no proportionality between current and voltage. The characteristic of such a resistor is shown in . For these resistors, one distinguishes between static resistance $R$ and dynamic (or differential) resistance $r$. The static resistance is determined for a specific operating point: at a given voltage, the current is read from the characteristic. The calculation is carried out according to Ohm's law: $R = \frac{U}{I}$ The dynamic resistance around the operating point is calculated from the current difference caused by a change in the applied voltage: $r = \frac{\Delta U}{\Delta I}$ {{drawio>lab_electrical_engineering:1_resistors:Fig-7_Nonlinear-resistors_V1.svg}}\\ An incandescent lamp is investigated as an example of a non-linear resistor. Build the measurement circuit shown in . \\ {{drawio>lab_electrical_engineering:1_resistors:Fig-8_light-bulb_V1.svg}}\\ \\ Set the voltage on the power supply to the voltage values from . Measure the corresponding current values and enter them in . {{drawio>lab_electrical_engineering:1_resistors:Table-6_light-bulb_V1.svg}}\\ \\ Plot the characteristic $I = f(U)$. \\ \\ \\ \\ \\ \\ Calculate the static resistance $R$ at the operating point $U = 7.0 ~{\rm V}$. \\ \\ \\ \\ Calculate the dynamic resistance $r$ at the operating point $U = 7.0 ~{\rm V}$. \\ \\ \\ \\ Compare the values with those from the direct resistance measurement (). \\ \\ \\ \\