There are, however, components of electrical circuits which do not obey Ohm's law; that is, their relationship between current and voltage (their "I"–"V" curve) is "nonlinear" (or non-ohmic). An example is the p–n junction diode (curve at right). As seen in the figure, the current does not increase linearly with applied voltage for a diode. One can determine a value of current ("I") for a given value of applied voltage ("V") from the curve, but not from Ohm's law, since the value of "resistance" is not constant as a function of applied voltage. Further, the current only increases significantly if the applied voltage is positive, not negative. The ratio "V"/"I" for some point along the nonlinear curve is sometimes called the "static", or "chordal", or DC, resistance, but as seen in the figure the value of total "V" over total "I" varies depending on the particular point along the nonlinear curve which is chosen. This means the "DC resistance" V/I at some point on the curve is not the same as what would be determined by applying an AC signal having peak amplitude Δ"V" volts or Δ"I" amps centered at that same point along the curve and measuring Δ"V"/Δ"I". However, in some diode applications, the AC signal applied to the device is small and it is possible to analyze the circuit in terms of the "dynamic", "small-signal", or "incremental" resistance, defined as the one over the slope of the "V"–"I" curve at the average value (DC operating point) of the voltage (that is, one over the derivative of current with respect to voltage). For sufficiently small signals, the dynamic resistance allows the Ohm's law small signal resistance to be calculated as approximately one over the slope of a line drawn tangentially to the "V"–"I" curve at the DC operating point.