In mathematics, the imaginary part of a complex number $z$, is the second element of the ordered pair of real numbers representing $z,$ i.e. if $z\; =\; (x,\; y)$, or equivalently, $z\; =\; x+iy$, then the imaginary part of $z$ is $y$. It is denoted by $\backslash mbox\{Im\}\; \backslash \{\; z\; \backslash \}$ or $\backslash Im\; \backslash \{\; z\; \backslash \}$. The complex function which maps $z$ to the imaginary part of $z$ is not holomorphic.

In terms of the complex conjugate $\backslash bar\{z\}$, the imaginary part of z is equal to $\backslash frac\{z-\backslash bar\{z\}\}\{2i\}$.

For a complex number in polar form, $z\; =\; (r,\; \backslash theta\; )$, or equivalently, $z\; =\; r(cos\; \backslash theta\; +\; i\; \backslash sin\; \backslash theta)$, it follows from Euler's formula that $z\; =\; re^\{i\backslash theta\}$, and hence that the imaginary part of $re^\{i\backslash theta\}$ is $r\backslash sin\backslash theta$.

In electric power, when a sine wave voltage drives a "linear" load (in other words, a load that makes the current also be a sine wave), the current $I$ in the power wires can be represented as a complex number $I\; =\; x\; +\; jy$. (Engineers use "j" to indicate the imaginary unit rather than "i". To them, "i" represents current). The "real current" x is related to the current when the voltage is maximum. The real current times the voltage gives the actual power consumed by the load (often all that power is dissipated as heat). The "imaginary current" y is related to the current when the voltage is zero. A load with purely imaginary current (such as a capacitor or inductor) dissipates no power; it merely accepts power temporarily then later pushes that power back on the power lines.

See also

• Real part
• Imaginary number

Complex numbers

Vikipedio:Projekto matematiko/Imaginara parto | Parte immaginaria | Parte imaginária