Electrical power

The physical quantity power (symbol from English power , unit watt , unit symbol  W) is the energy converted in a period of time based on this period of time. It is referred to as electrical power if the energy drawn or supplied is electrical energy . ${\displaystyle P}$

Connection with other quantities

With direct current

the actual electrical power is the product of the electrical voltage and the electrical current ${\displaystyle P}$  ${\displaystyle U}$  ${\displaystyle I}$

${\displaystyle P=U\cdot I}$

Behaves consumers as ohmic resistance , the power can be by application of Ohm's law by express ${\displaystyle R}$ ${\displaystyle U=R\cdot I}$

${\displaystyle P=I^{2}\cdot R\quad {\text{bzw.}}\quad P={\frac {U^{2}}{R}}}$

With alternating current

the quantities voltage and current are time- dependent quantities and . A distinction must be made between several service terms: ${\displaystyle t}$ ${\displaystyle u}$ ${\displaystyle i}$

• Instantaneous value of the performance or also instantaneous performance ${\displaystyle p}$

${\displaystyle p=u\cdot i}$

• Active power , the energy actually converted per time period. It is given in watts (unit symbol W). ${\displaystyle P}$
• Apparent power , also known as connected load or connected load. It is given in volt-amperes (symbol VA). ${\displaystyle S}$
• Reactive power , which is generally undesirable and unusable energy per time. It is specified in Var (unit symbol var). ${\displaystyle Q}$

If and are sinusoidal alternating quantities and of the same frequency, then it is also sinusoidal, but with twice the frequency and a constant component . The sizes are defined by averaging; for them there are no instantaneous values. ${\displaystyle u}$ ${\displaystyle i}$ ${\displaystyle p}$ ${\displaystyle S,\;P{\text{ und }}Q}$

The real power is the arithmetic mean (if the quantity is continuously available the equivalent ) of the instantaneous power:

Instantaneous power values with a sinusoidal curve The power actually consumed (curve 1) can be viewed as a superposition of a component that contributes to active power (curve 3) and a component that contributes to reactive power (curve 2) ${\displaystyle p(t)}$

${\displaystyle P={\overline {p}}={\frac {1}{T}}\int \limits _{t_{0}}^{t_{0}+T}u\cdot i\ \mathrm {d} t}$

In the case of periodic processes, the period duration or, for statistical processes, a sufficiently long time (mathematically strict:)   . ${\displaystyle T}$ ${\displaystyle \lim \;T\to \infty }$

The apparent power is formed from the effective values and , these are the root mean square values of voltage and current, ${\displaystyle U}$ ${\displaystyle I}$

${\displaystyle S=U\cdot I={\sqrt {\,{\overline {u^{2}}}\,}}\cdot {\sqrt {\,{\overline {i^{2}}}\,}}}$

The apparent power is greater than the real power in the case of consumers with impressed voltage in the current

• a phase shift or
• a distortion (additional harmonics )

cause. The difference is made by the total reactive power

${\displaystyle Q_{\mathrm {tot} }={\sqrt {S^{2}-P^{2}}}}$

specified.

Measuring circuits and associated power meter are in active power and reactive power explained. Apparatus measuring devices for apparent power are not common. However, there are multifunctional transmitters that are also designed for this.

According to the definition above, there is no rms value of the power . The " RMS power " is a formal quantity in audio technology, but has nothing to do with the physical quantity "power". ${\displaystyle {\sqrt {\,{\overline {p^{2}}}\,}}}$

Maximum power output

The maximum power that an electrical energy source can transfer to a consumer is achieved with power adjustment. However, 50% of the power is lost in the source. Power supply devices and generators therefore usually do not work with power adjustment, but with voltage adjustment . Power adjustment is sometimes used for the transmission of information, since a signal source often only has a small amount of electrical power available.

Performance as a device identifier

To identify the output of a device ( electrical consumer , energy converter ), the nominal output is used, which can differ considerably from the actual output. It is specified like an active power.

What is important here is the type of power indicated on the nameplate. For motors, the available mechanical power is given, for lamps, vacuum cleaners or loudspeakers, on the other hand, the electrical power consumed. In the case of generators , such as bicycle dynamos or alternators , the electrical power output is indicated.

The power ratings of audio amplifiers or loudspeakers are difficult to interpret . In the case of audio amplifiers, the sinusoidal output , music output , RMS output or peak output ( PMPO ) is often given. The values ​​differ considerably, often have little practical relevance and generally prevent comparability.

In the case of tweeter or woofer speakers, the power rating often refers to the music performance of the entire frequency range - they never endure this electrical power in continuous operation.

Net power

The terms gross power and net power are also used for technical systems for power generation . The gross power is the total nominal power of the generators; the net power is the gross power reduced by the sum of the power consumed by the auxiliary units ( internal requirements ) and the power losses due to transformation when feeding into the grid. The net output therefore indicates the electrical output of the power plant made available to the power grid . ${\displaystyle P_{\text{brutto}}}$ ${\displaystyle P_{\text{netto}}}$

See also

• Order of magnitude (performance) (exemplary performance values)
• Continuous output
• Installed capacity
• Power dissipation
• Electric power of a solar module
• Complex power

literature

• Klaus Tkotz: Electrical engineering . 25th edition, Verlag - Europa - Lehrmittel , 2006, ISBN 978-3808531594 .
• Ernst Hörnemann, Heinrich Hübscher: Electrical engineering specialist training in industrial electronics . 1 edition, Westermann Schulbuchverlag GmbH, Braunschweig 1998, ISBN 3-14-221730-4 .
• Wolfgang Bieneck: Elektro T basics of electrical engineering . 5th edition, Holland + Josenhans Verlag, Stuttgart 2005, ISBN 3-7782-4900-2 .
• Vance Dickason: Loudspeaker construction . 4th edition, Elektor-Verlag, Aachen 2007, ISBN 978-3-89576-116-4 .
• Berndt Stark: Loudspeaker manual . 7th edition, Richard Pflaum Verlag GmbH & Co.KG, Munich 1999, ISBN 3-7905-0807-1 .

Individual evidence

1. ^ DKE German Commission for Electrical, Electronic and Information Technologies: net output (of a power plant). In: E-Energy Glossary. August 7, 2011, accessed January 2, 2018 .