encyclopedia

Categories: Power

Power (physics)

Contents

1 Mechanical power

1.1 SI unit
1.2 Non-SI units

2 Electrical power

2.1 Instantaneous electrical power
2.2 Average electrical power for sinusoidal voltages
2.3 Electrical power transfer
2.4 Peak power and duty cycle

3 Power in optics

4 See also

5 External links

Mechanical power

In physics, power (symbol: P) is the amount of work W done per unit of time t. This can be modeled as an energy flow, equivalent to the rate of change of the energy in a system, or the time rate of doing work, as defined by

$P=\frac{dE}{dt}$

where

P is power

E is energy or work W

t is time

The units of power are therefore energy divided by time.

SI unit

The SI unit of power is the watt, which is equal to one joule per second.

The power consumption of a human is on average roughly 100 watts, ranging from 85 W during sleep to 800 W or more while playing a strenuous sport. Professional cyclists have been measured at 2000 W output for short periods of time.

Non-SI units

Non-SI units of power include horsepower (HP), Pferdestärke (PS), cheval vapeur (CV) and foot-pounds per minute. One unit of horsepower is equivalent to 33,000 foot-pounds per minute, or the power required to lift 550 pounds one foot in one second, and is equivalent to about 746 watts. Other units include: dBm, logarithmic measure with 1 milliwatt as reference; kilocalorie per hour (often referred to as Calories per hour)

Electrical power

Main article: Electric power

Instantaneous electrical power

The instantaneous electrical power P delivered to a component is defined as:

$P = I \cdot V \,\!$

where

P is the instanteous power, measured in watts

V is the potential difference (or voltage drop) across the component, measured in volts

I is the current flowing through it, measured in amperes

If the component is a resistor, then:

$P=I^2 \cdot R \,\!$

$P=\frac{V^2}{R}$

where

R is the resistance, measured in ohms

Average electrical power for sinusoidal voltages

The average power consumed by a two-terminal electrical device is a function of the root mean square values of the sinusoidal voltage across the terminals and the sinusoidal current passing through the device. That is,

$P=I \cdot U \cdot \cos\phi \,\!$

where

P is the power, measured in watts

I is the root mean square value of the sinusoidal alternating current (AC), measured in amperes

U is the root mean square value of the sinusoidal alternating voltage, measured in volts

φ is the phase angle between the voltage and the current sine functions.

The amplitudes of sinusoidal voltages and currents, such as those used almost universally in mains electrical supplies, are normally specified in terms of root mean square values. This makes the above calculation a simple matter of multiplying the two stated numbers together.

This figure can also be called the effective power, as compared to the larger apparent power which is expressed in volt-amperes reactive (VAR) and does not include the $cosφ$ term due to the current and voltage being out of phase. For simple domestic appliances or a purely resistive network, the "cos φ" term (called the power factor) can often be assumed to be unity, and can therefore be omitted from the equation. In this case, the effective and apparent power are assumed to be equal.

Electrical power transfer

The efficient transfer of electrical power is governed by the maximum power theorem, which states that for the transfer of maximum power from a source with a fixed internal resistance to a load, the resistance of the load must be equal to that of the source.

Peak power and duty cycle

In the case of a periodic signal $s (t)$ of period $T$ , like a train of identical pulses, the instantaneous power $p (t) = | s (t) | 2$ is also a periodic funtion of period $T$ . The peak power is simply defined by:

P 0 = max p (t)

The peak power is not always readily measurable, however, and the measurement of the average power $P a v g$ is more commonly performed by an instrument. If one defines the energy per pulse as:

$\epsilon_{pulse} = \int_{0}^{T}p(t) dt$

then the average power is:

$P_{avg} = \frac{1}{T} \int_{0}^{T}p(t) dt = \frac{\epsilon_{pulse}}{T}$

One may define the pulse length $τ$ such that $P 0 τ = ε p u l s e$ so that the ratios

$\frac{P_{avg}}{P_0} = \frac{\tau}{T}$

are equal. These ratios are called the duty cycle of the pulse train.

Power in optics

In optics, the term power is also used to express the ability of a lens or other optical device to focus light. It is measured in dioptres (inverse metres).

External links

Categories: Power

The contents of this article are licensed from Wikipedia.org under the GNU Free Documentation License.
How to see transparent copy

01-04-2007 01:21:04

| | | |