Power (physics)

 ( Force ) 

Power is the amount of energy transferred or converted per unit time. In the International System of Units, the unit of power is the watt, equal to one joule per second. Power is a scalar quantity.

Specifying power in particular systems may require attention to other quantities; for example, the power involved in moving a ground vehicle is the product of the aerodynamic drag plus traction force on the wheels, and the velocity of the vehicle. The output power of a Engine is the product of the torque that the motor generates and the angular velocity of its output shaft. Likewise, the power dissipated in an electrical element of a circuit is the product of the electric current flowing through the element and of the voltage across the element.Chapter 13, § 3, pp 13-2,3 The Feynman Lectures on Physics Volume I, 1963

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Definition Power is the rate with respect to time at which work is done or, more generally, the rate of change of total mechanical energy. It is given by: $$P\; =\; \backslash frac\{dE\}\{dt\},$$ where is power, is the total mechanical energy (sum of kinetic and potential energy), and is time.

For cases where only work is considered, power is also expressed as: $$P\; =\; \backslash frac\{dW\}\{dt\},$$ where is the work done on the system. However, in systems where potential energy changes without explicit work being done (e.g., changing fields or conservative forces), the total energy definition is more general.

We will now show that the mechanical power generated by a force F on a body moving at the velocity v can be expressed as the product: $$P\; =\; \backslash frac\{dW\}\{dt\}\; =\; \backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\; \{v\}$$

If a constant force F is applied throughout a distance x, the work done is defined as $W\; =\; \backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\{x\}$. In this case, power can be written as: $$P\; =\; \backslash frac\{dW\}\{dt\}\; =\; \backslash frac\{d\}\{dt\}\; \backslash left(\backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\{x\}\backslash right)\; =\; \backslash mathbf\{F\}\backslash cdot\; \backslash frac\{d\backslash mathbf\{x\}\}\{dt\}\; =\; \backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\; \{v\}.$$

If instead the force is variable over a three-dimensional curve C, then the work is expressed in terms of the line integral: $$W\; =\; \backslash int\_C\; \backslash mathbf\{F\}\; \backslash cdot\; d\backslash mathbf\; \{r\}$$

 = \int_{\Delta t} \mathbf{F} \cdot \frac{d\mathbf {r}}{dt} \  dt
 = \int_{\Delta t} \mathbf{F} \cdot \mathbf {v} \, dt.
     

From the fundamental theorem of calculus, we know that $$P\; =\; \backslash frac\{dW\}\{dt\}\; =\; \backslash frac\{d\}\{dt\}\; \backslash int\_\{\backslash Delta\; t\}\; \backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\; \{v\}\; \backslash ,\; dt\; =\; \backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\; \{v\}.$$ Hence the formula is valid for any general situation.

In older works, power is sometimes called activity.

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Units The dimension of power is energy divided by time. In the International System of Units (SI), the unit of power is the watt (W), which is equal to one joule per second. Other common and traditional measures are horsepower (hp), comparing to the power of a horse; one mechanical horsepower equals about 745.7 watts. Other units of power include per second (erg/s), foot-pound force per minute, dBm, a logarithmic measure relative to a reference of 1 milliwatt, per hour, BTU per hour (BTU/h), and tons of refrigeration.

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Average power and instantaneous power As a simple example, burning one kilogram of coal releases more energy than detonating a kilogram of TNT,Burning coal produces around 15-30 per kilogram, while detonating TNT produces about 4.7 megajoules per kilogram. For the coal value, see For the TNT value, see the article TNT equivalent. Neither value includes the weight of oxygen from the air used during combustion. but because the TNT reaction releases energy more quickly, it delivers more power than the coal. If is the amount of mechanical work performed during a period of time of duration , the average power over that period is given by the formula $$P\_\backslash mathrm\{avg\}\; =\; \backslash frac\{\backslash Delta\; W\}\{\backslash Delta\; t\}.$$ It is the average amount of work done or energy converted per unit of time. Average power is often called "power" when the context makes it clear.

Instantaneous power is the limiting value of the average power as the time interval approaches zero. $$P\; =\; \backslash lim\_\{\backslash Delta\; t\; \backslash to\; 0\}\; P\_\backslash mathrm\{avg\}\; =\; \backslash lim\_\{\backslash Delta\; t\; \backslash to\; 0\}\; \backslash frac\{\backslash Delta\; W\}\{\backslash Delta\; t\}\; =\; \backslash frac\{dW\}\{dt\}.$$

When power is constant, the amount of work performed in time period can be calculated as $$W\; =\; Pt.$$

In the context of energy conversion, it is more customary to use the symbol rather than .

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Mechanical power Power in mechanical systems is the combination of forces and movement. In particular, power is the product of a force on an object and the object's velocity, or the product of a torque on a shaft and the shaft's angular velocity.

Mechanical power is also described as the time derivative of work. In mechanics, the mechanical work done by a force on an object that travels along a curve is given by the line integral: $$W\_C\; =\; \backslash int\_C\; \backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\{v\}\; \backslash ,\; dt\; =\; \backslash int\_C\; \backslash mathbf\{F\}\; \backslash cdot\; d\backslash mathbf\{x\},$$ where defines the path and is the velocity along this path.

If the force is derivable from a potential (conservative), then applying the gradient theorem (and remembering that force is the negative of the gradient of the potential energy) yields: $$W\_C\; =\; U(A)\; -\; U(B),$$ where and are the beginning and end of the path along which the work was done.

The power at any point along the curve is the time derivative: $$P(t)\; =\; \backslash frac\{dW\}\{dt\}\; =\; \backslash mathbf\{F\}\; \backslash cdot\; \backslash mathbf\{v\}\; =\; -\backslash frac\{dU\}\{dt\}.$$

In one dimension, this can be simplified to: $$P(t)\; =\; F\; \backslash cdot\; v.$$

In rotational systems, power is the product of the torque and angular velocity , $$P(t)\; =\; \backslash boldsymbol\{\backslash tau\}\; \backslash cdot\; \backslash boldsymbol\{\backslash omega\},$$ where is angular frequency, measured in radians per second. The $\backslash cdot$ represents scalar product.

In fluid power systems such as hydraulic actuators, power is given by $$P(t)\; =\; pQ,$$ where is pressure in pascals or N/m², and is volumetric flow rate in m³/s in SI units.

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Mechanical advantage If a mechanical system has no losses, then the input power must equal the output power. This provides a simple formula for the mechanical advantage of the system.

Let the input power to a device be a force acting on a point that moves with velocity and the output power be a force acts on a point that moves with velocity . If there are no losses in the system, then $$P\; =\; F\_\backslash text\{B\}\; v\_\backslash text\{B\}\; =\; F\_\backslash text\{A\}\; v\_\backslash text\{A\},$$ and the mechanical advantage of the system (output force per input force) is given by $$\backslash mathrm\{MA\}\; =\; \backslash frac\{F\_\backslash text\{B\}\}\{F\_\backslash text\{A\}\}\; =\; \backslash frac\{v\_\backslash text\{A\}\}\{v\_\backslash text\{B\}\}.$$

The similar relationship is obtained for rotating systems, where and are the torque and angular velocity of the input and and are the torque and angular velocity of the output. If there are no losses in the system, then $$P\; =\; T\_\backslash text\{A\}\; \backslash omega\_\backslash text\{A\}\; =\; T\_\backslash text\{B\}\; \backslash omega\_\backslash text\{B\},$$ which yields the mechanical advantage $$\backslash mathrm\{MA\}\; =\; \backslash frac\{T\_\backslash text\{B\}\}\{T\_\backslash text\{A\}\}\; =\; \backslash frac\{\backslash omega\_\backslash text\{A\}\}\{\backslash omega\_\backslash text\{B\}\}.$$

These relations are important because they define the maximum performance of a device in terms of determined by its physical dimensions. See for example .

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Electrical power The instantaneous electrical power P delivered to a component is given by $$P(t)\; =\; I(t)\; \backslash cdot\; V(t),$$ where

• $P(t)$ is the instantaneous power, measured in ( per second),
• $V(t)$ is the voltage (or voltage drop) across the component, measured in , and
• $I(t)$ is the Electric current through it, measured in .

If the component is a resistor with time-invariant voltage to electric current ratio, then: $$P\; =\; I\; \backslash cdot\; V\; =\; I^2\; \backslash cdot\; R\; =\; \backslash frac\{V^2\}\{R\},$$ where $$R\; =\; \backslash frac\{V\}\{I\}$$ is the electrical resistance, measured in .

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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 function of period $T$. The peak power is simply defined by: $$P\_0\; =\; \backslash max\; p(t).$$

The peak power is not always readily measurable, however, and the measurement of the average power $P\_\backslash mathrm\{avg\}$ is more commonly performed by an instrument. If one defines the energy per pulse as $$\backslash varepsilon\_\backslash mathrm\{pulse\}\; =\; \backslash int\_0^T\; p(t)\; \backslash ,\; dt$$ then the average power is $$P\_\backslash mathrm\{avg\}\; =\; \backslash frac\{1\}\{T\}\; \backslash int\_0^T\; p(t)\; \backslash ,\; dt\; =\; \backslash frac\{\backslash varepsilon\_\backslash mathrm\{pulse\}\}\{T\}.$$

One may define the pulse length $\backslash tau$ such that $P\_0\backslash tau\; =\; \backslash varepsilon\_\backslash mathrm\{pulse\}$ so that the ratios $$\backslash frac\{P\_\backslash mathrm\{avg\}\}\{P\_0\}\; =\; \backslash frac\{\backslash tau\}\{T\}$$ are equal. These ratios are called the duty cycle of the pulse train.

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Radiant power Power is related to intensity at a radius $r$; the power emitted by a source can be written as: $$P(r)\; =\; I(4\backslash pi\; r^2).$$

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See also

• Simple machines
• Orders of magnitude (power)
• Pulsed power
• Intensity – in the radiative sense, power per area
• Power gain – for linear, two-port networks
• Power density
• Signal strength
• Sound power

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