Mechanical Power (physics)

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 motor 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 current flowing through the element and of the voltage across the element.

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:
$P = \frac,$
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:
$P = \frac,$
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: $P = \frac = \mathbf \cdot \mathbf$

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

If instead the force is ''variable over a three-dimensional curve C'', then the work is expressed in terms of the line integral:
$W = \int_C \mathbf \cdot d\mathbf = \int_ \mathbf \cdot \frac \ dt = \int_ \mathbf \cdot \mathbf \, dt.$

From the fundamental theorem of calculus, we know that $P = \frac = \frac \int_ \mathbf \cdot \mathbf \, dt = \mathbf \cdot \mathbf .$ Hence the formula is valid for any general situation.

In older works, power is sometimes called ''activity''.

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 ergs per second (erg/s), foot-pounds per minute, dBm, a logarithmic measure relative to a reference of 1 milliwatt, calories per hour, BTU per hour (BTU/h), and tons of refrigeration.

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 megajoules 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 work performed during a period of time of duration , the average power over that period is given by the formula
$P_\mathrm = \frac.$
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.
$P = \lim_ P_\mathrm = \lim_ \frac = \frac.$

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 .

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 work done by a force on an object that travels along a curve is given by the line integral:
$W_C = \int_C \mathbf \cdot \mathbf \, dt = \int_C \mathbf \cdot d\mathbf,$
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:
$P(t) = \frac = \mathbf \cdot \mathbf = -\frac.$

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

In rotational systems, power is the product of the torque and angular velocity ,
$P(t) = \boldsymbol \cdot \boldsymbol,$
where is angular frequency, measured in radians per second. The $\cdot$ 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.

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
$P = F_\text v_\text = F_\text v_\text,$
and the mechanical advantage of the system (output force per input force) is given by
$\mathrm = \frac = \frac.$

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
$P = T_\text \omega_\text = T_\text \omega_\text,$
which yields the mechanical advantage
$\mathrm = \frac = \frac.$

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

Electrical power

The instantaneous electrical power ''P'' delivered to a component is given by
$P(t) = I(t) \cdot V(t),$
where
*$P(t)$ is the instantaneous power, measured in watts (joules per second),
*$V(t)$ is the potential difference (or voltage drop) across the component, measured in volts, and
*$I(t)$ is the current through it, measured in amperes.

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

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 = \max (t)

The peak power is not always readily measurable, however, and the measurement of the average power $P_\mathrm$ is more commonly performed by an instrument. If one defines the energy per pulse as
$\varepsilon_\mathrm = \int_0^T p(t) \, dt$
then the average power is
$P_\mathrm = \frac \int_0^T p(t) \, dt = \frac.$

One may define the pulse length $\tau$ such that $P_0\tau = \varepsilon_\mathrm$ so that the ratios
$\frac = \frac$
are equal. These ratios are called the ''duty cycle'' of the pulse train.

Radiant power

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

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

References

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Force
Temporal rates
Physical quantities