Power in electric circuits
In addition to voltage and current, there is another measure of
free electron activity in a circuit: power. First, we need to
understand just what power is before we analyze it in any circuits.
Power is a measure of how much work can be performed in a given
amount of time. Work is generally defined in terms of the
lifting of a weight against the pull of gravity. The heavier the
weight and/or the higher it is lifted, the more work has been done.
Power is a measure of how rapidly a standard amount of work
is done.
For American automobiles, engine power is rated in a unit called
"horsepower," invented initially as a way for steam engine
manufacturers to quantify the working ability of their machines in
terms of the most common power source of their day: horses. One
horsepower is defined in British units as 550 ft-lbs of work per
second of time. The power of a car's engine won't indicate how tall
of a hill it can climb or how much weight it can tow, but it will
indicate how fast it can climb a specific hill or tow a
specific weight.
The power of a mechanical engine is a function of both the
engine's speed and it's torque provided at the output shaft. Speed
of an engine's output shaft is measured in revolutions per minute,
or RPM. Torque is the amount of twisting force produced by the
engine, and it is usually measured in pound-feet, or lb-ft (not to
be confused with foot-pounds or ft-lbs, which is the unit for work).
Neither speed nor torque alone is a measure of an engine's power.
A 100 horsepower diesel tractor engine will turn relatively
slowly, but provide great amounts of torque. A 100 horsepower
motorcycle engine will turn very fast, but provide relatively little
torque. Both will produce 100 horsepower, but at different speeds
and different torques. The equation for shaft horsepower is simple:
Notice how there are only two variable terms on the right-hand
side of the equation, S and T. All the other terms on that side are
constant: 2, pi, and 33,000 are all constants (they do not change in
value). The horsepower varies only with changes in speed and torque,
nothing else. We can re-write the equation to show this
relationship:
Because the unit of the "horsepower" doesn't coincide exactly
with speed in revolutions per minute multiplied by torque in
pound-feet, we can't say that horsepower equals ST. However,
they are proportional to one another. As the mathematical
product of ST changes, the value for horsepower will change by the
same proportion.
In electric circuits, power is a function of both voltage and
current. Not surprisingly, this relationship bears striking
resemblance to the "proportional" horsepower formula above:
In this case, however, power (P) is exactly equal to current (I)
multiplied by voltage (E), rather than merely being proportional to
IE. When using this formula, the unit of measurement for power is
the watt, abbreviated with the letter "W."
It must be understood that neither voltage nor current by
themselves constitute power. Rather, power is the combination of
both voltage and current in a circuit. Remember that voltage
is the specific work (or potential energy) per unit charge, while
current is the rate at which electric charges move through a
conductor. Voltage (specific work) is analogous to the work done in
lifting a weight against the pull of gravity. Current (rate) is
analogous to the speed at which that weight is lifted. Together as a
product (multiplication), voltage (work) and current (rate)
constitute power.
Just as in the case of the diesel tractor engine and the
motorcycle engine, a circuit with high voltage and low current may
be dissipating the same amount of power as a circuit with low
voltage and high current. Neither the amount of voltage alone nor
the amount of current alone indicates the amount of power in an
electric circuit.
In an open circuit, where voltage is present between the
terminals of the source and there is zero current, there is zero
power dissipated, no matter how great that voltage may be. Since
P=IE and I=0 and anything multiplied by zero is zero, the power
dissipated in any open circuit must be zero. Likewise, if we were to
have a short circuit constructed of a loop of superconducting wire
(absolutely zero resistance), we could have a condition of current
in the loop with zero voltage, and likewise no power would be
dissipated. Since P=IE and E=0 and anything multiplied by zero is
zero, the power dissipated in a superconducting loop must be zero.
(We'll be exploring the topic of superconductivity in a later
chapter).
Whether we measure power in the unit of "horsepower" or the unit
of "watt," we're still talking about the same thing: how much work
can be done in a given amount of time. The two units are not
numerically equal, but they express the same kind of thing. In fact,
European automobile manufacturers typically advertise their engine
power in terms of kilowatts (kW), or thousands of watts, instead of
horsepower! These two units of power are related to each other by a
simple conversion formula:
So, our 100 horsepower diesel and motorcycle engines could also
be rated as "74570 watt" engines, or more properly, as "74.57
kilowatt" engines. In European engineering specifications, this
rating would be the norm rather than the exception.
- REVIEW:
- Power is the measure of how much work can be done in a given
amount of time.
- Mechanical power is commonly measured (in America) in
"horsepower."
- Electrical power is almost always measured in "watts," and it
can be calculated by the formula P = IE.
- Electrical power is a product of both voltage and
current, not either one separately.
- Horsepower and watts are merely two different units for
describing the same kind of physical measurement, with 1
horsepower equaling 745.7 watts.
Lessons In Electric Circuits copyright (C) 2000-2002 Tony
R. Kuphaldt, under the terms and conditions of the
Design
Science License.
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