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handbook of modern sensors

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3.14 Dynamic Models <strong>of</strong> Sensor Elements 115<br />

several independent variables; however, one <strong>of</strong> them must be time. The resulting<br />

model is referred to as a lumped parameter model. In this section, mathematical<br />

models are formed by applying physical laws to some simple lumped parameter sensor<br />

elements. In other words, for the analysis, a sensor is separated into simple elements<br />

and each element is considered separately. However, once the equations describing<br />

the elements have been formulated, individual elements can be recombined to yield<br />

the mathematical model <strong>of</strong> the original sensor. The treatment is intended not to be<br />

exhaustive, but rather to introduce the topic.<br />

3.14.1 Mechanical Elements<br />

Dynamic mechanical elements are made <strong>of</strong> masses, or inertias, which have attached<br />

springs and dampers. Often the damping is viscous, and for the rectilinear motion,<br />

the retaining force is proportional to velocity. Similarly, for the rotational motion, the<br />

retaining force is proportional to angular velocity. Also, the force, or torque, exerted<br />

by a spring or shaft is usually proportional to displacement. The various elements and<br />

their governing equations are summarized in Table 3.4.<br />

One <strong>of</strong> the simplest methods <strong>of</strong> producing the equations <strong>of</strong> motion is to isolate<br />

each mass or inertia and to consider it as a free body. It is then assumed that each <strong>of</strong><br />

the free bodies is displaced from the equilibrium position, and the forces or torques<br />

acting on the body then drive it back to its equilibrium position. Newton’s second law<br />

<strong>of</strong> motion can then be applied to each body to yield the required equation <strong>of</strong> motion.<br />

For a rectilinear system, Newton’s second law indicates that for a consistent system<br />

<strong>of</strong> units, the sum <strong>of</strong> forces equals the mass times the acceleration. In the SI system <strong>of</strong><br />

units, force is measured in newtons (N), mass in kilograms (kg), and acceleration in<br />

meters per second squared (m/s 2 ).<br />

For a rotational system, Newton’s law becomes the sum <strong>of</strong> the moments equals the<br />

moment <strong>of</strong> inertia times the angular acceleration. The moment, or torque, has units<br />

Table 3.4. Mechanical, Thermal, and Electrical Analogies

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