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handbook of modern sensors

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118 3 Physical Principles <strong>of</strong> Sensing<br />

and, in the result, we obtain the differential equation<br />

dT h<br />

dt<br />

+ T h<br />

RC = Q 1<br />

C + T a<br />

RC . (3.161)<br />

This is a first-order differential equation which is typical for thermal systems. A<br />

thermal element, if not a part <strong>of</strong> a control system with a feedback loop, is inherently<br />

stable.Aresponse <strong>of</strong> a simple thermal element may be characterized by a thermal time<br />

constant, which is a product <strong>of</strong> thermal capacity and thermal resistance: τ T = CR. The<br />

time constant is measured in units <strong>of</strong> time (s) and, for a passively cooling element, is<br />

equal to the time which it takes to reach about 37% <strong>of</strong> the initial temperature gradient.<br />

3.14.3 Electrical Elements<br />

There are three basic electrical elements: the capacitor, the inductor, and the resistor.<br />

Again, the governing equation describing the idealized elements are given in Table<br />

3.4. For the idealized elements, the equations describing the sensor’s behavior may be<br />

obtained from Kirchh<strong>of</strong>f’s laws, which directly follow from the law <strong>of</strong> conservation<br />

<strong>of</strong> energy:<br />

Kirchh<strong>of</strong>f’s first law: The total current flowing toward a junction is equal to the total<br />

current flowing from that junction (i.e., the algebraic sum <strong>of</strong> the currents flowing<br />

toward a junction is zero).<br />

Kirchh<strong>of</strong>f’s second law: In a closed circuit, the algebraic sum <strong>of</strong> the voltages across<br />

each part <strong>of</strong> the circuit is equal to the applied e.m.f.<br />

Let us assume that we have a sensor whose elements may be represented by a circuit<br />

shown in Fig. 3.50B. To find the circuit equation, we will use the Kirchh<strong>of</strong>f’s first<br />

law, which is sometimes called Kirchh<strong>of</strong>f’s current law. For the node,<br />

i 1 − i 2 − i 3 = 0, (3.162)<br />

and for each current,<br />

i 1 = e − V 3<br />

R 1<br />

= 1 L<br />

∫<br />

(V 3 − V 1 )dt,<br />

i 2 = V 1 − V 2<br />

R 3<br />

= C dV 2<br />

dt ,<br />

i 3 = V 1<br />

R 2<br />

. (3.163)<br />

When these expressions are substituted into Eq. (3.162), the resulting equation becomes<br />

V 3<br />

+ V 1 − V 2<br />

+ 2 V 1<br />

+ C dV 2<br />

− 1 ∫<br />

(V 3 − V 1 )dt= e . (3.164)<br />

R 1 R 3 R 2 dt L<br />

R 1<br />

In Equation (3.164), e/R 1 is the forcing input, and the measurable outputs are V 1 ,<br />

V 2 , and V 3 . To produce Equation (3.164), three variables i 1 , i 2 , and i 3 have to be

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