U.S. patent number 3,857,017 [Application Number 05/245,773] was granted by the patent office on 1974-12-24 for unitary thermal reference source.
This patent grant is currently assigned to Dynarad, Inc.. Invention is credited to Carl H. Whittier.
United States Patent |
3,857,017 |
Whittier |
December 24, 1974 |
UNITARY THERMAL REFERENCE SOURCE
Abstract
A thermal reference source in which the interrelated functions
of heater, radiator, and temperature sensor are provided by a
unitary and integrally formed structure. The reference is formed of
a homogeneous, temperature sensitive resistive material shaped to
define a radiative cavity and includes terminals for connection to
an associated control circuit. Temperature changes are sensed in a
substantially instantaneous manner and rapid control easily
maintained.
Inventors: |
Whittier; Carl H. (Wayland,
MA) |
Assignee: |
Dynarad, Inc. (Norwood,
MA)
|
Family
ID: |
22928017 |
Appl.
No.: |
05/245,773 |
Filed: |
April 20, 1972 |
Current U.S.
Class: |
219/501; 219/504;
219/499; 219/505 |
Current CPC
Class: |
H05B
3/00 (20130101); G05D 23/2401 (20130101); G01J
5/522 (20130101) |
Current International
Class: |
G01J
5/52 (20060101); G05D 23/20 (20060101); H05B
3/00 (20060101); G05D 23/24 (20060101); H05b
001/02 () |
Field of
Search: |
;250/84,85
;219/300,469,470,471,501,504,505,553,499,313,390,427 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Trammell; James D.
Assistant Examiner: Bell; Fred E.
Attorney, Agent or Firm: Weingarten, Maxham &
Schurgin
Claims
What is claimed is:
1. A thermal reference comprising:
a generally hollow, cylindrical structure open at each end and
formed of an electrically resistive material having a significantly
non-zero resistance temperature coefficient;
said cylindrical structure having an elbow curve in a portion
thereof whereby an interior surface of said structure occludes the
view through said cylindrical structure from end to end;
first and second terminals on said structure at said ends for
receiving electrical current;
means for applying electrical current to said structure at said
first and second terminals to provide a distributed current through
said structure;
the flow of electrical current through said structure being
directly operative to simultaneously affect the temperature,
radiation, and resistance of said structure.
2. The thermal reference of claim 1 further including:
means for sensing the resistance of said structure between said
terminals; and
means for controlling the application of current to said structure
to maintain a predetermined resistance for said material.
3. A unitary thermal reference source comprising:
an elongated unitary structure open at at least one end and formed
of an electrically resistive material having a non-zero resistance
temperature coefficient and having a cavity therein terminating at
said at least one open end in an aperture from which thermal energy
is radiated;
first and second electrical terminals affixed and in electrical
contact with respective opposite ends of said elongated structure;
and
means for applying electrical current directly to said structure at
said first and second electrical terminals to provide a distributed
current flow through said structure;
the flow of electrical current through said structure being
directly operative to simultaneously affect the temperature,
radiation and resistance of said structure;
said means for applying electrical current to said terminals
further including means for controlling the current applied to said
first and second terminals in response to the resistance of said
structure between said terminals and operative to maintain said
resistance of said structure at a predetermined value.
4. The thermal reference of claim 3 wherein said current
controlling means further includes:
a resistive bridge having said structure as one leg thereof
connected between said first and second terminals;
means for applying electrical current to a first pair of opposite
nodes of said bridge;
means for sensing the potential difference between a second pair of
opposite nodes of said bridge; and
means responsive to the sensed potential difference for regulating
the current applied to said first pair of opposite nodes of said
bridge so as to maintain said sensed potential difference at a
predetermined value.
Description
FIELD OF THE INVENTION
This invention relates to thermal reference sources and more
particularly to a thermal source for providing an accurate and
controllable thermal radiation standard.
BACKGROUND OF THE INVENTION
In thermal instrumentation it is often necessary to employ a
reference source which provides thermal radiation at predetermined
temperatures for monitoring, calibrating, or other purposes.
Reference sources which accomplish these functions are known in the
art and typically comprise a structure capable of radiating energy
in a selected temperature range, the radiating structure being
indirectly heated such as by separate electrical heating coils
wound therearound. In order to maintain a predetermined operating
level, the temperature of the radiating structure is monitored by
one or more separate sensors attached to the structure. These
sensors typically include a thermocouple affixed to the structure
or a coil of temperature sensitive wire, such as platinum, wound
therearound.
These prior art reference sources suffer several disadvantages
which limit their utility. In addition to the complexity of making
such sources, they have proved to be less than ideal in providing
uniform and accurate temperature references. The indirect heating
of the radiating structure from a number of separate coils or
heated spots results in the inefficient transfer of heat from the
coils to the radiating structure. Control of the temperature of
this structure also depends upon indirect temperature monitoring
from separate sensors. An inherent time delay exists in the
transfer of heat from the heater coils to the radiating structure
and thence to the thermal sensors and the speed and accuracy of
temperature regulation is thus limited and requires expensive
control electronics to even partially compensate. Moreover,
variation in the properties of the separate heaters and/or sensors
can contribute further errors to the level of output radiation. The
indirect heating of a radiating structure from a series of discrete
points also is likely to cause variation in the heating of the
overall structure and radiation of temperatures outside the desired
range.
BRIEF SUMMARY OF THE INVENTION
These and other problems of the prior art are overcome by a thermal
reference which, according to a preferred embodiment of the
invention, comprises a unitary radiative structure of a homogenous
electrically resistive composition that integrally provides the
functions of heater and temperature sensor as well as thermal
radiator. Properties of the unitary structure directly provide the
functions of heating, radiating and temperature sensing and thereby
eliminate the inefficiencies of indirect heat transfer. There is
thus no thermal gradient or time lag between heating and sensing or
radiating and sensing.
The radiative structure typically comprises an electrically
resistive material formed in a shape defining a radiative cavity
and having electrical connections for application of energizing
current thereto. To provide the directly coacting functions of
heater, radiator, and sensor, a thermistor material is typically
employed to provide a temperature sensitive electrical resistance
for the structure material. Temperature regulation is achieved by
connecting the unitary structure as one arm of an electrical bridge
circuit which is excited to heat the structure to a requisite
level. The temperature dependent device resistance is employed in a
circuit to adjust the excitation current to maintain radiation at
an intended temperature.
DESCRIPTION OF THE DRAWINGS
These and other features of the invention will be more fully
understood by reference to the following detailed description of a
preferred embodiment presented for purposes of illustration and not
by way of limitation and to the accompanying drawings of which:
FIG. 1 is a prior art thermal source over which the present
invention is an improvement;
FIGS. 2A and 2B are pictorial and sectional views, respectively, of
a thermal reference source according to the invention;
FIG. 3 is a schematic diagram of circuitry useful in controlling
the temperature of the thermal reference of the invention;
FIG. 4 is a graph illustrating typical resistance versus
temperature characteristics of the thermal reference of the
invention; and
FIG. 5 is a sectional view of a modification of the embodiment of
the invention shown in FIGS. 2A and 2B.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
Referring to FIG. 1, a prior art device of conventional design for
providing a thermal reference comprises a black body shell 12
defining a cavity and having an interior surface for radiating
thermal energy in a spectral emittance band characteristic of a
desired temperature. To excite the body to a predetermined
temperature a plurality of turns of a heater coil 14 are wrapped
around the exterior surface of the shell 12 and in intimate contact
thermally. The coil 14 may be energized by a suitable current from
a source not shown. A plurality of turns of a separate coil 16 are
wound in bifilar manner around shell 12, this coil 16 being
composed of a wire such as platinum, the resistance of which varies
with temperature and which serves as a sensor for measuring the
temperature of shell 12. The coil 16 may be connected to a
controller for the source of current for heater coil 14 for control
of the current passing through coil 14 in order to maintain a
predetermined cavity radiating temperature.
As can be seen from FIG. 1 the ultimate goal of providing a
predetermined radiation from body 12 is achieved through indirect
heating and sensing of device temperature with distinct coils 14
and 16 respectively. Despite good thermal contact with the body 12
to minimize heat transfer losses, the efficiency of thermal
transfer is still such as to cause a gradient between the coils 14
and 16 and the cavity resulting in a variation from point to point
in the body and inaccuracies in the sensed temperature.
Not only do these inaccuracies exist in the prior art structure of
FIG. 1 but the construction of such devices, requiring the
interspersing of two coils having controlled spacing, is
complicated and often demands hand fabrication.
Referring now to FIGS. 2A and 2B, pictorial and sectional views are
presented of a thermal reference according to the invention and
which provides combined heating, sensing, and radiating functions
in a single structure which completely avoids the problems of heat
transfer efficiency and temperature variations. About an axis of
symmetry 18 a cavity 20 is defined by a cylinder 22 which is
composed of a material having an electrical resistance that varies
with temperature. On opposite ends 24 and 26, annular electrical
contacts 28 and 30 respectively are secured in electrical contact
with the material of cylinder 22. The material of cylinder 22 has
an inner radiating surface 32 which creates an internal radiator
that may be viewed through either end of cylinder 22.
Various types of compositions can be used for the material of
cylinder 22. The significant characteristics for the material are
that it have a resistance which varies with temperature, either a
positive or negative temperature coefficient as indicated in FIG. 4
being acceptable. As an example, thermistor materials have
generally been found satisfactory for use in forming the cylinder
22.
The electrical connectors 28 and 30 may be of any electrically
conductive material which, when necessary, may be matched in its
coefficient of thermal expansion to the substance composing the
cylinder 22.
As indicated in FIG. 2B electrical excitation may be provided from
a battery 36 to heat cylinder 22 through a variable resistor 38. It
can be seen that once an equilibrium condition exists with current
flowing from the battery 36 through the resistor 38 and cylinder
22, any change in temperature of the cylinder 22 will alter its
resistance and vary the current and power flowing through the
cylinder 22. By selecting an appropriate value of resistance in
resistor 38 and resistance and temperature coefficient for cylinder
22, the temperature change will be counteracted by a change in
power applied to the cylinder 22 in a sense tending to restore the
original temperature equilibrium.
The utilization of the combined heating, sensing and radiating
properties in the material of cylinder 22 for providing a well
regulated temperature reference can be better described, however,
by reference to FIG. 3. As indicated there, the cylinder 22 is
connected into a bridge circuit 39 through its electrical contacts
28 and 30. In particular the contact 30 is connected to ground
along with one terminal of a variable resistor 40. The contact 28
is connected to a fixed resistor 42 through a terminal 44 of the
bridge. The ungrounded terminal of the variable resistor 40 is
connected to a fixed resistor 46 through a terminal 48. The
opposite terminals of fixed resistors 42 and 46 are tied together
at a terminal 50.
The terminals 44 and 48 are applied to differential inputs of a
high gain amplifier 52. The output of the amplifier 52 is applied
through a resistor 54 to an operational amplifier 56 having a path
of negative feedback therearound through a resistor 58 to cause the
amplifier 56 to operate with a gain determined by the ratio of the
resistor 58 to the resistor 54. A further differential amplifier 60
receives on a noninverting input the output of the operational
amplifier 56, and on an inverting input the potential supplied by a
reference 62. The output of the amplifier 60, as referenced to
ground, is applied to the terminal 50.
To explain the operation of the circuitry of FIG. 3 it will be
assumed that the material comprising the cylinder 22 has a positive
temperature coefficient as indicated by curve 64 in FIG. 4 and that
it is desired to regulate the temperature thereof at a temperature
T.sub.o which produces a corresponding cylinder resistance R.sub.o.
Initially the variable resistor 40 will be adjusted so that its
resistance takes on the value R.sub.o. Assuming at initial turn-on
that the resistance between the connectors 28 and 30 is
substantially less than R.sub.o, the output of the amplifier 60
will be a large positive potential thereby increasing the voltage
applied to the terminal 50 and correspondingly the current through
the cylinder 22. At this point the cylinder 22 will begin to
increase in temperature and in resistance. At a predetermined value
of resistance, differing from R.sub.o by a small error, depending
upon the gains and offsets of the amplifiers, an equilibrium
condition is reached with the difference between the two inputs to
the amplifier 52 as small as desired. As further embellishments,
the amplifiers can be made of conventional saturating designs so
that enormously high voltages are avoided. If resistor 58 is
replaced with a capacitor, integrating control can be achieved or a
combination employed.
If the material forming the cylinder 22 has a negative temperature
coefficient such as in curve 66 in FIG. 4, it would be necessary to
provide an inversion in the variation of current applied to
terminal 50 with resistance. The circuitry of FIG. 4 could be
readily modified to accomplish this function by an inversion of
signal variations as is known in the art.
Referring now to FIG. 5 a modification of the thermal reference of
FIGS. 2A and 2B is shown. A cylinder 70 is provided defining an
inner cavity 72 and having a gradually curved elbow portion 74.
Annular electrical contacts 76 and 78 are attached to either end as
before to apply electrical current to the material of cylinder 70.
When viewing the cavity 72 from the end of the contact 76, the
elbow portion 74 optically closes the cavity 72 with a minimum of
distortion to the uniformity of the cylinder 70 and without closing
one of its ends. This facilitates providing a uniform heating to
the cylinder 70. A similar result may be achieved by a shallow
taper to the cavity 20 in FIG. 2B or by other techniques or
curves.
While the thermal reference indicated above has been discussed with
reference to particular cavity shapes and circuit configurations,
modifications departing from these specific patterns may be
employed. It is accordingly intended to limit the scope of the
invention only as indicated in the following claims.
* * * * *