U.S. patent number 3,586,100 [Application Number 04/809,258] was granted by the patent office on 1971-06-22 for heat dissipating devices for the collectors of electron-beam tube.
This patent grant is currently assigned to Nippon Electric Company, Limited. Invention is credited to Ryuzo Orui, Susumu Yasuda.
United States Patent |
3,586,100 |
Yasuda , et al. |
June 22, 1971 |
**Please see images for:
( Certificate of Correction ) ** |
HEAT DISSIPATING DEVICES FOR THE COLLECTORS OF ELECTRON-BEAM
TUBE
Abstract
A heat-dissipating device for the collectors of electron-beam
tubes such as a traveling wave tube. The collector slides loosely
into a bore within a cylindrical heat-absorbing and conducting
member. The heat-absorbing member is connected to a finned
heat-radiating structure to which heat is conducted for
dissipation. A tight fitting between the collector and the
heat-absorbing member is created by the presence of a restraining
collar placed around the heat-absorbing member. The collar has a
smaller coefficient of expansion than the heat-absorbing member,
and the heat-absorbing member has longitudinal slots therein, the
net effect of which is to cause the heat-absorbing member to
constrict about the collector when the assembly heats to operating
temperature. BACKGROUND OF THE INVENTION
Inventors: |
Yasuda; Susumu (Tokyo,
JA), Orui; Ryuzo (Tokyo, JA) |
Assignee: |
Nippon Electric Company,
Limited (Tokyo, JA)
|
Family
ID: |
13435765 |
Appl.
No.: |
04/809,258 |
Filed: |
March 21, 1969 |
Foreign Application Priority Data
|
|
|
|
|
Sep 28, 1968 [JA] |
|
|
70585/68 |
|
Current U.S.
Class: |
165/80.3; 165/81;
174/16.1; 313/45; 165/185; 313/40 |
Current CPC
Class: |
F28F
13/00 (20130101); H01J 19/36 (20130101); H01J
23/033 (20130101); H01J 2893/0027 (20130101) |
Current International
Class: |
H01J
23/02 (20060101); H01J 19/36 (20060101); H01J
19/00 (20060101); H01J 23/033 (20060101); H01j
007/24 () |
Field of
Search: |
;317/234A ;174/16
;313/45,40 ;165/80,185,81 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Davis, Jr.; Albert W.
Claims
What we claim is:
1. A heat-dissipating device for the collector of an electron-beam
tube comprising a heat-radiating member, a heat-conducting member
disposed adjacent said heat-radiating member in thermal contact
therewith, said heat-conducting member having an axial bore having
a normal diameter for relatively loosely receiving therein the
collector of an electron-beam tube prior to the operation of the
tube, said bore extending from one end of said heat-conducting
member inwardly a distance corresponding to at least a fraction of
the full length thereof, at least one slot extending in the axial
direction of said bore a distance corresponding to at least a
fraction of the full length of said heat-conducting member and in
the transverse direction thereof the full width of said
heat-conducting member, and at least one annular member fitted on
the peripheral surface of said heat-conducting member coaxially
therewith and surrounding at least a fraction of the full length
thereof containing said at least one slot, said at least one
annular member being made of a material possessing a smaller
thermal expansion coefficient than that of the material of which
said heat-conducting member is made, said annular member defining
means when the tube is in operation and thus heated for acting upon
said conducting member to thereby restrain the outward radial
expansion of said heat-conducting member, modify the diameter of
said bore, and cause the collector to establish a relatively close
fit between the collector and said heat-conducting member.
2. A heat-dissipating device for heat-generating electronic
elements or the like comprising: a heat-dissipating structure
having a recess therein, heat-conducting means positioned within
the recess of and in heat-transferring relationship with said
heat-dissipating structure so that heat will flow from said
heat-conducting member to said heat-dissipating structure, said
heat-conducting means having an aperture therein adapted to
slidingly receive a heat-generating element, and at least one
substantially longitudinal slot through the body thereof
communicating around and against a portion of said heat-conducting
means and within a plane substantially normal to the longitudinal
axis there to retard outward radial expansion of said
heat-conducting means, said band being constructed of a material
having a coefficient of expansion substantially smaller than the
coefficient of expansion of the material of which said
heat-conducting means is constructed, so that when heated by the
heat-generating element placed therein, said retaining band means
acts on said heat-conducting means to cause the latter to expand
radially inwardly and thereby modify the diameter of said aperture
to thereby establish a relatively close fit between the
heat-generating element and said heat-conducting means.
3. The device of claim 2 wherein said retaining band is disposed
around the area of said heat-conducting means containing said slot,
and wherein said heat-conducting means has a neck therein, said
neck being between the portion of said heat-conducting means having
the slot therein and the remainder thereof.
4. The device of claim 3 wherein said heat-dissipating structure
and said heat-conducting means have a common bore therethrough
sized to slidingly receive a collector of an electron-beam tube,
and wherein the aperture in said heat-conducting means comprises a
portion of the bore.
5. The device of claim 4 wherein said heat-conducting device is
substantially cylindrical and has opposing slots therein along a
plane containing the longitudinal axis of said heat-conducting
device, and extending from the end opposite the neck thereof
through said neck.
6. The device of claim 5 wherein said retaining band comprises a
ring frictionally fitted around a substantial portion of said
cylindrical heat-conducting means containing the opposing
slots.
7. The device of claim 6 wherein one end of said heat-conducting
means abuts said heat-dissipating structure, and wherein a
substantial portion of said heat-conducting means opposite said
abutting end tapers outwardly, and wherein said retaining ring
tapers correspondingly, and wherein said heat-dissipating device is
further comprised of means to thread said retaining ring into said
heat-conducting means.
Description
This invention relates to heat-dissipating devices for heat
producing electronic elements and particularly for the collectors
of electron-beam tubes such as the traveling-wave tube,
backward-wave tube, and the like.
A heat-dissipating system for a traveling-wave tube has been widely
used. According to this system, a tapered section of the collector
fits into a conical bore of a heat-radiating member and the desired
fit between the two concentric conical contacting surfaces is
maintained by adjusting a clamping nut fitted on a threaded
boltlike projection at the end of the collector.
The cooling efficiency of such a device for the collector has been
found to be considerably higher when the two conical contacting
surfaces of the collector and the heat radiating member are fitted
tightly together. The need for manual control of the clamping nut,
however, is inconvenient, in that it restricts the mounting
position of the traveling-wave tube in the microwave communication
equipment to positions where the clamping nut is accessible.
The ever-increasing demand for greater miniaturization of
present-day electronic equipment has necessitated the efficient
utilization of available space and a higher concentration per unit
volume of component parts, including traveling-wave tubes in
microwave communication equipment. In extreme cases, the
heat-radiating member of a traveling-wave tube must be positioned
in a remote location in the equipment in order to provide ease of
tube replacement from the opposite side, which positioning
prohibits manual adjustments of the aforementioned variety.
Therefore, there has been an increasing demand among equipment
designers and users for the advent of a new heat-dissipating system
for the collectors of electron-beam tubes which dispenses with the
need for such clamping nut adjustment in tube insertion or
removal.
It is consequently a general object of this invention to provide a
new and improved heat-dissipating system for the collectors of
electron-beam tubes which overcomes the aforementioned difficulties
of the prior art. Stated more particularly, it is an object of this
invention to provide a new and improved heat-dissipating device for
the collectors of electron-beam tubes which dispenses with manual
control of the clamping nut as in the prior art, automatically
provides a tight fit between the contacting surfaces of the
collector and the heat-conducting element after the tube has been
operated for a predetermined time interval, and which further
enables tube removal after the tube operation has been suspended
for a predetermined time interval.
SUMMARY
A heat-dissipating device according to this invention comprises a
heat transfer or conducting member, generally but not exclusively,
of cylindrical or tapered cylindrical form provided with a
cylindrical or conical axial bore for insertion of the collector of
an electron-beam tube, one or more slots in the sides of the heat
transfer member extend generally from one end inwardly in the axial
direction thereof for a distance corresponding at least to a
fraction of the overall length thereof, and in the transverse
direction thereof by a width corresponding to the full wall
thickness of the heat transfer member from the bore wall surface to
the peripheral wall surface. A neck near the inner end of the heat
transfer member generally facilitates the contraction of the
slotted sides thereof about the collector. At least one annular
retainer means made of a material having a smaller thermal
expansion coefficient than the material of the heat-conducting
element fitted around the peripheral surface of the heat transfer
member so as to surround at least a fraction of the length of the
slotted sides thereof. A heat radiating member of any suitable
geometrical shape adapted for heat dissipation is disposed adjacent
the heat conducting member to establish direct or indirect thermal
contact therebetween. A single slot which extends throughout the
full axial length of the heat-conducting member, or a plurality of
slots the opposite ends of each terminate inside of the
heat-conducting member are suitable alternatives to the
above-described slots. An outstanding advantage of this assembly is
that a tight fit between the tube collector and the heat transfer
element is automatically obtained soon after the tube is put into
operation.
The principles of this invention may best be understood by
reference to the following description of two preferred embodiments
of this invention illustrated in the accompanying drawings.
Throughout the specification and drawings, all like parts or
members are given like designation numbers to facilitate a better
understanding of the invention.
FIG. 1 is a longitudinal cross-sectional view of a heat-dissipating
device according to a first preferred embodiment of this
invention;
FIG. 2 is an end view of the device shown in FIG. 1;
FIG. 3 is a side view of a heat-conducting member used in the first
embodiment of this in invention shown in FIG. 1;
FIG. 4 is an end view of the heat-conducting element shown in FIG.
3;
FIG. 5 is a longitudinal cross-sectional view of a heat-dissipating
device according to a second preferred embodiment of this
invention;
FIG. 6 is an end view of the device shown in FIG. 5.
Now referring in more detail to FIGS. 1 and 2, there is shown a
heat-dissipating device 1 for dissipating heat produced by the
collector 4 of a traveling-wave tube 3 (only the collector and its
vicinity thereof are illustrated). The device is composed of a
cylindricaL heat-radiating radiating member 9 provided with an
axial bore 9a, and an axial counterbore 9b, and having a plurality
of fins 8. A heat-conducting member 7 provided with a flangelike 7a
at the inner end for maintaining a low-resistance thermal contact
with the internal sidewall surface 10 of the heat-radiating member
is attached to surface 10 by member 9 by means of solder or screws.
Conducting member 7 has an axial bore 5 therethrough for the
insertion of the collector 4, and a pair of symmetrical slots 6
extending inwardly from the outer end of conducting member 7 and
disposed in a plane containing the axis of bore 5. An annular
member 12 is fitted securely on the peripheral surface 7b of
conducting member 7 to impose a restraint on the thermal expansion
in the radial direction of the heat-conducting member 7 when the
latter is heated.
The heat-conducting element 7 is made of a material possessing a
high thermal conductivity and a high thermal expansion coefficient
such as aluminum (thermal expansion coefficient is approximately
23.5.times.10 .sup.-.sup.6), whereas the annular member 12 is made
of a material possessing a low thermal expansion coefficient such
as a nickel-iron alloy containing 36 percent nickel (thermal
expansion coefficient is approximately
1.5.times.10.sup.-.sup.6).
The figures illustrate the structure of the device 1 before being
heated to operating temperature.
The diameter of the bore 5 is designed to be larger than the
diameter of the collector 4 by tens of microns under this
condition. When the tube 3 is placed in operation, a power loss of
the collector 4 causes its temperature to rise. Since the collector
4 and the heat-conducting member 7 are initially in partial contact
with each other in spite of the presence of a clearance
therebetween, the temperatures of members 7 and 12 begin to rise
gradually and simultaneously, and the heat-conducting member 7
begins to thermally expand.
Since the annular member 12 is made of a material possessing the
smaller thermal expansion coefficient of the two, and is initially
tightly fitted on the external peripheral surface 7b of the element
7, the outward radial thermal expansion of conducting member 7 is
restrained, resulting in the inward expansion of the outer end of
the element 7 as indicated by the arrows 16 and 17 (FIG. 2), which
inward expansion is substantially perpendicular to the plane
containing the slots. Therefore this portion of conducting member 7
is compressed firmly against the collector 4. The constricted neck
portion 18 in conducting member 7 some distance removed from the
edge of the annular member 12 to facilitates the inward expansion
of the right-hand side of conducting member 7.
The compressive force of conducting member 7 against the collector
4 thus created is extremely large, resulting in a decrease in
thermal resistance between the contacting peripheral surface 42 of
the collector 4 and surface of bore 5 in the heat-conducting
conducting member 7; and promotes efficient conduction of the heat
generated by the collector 4 to the heat-radiating member 9 for
subsequent dissipation into the air.
The region of the collector 4 compressed by the heat-conducting
member 7 is restricted to that portion which is surrounded by the
annular member 12. According to our experiment, however, excessive
local temperature rises at that portion of the collector 4 not
directly compressed are avoided and the temperature distribution
along the axial length of the collector 4 made approximately
uniform by selecting a collector made of material possessing a high
thermal conductivity (such as copper), and having a wall
sufficiently thick to carry heat to the region of contact between
collector 4 and conducting element 7.
A second embodiment of this invention is illustrated in FIGS. 5 and
6. This embodiment differs from the first in the following
respects: (a) element 7 is tapered toward the outer end, and
annular member 12 is correspondingly shaped so that together they
form two concentric conical surfaces 13 that can fit together; (b)
the end outer portion of element 7 is threaded as shown at 14 and
annular member 12 is internally threaded to thread thereon. The
clearance between the collector 4 and the heat-conducting member 7
is initially set by tightening annular member 12 on element 7, and
no further adjustment is needed. This adjustment is accomplished
before installation of the device in communication equipment.
The second embodiment functions upon the same principles and in
substantially the same manner as the embodiment of FIG. 1;
therefore a detailed description is omitted. An advantage of the
second embodiment over the first is that dimensional tolerances of
the mating surfaces of members 7 and 12 less rigorous and machining
becomes easier, because the tightness of fit between elements 7 and
12 and the clearance between element 7 and collector 4 can be
suitably controlled by tightening threaded member 12.
The relationship between the dimensions of various components and
materials to be used therefor which have been taken into
consideration in designing the heat-dissipating devices above
described are as follows.
SYMBOL DEFINITIONS
T.sub.0 = room temperature
d.sub.1 = diameter of the collector 4 of a traveling-wave tube when
the tube is at room temperature
d.sub.2 = diameter of bore 5 of heat-conducting member when member
7 is at room temperature 7
d.sub.3 = inside diameter of annular member 12 (maximum inside
diameter of the tapered section in case of the second embodiment)
when at room temperature
T.sub. 1 = temperature of collector 4 under steady operating
condition of the traveling-wave tube
T.sub. 2 = temperature of heat-conducting member 7 and annular
member 12 fitted thereon under steady operating conditions of the
traveling-wave tube
.alpha..sub.1 = thermal expansion coefficient of the collector
4
.alpha..sub.2 = thermal expansion coefficient of the
heat-conducting member 7
.alpha..sub.3 = thermal expansion coefficient of the annular member
12
d .sub.1 ' = diameter of collector 4 under steady state operating
conditions of the traveling-wave tube
d.sub.2 ' = diameter of bore 5 at that part of collector which is
compressed by members 7 and 9 in a direction perpendicular to the
plane containing two slots 6 under steady state operating condition
of the traveling-wave tube.
Then d.sub. 1' and d.sub. 2 ' can be expressed as
d.sub.1 '=d.sub.1 [1+.alpha..sub.1 (T.sub.1 -T.sub.0)] (1)
d.sub.2 '=d.sub.2 +(T.sub.2 -T.sub.0)[ .alpha..sub.2 d.sub.2
-(.alpha..sub.2 -.alpha..sub.3) d.sub.3 ] (2)
In order for collector 4 to be compressed by the heat-conducting
member 7 will be
d.sub.1 '>d.sub.2 ' (3)
Numerical data for an experimental model which was designed and
fabricated according to the second embodiment on the basis of the
foregoing equations is as follows: ##SPC1##
Diameters at various parts of the heat-conducting member 7 and the
annular member 12 are as indicated in Table 1. ##SPC2##
Using the numerical data indicated in Table 1 and the temperature
rises assumed above, the diameter d.sub.1 ' of the collector 4 and
the diameter d.sub.2 ' at the compressing part of the
heat-conducting member 7 under operating condition of the tube were
derived by computation as 8.972 mm. and 8.957 mm., respectively.
Therefore the condition for compression (3) is well
established.
In the above experiment, the clearance between the collector 4 and
the heat-conducting member 7 was made to be 0.05 mm. with the
assembly at T.sub.0, so that the tube could easily be inserted into
and withdrawn from the bore therefrom. It was observed that the
compression occurred in about 7 minutes after the tube was put into
operation. It was further confirmed that the temperatures of
collector 4, heat-conducting member 7, and heat-radiating member 9
under steady state of tube operation were 105.degree. C.,
93.degree. C., and 80.degree. C., respectively. In view of the
allowable maximum temperature of 180.degree. C. for the collector,
it was confirmed that cooling of the collector was satisfactory. No
excessive temperature rise of the collector 4 was detected during
the 7-minute warmup interval, and the tube could be easily
withdrawn after the operation of the tube had been suspended for
about 45 seconds.
Among the outstanding merits of this invention as reduced into
practice will be recapitulated.
No manual control on the collector side of the device such as
turning the clamping nut is required in tube replacement; the
replacement tube can thus be inserted or removed from the end
opposite that of the collector, as the collector slides freely
within the heat-dissipating device of the invention. Thus the
device may be located at an inaccessible or innermost part in the
equipment.
The cooling efficiency of the devices compares favorably with those
of conventional devices for the following. The outward radial
thermal expansion of the heat-conducting member is restricted by
the provision of at least one annular retaining member possessing a
smaller thermal expansion coefficient. This causes inward radial
thermal expansion of the heat-conducting member 7, which is further
aided by the presence of the slot or slots. As a result, the
collector is strongly compressed by the thermally expanded
heat-conducting member along at least a fraction of the full length
thereof, which reduces the thermal resistance between the
contacting surfaces. Even if the temperature rise is not so large,
the compression achieved is at least equal to that which could be
obtained by tightening the nut according to the conventional
design.
Utilization of the invention frees the designer of microwave
communication equipment and the like incorporating electron-beam
tubes from past restriction arising from the need for access to the
heat-dissipating device therefore.
While the principles of the invention have been described in
connection with the above specific apparatus, it is to be clearly
understood that this description is made only by way of example and
not as a limitation to the scope of the invention.
* * * * *