Thick film element having coated substrate with high heat conductivity

Information

  • Patent Grant
  • 11419186
  • Patent Number
    11,419,186
  • Date Filed
    Saturday, March 26, 2016
    8 years ago
  • Date Issued
    Tuesday, August 16, 2022
    a year ago
Abstract
The present invention provides a thick film element having a coated substrate with high heat conductivity, which comprises a carrier, a thick film coating deposited on the carrier and a covering layer overlaid on the coating. The thick film coating is a heating material, and the mode of heating is electrical heating. The carrier, the thick film coating and the covering layer are selected from a material that fulfills every of the following equations:
Description
FIELD OF THE INVENTION

The present invention relates to the field of thick film, and more particularly to a thick film element having a coated substrate with high heat conductivity.


BACKGROUND OF THE INVENTION

Thick film heating elements refer to heating elements that are made by fabricating exothermic materials on a substrate into thick films and providing electricity thereto to generate heat. The conventional heating methods include electrical heated tube heating and PTC heating. An electrical heated tube heating element uses a metal tube as the outer case and distributes nickel-chromium or iron-chromium alloy spirally therein to form heater strips; the clearance space is then filled with magnesite clinker that has excellent thermal conductivity and insulativity and sealed with silica gel from two ends of the tube. The PTC heating method uses ceramics as the exothermic material. Both electrical heated tube heating and PTC heating conduct heat indirectly with low thermal efficiency, and are structurally huge and bulky. Besides, in consideration of environmental protection, heaters using these two types of heating methods stain easily after repeatedly heating and cleaning thereof is not easy. Additionally, PTC heaters contain lead and other hazardous substances and are easily oxidized, causing power attenuation and short service life.


Chinese application CN201310403454.9 discloses a ceramic tile-based resistance slurry for thick film circuits and the preparation method thereof, which provides a resistance slurry that matches ceramic tiles and provides a possibility for preparation of a new underfloor heating elements. The raw materials of the resistance slurry include solid phase contents (including glass ceramic powder and silver powder) and organic binding agent, with the weight percentage of each of the materials being 70-85% of glass ceramic powder and 15-30% of organic binding agent; the sum of which are 100%. The resistance slurry is mainly used to be printed on the back of ceramic tiles to form a thick film circuit.


Chinese application CN201020622756.7 discloses a thick film circuit device, which comprises a ceramic substrate, a thick film circuit wafer and electric wires. The thick film circuit wafer is disposed on the ceramic substrate, and outer sides of the ceramic substrate are covered by an epoxy layer. The two electric wires are connected to both sides of the ceramic substrate, and the connection points between the electric wires and the ceramic substrate are covered by in the epoxy layer.


It could be seen from the above technologies that thick film technology is developing gradually; however, at present the researches mostly focus on developing resistance slurry for thick film circuits but rarely on the component products of thick films. The technical solution of the above-mentioned thick film circuit device realizes disposing thick film circuits within the ceramic substrate and epoxy layer, but thermal conductivity thereof is not excellent. The application of thick films in products greatly broadens the development of heating products. The existing heating device could meet the demands of heating; however, heating device that performs unilateral heat transfer is rarely seen, or unilateral heat transfer of such device is too poor, making it difficult to reduce heat loss by keeping high unilateral thermal conduction properties.


SUMMARY OF THE INVENTION

To solve the problems mentioned above, the present invention provides a thick film element having a coated substrate with high heat conductivity that has the advantages of small volume, high efficiency, environmental-friendly, high safety performance and long service lifespan.


The concept of thick film in the present invention is a term comparative to thin films. Thick film is a film layer with a thickness ranging from several microns to tens of microns formed by printing and sintering on a carrier; the material used to manufacture the film layer is known as thick film material, and the coating made from the thick film is called thick film coating. The thick film element has the advantages of high power density, fast heating speed, high working temperature, fast heat generating rate, high mechanical strength, small volume, easy installation, uniform heating temperature field, long lifespan, energy saving and environmental friendly, and excellent safety performance.


The thick film element having a coated substrate with high heat conductivity of the present invention comprises a carrier, a thick film coating deposited on the carrier and a covering layer overlaid on the coating. The thick film coating is a heating material, and the mode of heating is electrical heating. The carrier, the thick film coating and the covering layer are selected from a material that fulfills every of the following equations:









λ
3


A








T
3

-

T
0



d
3



=

a
×

λ
1


A








T
1

-

T
0



d
1




,







λ
2


A








T
2

-

T
0



d
2



=

b
×

λ
1


A








T
1

-

T
0



d
1




,








λ
2


A








T
2

-

T
0



d
2



=

c
×

λ
3


A








T
3

-

T
0



d
3




;








10

a


10
4


,

0
<
b


10
6


,


0
<
c


10
3


;






T2<TMinimum melting point of the covering layer;


T2<TMinimum melting point of the carrier;


T0≤25° C.;


wherein the value of







λ
1


A








T
1

-

T
0



d
1







represents the heat transfer rate of the covering layer;


the value of







λ
2


A








T
2

-

T
0



d
2







represents the heat generating rate of the thick film coating; the value of







λ
3


A








T
3

-

T
0



d
3







represents the heat transfer rate of the carrier;


λ1 represents the heat conductivity coefficient of the covering layer at the temperature of T1; λ2 represents the heat conductivity coefficient of the thick film coating at the temperature of T2;


λ3 represents the heat conductivity coefficient of the carrier at the temperature of T3;


A represents the contact area of the thick film coating with the covering layer or the carrier;


d1 represents the thickness of the covering layer;


d2 represents the thickness of the thick film coating;


d3 represents the thickness of the carrier;


T0 represents the initial temperature of the thick film element;


T1 represents the surface temperature of the covering layer;


T2 represents the heating temperature of the thick film coating;


T3 represents the surface temperature of the carrier;


d2≤50 μm;


and d1≥10 μm; 10 μm≤d3≤20 cm;


TMinimum melting point of the carrier>25° C.;


λ3≥λ1;


the covering layer refers to a dielectric layer covering the thick film coating by printing and/or sintering or gluing, and the area of the covering layer is larger than that of the thick film coating.


The carrier is the dielectric layer carrying the thick film coating. The thick film coating covers the carrier by printing, coating, spraying or sintering, and is the coated substrate of the thick film element.


The heat conductivity coefficient refers to the heat transferred by a one-meter-thick material having a temperature difference between two side surfaces of 1 degree (K, ° C.) through one square meter (1 m2) area within one second (1 S) under a stable heat transfer condition. Unit of the heat conductivity coefficient is watt/meter·degree (W/(m·K), and K may be replaced by ° C.).


The covering layer, the thick film coating and the carrier stick closely with each other at the electrical heating parts of the thick film elements, and both sides of the thick film coating connect to external electrodes. When given electricity, the thick film energy. Heat generating rate of the thick film coating could be calculated by







λ
2


A








T
2

-

T
0



d
2







according to heat conductivity coefficient, contact area, initial temperature, heating temperature and thickness of the thick film coating, wherein T2 represents the heating temperature of the thick film.


The present invention features in that the thick film element has a coated substrate having high heat conductivity, and that the heat generating rate of the covering layer, the thick film coating and the carrier should meet the following requirements:


(1) The heat transfer rate of the covering layer and the thick film coating should satisfy the following formula:









λ
3


A








T
3

-

T
0



d
3



=

a
×

λ
1


A








T
1

-

T
0



d
1




,





wherein 10≤a≤104; for those thick film elements satisfied the above equation, the heat transfer ability of their carrier is superior to that of the covering layer, which means that the carrier is fast while the covering layer is slow at temperature rising or that the temperature difference between the covering layer and the carrier is large after stable heat balance. Therefore, the thick film elements generally show the technical effect of carrier heating.


(2) The heat generating rate of the thick film coating and the heat transfer rate of the covering layer should satisfy the following formula:









λ
2


A








T
2

-

T
0



d
2



=

b
×

λ
1


A








T
1

-

T
0



d
1




,





wherein 0<b≤106; if the heat generating rate of the thick film coating is much larger than the heat transfer rate of the covering layer, the continuously accumulated heat of the thick film coating could not be conducted away, such that the temperature of the thick film coating keeps rising, and when the temperature is higher than the minimum melting point of the covering layer, the covering layer would begin to melt or even burn, which would destroy the structure of the covering layer or the carrier, thus destroying the thick film elements.


(3) The heat generating rate of the thick film coating and the heat transfer rate of the carrier should satisfy the following formula:









λ
2


A








T
2

-

T
0



d
2



=

c
×

λ
3


A








T
3

-

T
0



d
3




,

0
<
c


10
3


,





if the heat generating rate of the thick film coating is much larger than the heat transfer rate of the carrier, the continuously accumulated heat of the thick film coating could not be conducted away, such that the temperature of the thick film coating keeps rising, and when the temperature is higher than the minimum melting point of the carrier, the carrier would begin to melt or even burn, which would destroy the structure of the carrier, thus destroying the thick film elements.


(4) The heating temperature of the thick film coating could not be higher than the minimum melting point of the covering layer or the carrier, and should meet the requirements: T2<TMinimum melting point of the covering layer and T2<TMinimum melting point of the carrier. Excessively high heating temperature should be avoided to prevent destruction of the thick film elements.


When the above-mentioned requirements are met, the heat transfer rate of the covering layer and the carrier is determined by properties of the material and the thick film element.








λ
3


A








T
3

-

T
0



d
3



,




The formula for calculating the heat transfer rate of the carrier is wherein λ3 represents the heat conductivity coefficient of the carrier, with the unit being W/m·k, and is determined by properties of the materials for preparing the carrier; d3 represents the thickness of the carrier, and is determined by preparation technique and requirements of the thick film elements; T3 represents the surface temperature of the carrier, and is determined by properties of the thick film elements.


The formula for calculating the heat transfer rate of the covering layer is








λ
1


A








T
1

-

T
0



d
1



,





wherein λ1 represents the heat conductivity coefficient of the covering layer, with the unit being W/m·k, and is determined by properties of the material for preparing the covering layer; d1 represents the thickness of the covering layer, and is determined by preparation technique and requirements of the thick film elements; T1 represents the surface temperature of the covering layer, and is determined by properties of the thick film elements.


Preferably, the heat conductivity coefficient of the carrier λ3 is ≥3 W/m·k, the heat conductivity coefficient of the covering layer λ1 is ≤3 W/m·k; wherein 10≤a≤104, 104≤b≤106, 10≤c≤103.


Preferably, the carrier and the thick film coating are bound by printing or sintering; the thick film coating and the covering layer are bound by printing, coating, spraying, sintering, or gluing.


Preferably, as shown in FIG. 1, the region 140 between the carrier 110 and the covering layer 130 without the thick film coating 120 is bound by printing, coating, spraying or sintering, or with gluing.


Preferably, the carrier includes polyimides, organic insulating materials, inorganic insulating materials, ceramics, glass ceramics, quartz, stone materials, fabrics and fiber.


Preferably, the thick film coating is one or more of silver, platinum, palladium, palladium oxide, gold and rare earth materials.


Preferably, the covering layer is made from one or more of polyester, polyimide or polyetherimide (PEI), ceramics, silica gel, asbestos, micarex, fabric and fiber.


Preferably, the area of the thick film coating is smaller than or equal to the area of the covering layer or the carrier.


The present invention also provides a use of the thick film element for coating products with substrate heating.


The beneficial effects of the present invention are as follows:


(1) The coated substrate of the thick film element of the present invention has a high heat conductivity, and is suitable for coating products with substrate heating to improve heat transfer efficiency and reduce heat loss when double-sided heating is not required.


(2) The three-layered structure of the thick film element of the present invention could be directly bound by printing or sintering, and the thick film coating would heat the carrier directly without the need of any medium. Hence, heat could be conducted to the carrier directly, thus improving heat conduction efficiency. Additionally, the covering layer of the present invention is overlaid on the thick film coating, avoiding electric leakage of the thick film coating after given electricity and improving safety performance.


The thick film element of the present invention generates heat by the thick film coating, the thickness range of which is at the micrometer level, and has a uniform heat generating rate and long service lifespan.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 is a schematic cross-sectional view of a thick film element in accordance with the present invention.





DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

The present invention will now be described more specifically with reference to the following embodiments. It is to be noted that the following descriptions of preferred embodiments of this invention are presented herein for purpose of illustration and description only. It is not intended to be exhaustive or to be limited to the precise form disclosed.


Referring to FIG. 1, the present invention discloses a thick film element 100 having a coated substrate with high heat conductivity, which comprises a carrier 110, a thick film coating 120 deposited on the carrier 110 and a covering layer 130 overlaid on the coating 120; the thick film coating 120 is a heating material, and the mode of heating is electrical heating, wherein the carrier 110, the thick film coating 120 and the covering layer 130 are selected from a material that fulfills every of the following equations:









λ
1


A








T
1

-

T
0



d
1



=

a
×

λ
3


A








T
3

-

T
0



d
3




,







λ
2


A








T
2

-

T
0



d
2



=

b
×

λ
1


A








T
1

-

T
0



d
1




,








λ
2


A








T
2

-

T
0



d
2



=

c
×

λ
3


A








T
3

-

T
0



d
3




;








10

a


10
4


,

0
<
b


10
6


,


0
<
c


10
3


;






T2<TMinimum melting point of the covering layer;


T2<TMinimum melting point of the carrier;


T0≤25° C.;


d2≤50 μm;


and d1≥10 μm; 10 μm≤d3≤20 cm;


TMinimum melting point of the carrier>25° C.;


λ3≥λ1.


The following embodiments include 20 thick film elements prepared by the inventors, and the materials for preparing the covering layer, the thick film coating and the carrier of the 20 listed thick film elements all satisfy the equations above. The detailed preparing method and formula are provided as follows:


EMBODIMENTS

Silver paste with a heat conductivity coefficient of λ2 is selected to prepare the thick film coating, polyimides with a heat conductivity coefficient of λ3 is selected to prepare the carrier, and polyimides with a heat conductivity coefficient of λ1 is selected to prepare the covering layer. The three layers are bound by sintering, The area of the prepared thick film coating is A2, the thickness is d2; the area of the covering layer is A1, the thickness is d1; the area of the carrier is A3, the thickness is d3.


Turn on an external DC power supply to charge the thick film coating. The thick film starts to heat up; when the heating is stabled, measure the surface temperature of the covering layer and the carrier, and the heating temperature of the thick film coating under a stable heating state are measured. Heat transfer rate of the covering layer and the carrier, and heat generating rate of the thick film coating are calculated according to the following formula:








λ
1


A








T
1

-

T
0



d
1



,


λ
2


A








T
2

-

T
0



d
2



,


λ
3


A









T
3

-

T
0



d
3


.






Tables 1 to 4 are the 20 thick film elements prepared by the inventors. After provided electricity to heat for 2 minutes, the thick film elements are measured according the national standards to obtain the performance data (heat conductivity coefficient, surface temperature) as shown in the Tables. The thickness, contact area, initial temperature are measured before heating.


The methods to measure the heat conductivity coefficient of the covering layer, the thick film coating and the carrier are as follows:


(1) Switch on the power and adjust the heating voltage to a specific value, then turn on the power switch of the device with 6V power and preheat for 20 minutes;


(2) Conduct zero calibration for the light spot galvanometer;


(3) Calibrate the standard operating voltage of UJ31 potentiometer according to the room temperature, set the commutator switch of the potentiometer to a standard position and adjust the operating current of the potentiometer; As the voltage of standard batteries varies with the temperature, room temperature calibration is calculated by the following formula:

Et=E0−[39.94(t−20)+0.929(t−20)2]; wherein E0=1.0186V.


(4) Place a heating plate and lower thermoelectric couples on the bottom part of a thin test specimen; place upper thermoelectric couples on the upper part of the thin test specimen. It should be noted that the thermoelectric couples must be placed at the central position of the test specimen, and cold sections of the thermoelectric couples must be placed in an ice bottle.


(5) Place the commutator switch of the potentiometer is at position 1, measure the initial temperatures at the upper part and the lower part of the test specimen; proceed only when the temperature difference between the upper part and the lower part is smaller than 0.004 mV (0.1° C.).


(6) Pre-add 0.08 mV to the initial thermoelectric potential of the upper thermoelectric couples, turn on the heating switch to start heating; meanwhile, watch the time with a stopwatch; when the light spot of a light spot galvanometer returns to zero position, turn off the heat source to obtain excess temperature and heating time of the upper part.


(7) Measure the thermoelectric potential of the lower thermoelectric couples after 4-5 minutes to obtain excess temperature and heating time of the lower part.


(8) Place the commutator switch of the potentiometer at position 2, turn on the heating switch to measure the heating current.


(9) End the test, turn off the power and clear up the instrument and equipment.


The temperature is measured by using a thermo-couple thermometer as follows:


(1) Connect thermo-sensing wires to the surfaces of the thick film coating, the carrier, and the covering layer of the heating elements, and the outdoor air.


(2) Provide electricity to the heating product with rated power, and measure the temperatures at all parts.


(3) Record the temperature T0, T1, T2, T3 at all parts of the product at every time interval by a connected computer.


The thickness is measured by using a micrometer and by piling and averaging the values.


The method to measure the melting point is as follows:


The detection instrument: differential scanning calorimeter, model DSC2920, manufactured by TA Instruments (USA). The instrument is qualified (Level A) as verified by Verification Regulation of Thermal Analyzer 014-1996.


(1) Ambient temperature: 20-25° C.; Relative humidity: <80%;


(2) Standard material for instrument calibration: Thermal analysis standard material—Indium; standard melting point 429.7485 K (156.60).


(3) Measuring procedure: referring to “GB/T19466.3-2004/ISO” for the detection procedure.


Repeat the measurement for three times to ensure normal operation of the instrument before sample testing: weight 1-2 ng of the sample, with an accuracy of 0.01 mg, place the sample in an aluminum sample plate. Testing conditions: heat the sample to 200° C. at a rate of 10° C./min, and repeat the measurement for ten times. Measurement model: collect the information of melting points by the computer and instrument, determine the initial extrapolated temperature of the endothermic melting peak by automatic collection of measured data and program analysis of spectra to directly obtain the measurement model. The measurement results are calculated according to the Bessel formula.


Table 1 is the performance data of the covering layers of the thick film elements in Embodiments 1 to 20. The details are as follows:











TABLE 1









Covering Layer














Heat








Conductivity

Surface

Initial



Coefficient
Thickness d1
Temperature
TMinimum melting point of the covering layer
Temperature
Heat Transfer



λ1 (W/m · k)
(μm)
T1 (° C.)
(° C.)
T0 (° C.)
Rate/106

















Embodiment 1
2.3
4000
50
350
25
0.00023


Embodiment 2
2.2
5000
45
350
25
0.0001584


Embodiment 3
2.3
5000
50
350
25
0.000184


Embodiment 4
4.6
5000
53
350
25
0.0005152


Embodiment 5
2.2
6000
46
350
25
0.0001232


Embodiment 6
2
6000
45
350
25
0.000106667


Embodiment 7
1.8
6000
45
350
25
0.000096


Embodiment 8
2.2
8000
48
350
25
0.000107525


Embodiment 9
2.4
8000
45
350
25
0.000096


Embodiment
1.85
10000
45
350
25
0.0000666


10


Embodiment
2.1
10000
50
350
25
0.000084


11


Embodiment
2.12
20000
50
350
25
0.000053


12


Embodiment
2.2
20000
45
350
25
0.0000352


13


Embodiment
2.23
2000
45
350
25
0.0005798


14


Embodiment
2.2
2000
55
350
25
0.000594


15


Embodiment
2.2
12000
55
350
25
0.000143


16


Embodiment
2.23
12000
45
350
25
5.94667E−05


17


Embodiment
2.05
12000
45
350
25
6.83333E−05


18


Embodiment
2.2
7000
50
350
25
0.000125714


19


Embodiment
2.2
7000
50
350
25
9.42857E−05


20









Table 2 is the performance data of the thick film coatings of the thick film elements in Embodiments 1 to 20. The details are as follows:











TABLE 2









Thick Film Coating














Heat








Conductivity


Heating
Initial



Coefficient λ2
Thickness d2

Temperature
Temperature
Heat Generating



(W/m · k)
(μm)
Area A2 (m2)
T2 (° C.)
T0 (° C.)
Rate/106

















Embodiment 1
380
50
0.016
116
25
11.0656


Embodiment 2
320
50
0.018
110
25
9.792


Embodiment 3
380
40
0.016
103
25
11.856


Embodiment 4
380
40
0.02
112
25
16.53


Embodiment 5
380
30
0.016
98
25
14.79466667


Embodiment 6
381
30
0.016
97
25
14.6304


Embodiment 7
381
30
0.016
95
25
14.224


Embodiment 8
381
25
0.017
108
25
21.50364


Embodiment 9
380
25
0.016
97
25
17.5104


Embodiment
380
25
0.018
100
25
20.52


10


Embodiment
380
30
0.016
100
25
15.2


11


Embodiment
380
30
0.02
108
25
21.02666667


12


Embodiment
381
20
0.016
95
25
21.336


13


Embodiment
381
20
0.026
98
25
36.1569


14


Embodiment
381
30
0.018
99
25
16.9164


15


Embodiment
380.5
30
0.026
110
25
28.03016667


16


Embodiment
380.5
35
0.016
103
25
13.56754286


17


Embodiment
380.5
35
0.02
98
25
15.87228571


18


Embodiment
380.5
25
0.016
94
25
16.80288


19


Embodiment
380.5
25
0.012
102
25
14.06328


20









Table 3 is the performance data of the carriers of the thick film elements in Embodiments 1 to 20. The details are as follows:











TABLE 3









Carrier














Heat








Conductivity

Surface

Initial



Coefficient
Thickness d3
Temperature T3
TMinimum melting point of the carrier
Temperature
Heat Transfer



λ3 (W/m · k)
(μm)
(° C.)
(° C.)
T0 (° C.)
Rate/106

















Embodiment 1
7.15
20
105
350
25
0.4576


Embodiment 2
7.15
80
100
350
25
0.12065625


Embodiment 3
7.15
50
90
350
25
0.14872


Embodiment 4
7.16
100
108
350
25
0.118856


Embodiment 5
7.16
20
86
350
25
0.349408


Embodiment 6
7.16
200
90
350
25
0.037232


Embodiment 7
7.21
300
84
350
25
0.022687467


Embodiment 8
7.21
80
90
350
25
0.099588125


Embodiment 9
7.21
20
87
350
25
0.357616


Embodiment
7.18
50
95
350
25
0.180936


10


Embodiment
7.18
50
93
350
25
0.1562368


11


Embodiment
7.18
50
105
350
25
0.22976


12


Embodiment
7.15
30
85
350
25
0.2288


13


Embodiment
7.15
30
88
350
25
0.39039


14


Embodiment
7.15
25
85
350
25
0.30888


15


Embodiment
7.17
25
100
350
25
0.55926


16


Embodiment
7.17
50
94
350
25
0.1583136


17


Embodiment
7.22
50
88
350
25
0.181944


18


Embodiment
7.22
50
91
350
25
0.1524864


19


Embodiment
7.22
45
92
350
25
0.128997333


20









Table 4 is the heat transfer rates calculated according to the performance data listed in Tables 1, 2 and 3. The heat transfer rates of the covering layer, the thick film coating and the carrier are calculated by ratio to obtain the limiting condition of the material of the present invention, namely the following equations:









λ
3


A








T
3

-

T
0



d
3



=

a
×

λ
1


A








T
1

-

T
0



d
1




,







λ
2


A








T
2

-

T
0



d
2



=

b
×

λ
1


A








T
1

-

T
0



d
1




,








λ
2


A








T
2

-

T
0



d
2



=

c
×

λ
3


A








T
3

-

T
0



d
3




;






wherein 10≤a≤104, 0<b≤106, 0<c≤103.

















TABLE 4








Thick Film








Covering
Coating




Layer
Heat
Carrier



Heat Transfer
Generating
Heat Transfer



Satisfy the



Rate
Rate
Rate
a
b
c
Equations?























Embodiment 1
230
11065600
457600
1989.5652
48111.304
24.181818
Yes


Embodiment 2
158.4
9792000
120656.25
761.71875
61818.182
81.156177
Yes


Embodiment 3
184
11856000
148720
808.26087
64434.783
79.72028
Yes


Embodiment 4
515.2
16530000
118856
230.69876
32084.627
139.07586
Yes


Embodiment 5
123.2
14794666.67
349408
2836.1039
120086.58
42.342095
Yes


Embodiment 6
106.6666667
14630400
37232
349.05
137160
392.9523
Yes


Embodiment 7
96
14224000
22687.46667
236.32778
148166.67
626.95409
Yes


Embodiment 8
107.525
21503640
99588.125
926.18577
199987.35
215.92574
Yes


Embodiment 9
96
17510400
357616
3725.1667
182400
48.964252
Yes


Embodiment 10
66.6
20520000
180936
2716.7568
308108.11
113.41027
Yes


Embodiment 11
84
15200000
156236.8
1859.9619
180952.38
97.288219
Yes


Embodiment 12
53
21026666.67
229760
4335.0943
396729.56
91.515785
Yes


Embodiment 13
35.2
21336000
228800
6500
606136.36
93.251748
Yes


Embodiment 14
579.8
36156900
390390
673.31839
62360.987
92.617383
Yes


Embodiment 15
594
16916400
308880
520
28478.788
54.7669
Yes


Embodiment 16
143
28030166.67
559260
3910.9091
196015.15
50.120099
Yes


Embodiment 17
59.46666667
13567542.86
158313.6
2662.2242
228153.75
85.700425
Yes


Embodiment 18
68.33333333
15872285.71
181944
2662.5951
232277.35
87.237203
Yes


Embodiment 19
125.7142857
16802880
152486.4
1212.96
133659.27
110.19265
Yes


Embodiment 20
94.28571429
14063280
128997.3333
1368.1535
149156
109.01993
Yes









The results listed in Table 4 show that the thick films prepared according to Embodiments 1 to 20 all satisfy the equations; and the carrier, i.e. coated substrate, has the function of generating heat and the temperature difference between the two sides are more than 40° C., so as to achieve the function of heat generation. When in use, the product could reduce heat loss when the coated substrate of the thick film element is heated, and the temperature could rise to more than 100° C. after giving electricity for two minutes, which demonstrates that the thick film element of the present invention has high heat generation efficiency.


Tables 5 to 8 are the performance data of the thick film elements in contrasting examples 1 to 10 of the present invention. All the performance data is measured as those shown in Tables 1 to 4. The details are as follows:











TABLE 5









Covering Layer














Heat








Conductivity

Surface

Initial



Coefficient λ1
Thickness d1
Temperature
TMinimum melting point of the covering layer
Temperature
Heat Transfer Rate/



(W/m · k)
(μm)
T1 (° C.)
(° C.)
T0 (° C.)
106

















Contrasting
7.18
25
113
350
25
0.4043776


Example 1


Contrasting
2.2
25
55
350
25
0.14784


Example 2


Contrasting
2.23
25
102
350
25
0.1098944


Example 3


Contrasting
7.17
50
53
350
25
0.2248512


Example 4


Contrasting
7.21
50
97
350
25
0.1661184


Example 5


Contrasting
7.18
75
51
350
25
0.139387733


Example 6


Contrasting
1.8
75
94
350
25
0.026496


Example 7


Contrasting
2.2
75
47
350
25
0.036138667


Example 8


Contrasting
2.4
100
93
350
25
0.026112


Example 9


Contrasting
7.18
100
44
350
25
0.0763952


Example 10


















TABLE 6









Thick Film Coating














Heat








Conductivity


Heating
Initial



Coefficient λ2
Thickness d2

Temperature
Temperature
Heat Generating



(W/m · k)
(μm)
Area A2 (m2)
T2 (° C.)
T0 (° C.)
Rate/106

















Contrasting
382
50
0.016
116
25
11.12384


Example 1


Contrasting
382
50
0.056
56
25
13.26304


Example 2


Contrasting
382
40
0.016
103
25
11.9184


Example 3


Contrasting
382
40
0.056
55
25
16.044


Example 4


Contrasting
382
30
0.016
98
25
14.87253333


Example 5


Contrasting
382
30
0.056
52
25
19.2528


Example 6


Contrasting
382
30
0.016
95
25
14.26133333


Example 7


Contrasting
382
25
0.056
49
25
20.53632


Example 8


Contrasting
382
25
0.016
97
25
17.60256


Example 9


Contrasting
382
25
0.056
46
25
17.96928


Example 10


















TABLE 7









Carrier














Heat








Conductivity

Surface

Initial



Coefficient
Thickness d3
Temperature
TMinimum melting point of the carrier
Temperature
Heat Transfer



λ3 (W/m · k)
(mm)
T3 (° C.)
(° C.)
T0 (° C.)
Rate/103

















Contrasting
7.16
1
105
350
25
9.1648


Example 1


Contrasting
7.16
2
42
350
25
3.40816


Example 2


Contrasting
7.16
4
87
350
25
1.77568


Example 3


Contrasting
7.18
1
43
350
25
7.23744


Example 4


Contrasting
7.18
2
86
350
25
3.50384


Example 5


Contrasting
7.18
1
40
350
25
6.0312


Example 6


Contrasting
7.21
2
84
350
25
3.40312


Example 7


Contrasting
7.21
3
38
350
25
1.749626667


Example 8


Contrasting
7.22
1
87
350
25
7.16224


Example 9


Contrasting
7.22
2
40
350
25
3.0324


Example 10
























TABLE 8








Thick Film








Covering
Coating



Layer
Heat
Carrier



Heat Transfer
Generating
Heat Transfer



Satisfy the



Rate
Rate
Rate
a
b
c
equations?























Contrasting
404377.6
11123840
9164.8
0.022664
27.508546
1213.757
No


Example 1


Contrasting
147840
13263040
3408.16
0.023053
89.712121
3891.5544
No


Example 2


Contrasting
109894.4
11918400
1775.68
0.0161581
108.45321
6712.0202
No


Example 3


Contrasting
224851.2
16044000
7237.44
0.0321877
71.353855
2216.8059
No


Example 4


Contrasting
166118.4
14872533.33
3503.84
0.0210924
89.529717
4244.6383
No


Example 5


Contrasting
139387.7333
19252800
6031.2
0.0432692
138.12406
3192.2006
No


Example 6


Contrasting
26496
14261333.33
3403.12
0.128439
538.24477
4190.6643
No


Example 7


Contrasting
36138.66667
20536320
1749.626667
0.0484143
568.26446
11737.544
No


Example 8


Contrasting
26112
17602560
7162.24
0.2742892
674.11765
2457.6892
No


Example 9


Contrasting
76395.2
17969280
3032.4
0.0396936
235.21478
5925.7618
No


Example 10









Material and structure of the thick film elements in the Contrasting Examples 1 to 10 listed in the above tables neither meet the material selection requirement of the present invention, nor satisfy the equations of the present invention. After given electricity and heat generation, the temperature differences between the two sides of the thick film elements in the Contrasting Examples 1 to 10 are not significantly different, and the heating temperature difference between the covering layer and the carrier is smaller than 15° C. The thick film elements prepared according to such material selections do not meet the requirement of the thick film element having a coated substrate with high heat conductivity of the present invention or meet the product requirement of the present invention, which demonstrates the heat transfer rate and correlation of the present invention.


According to the disclosure and teaching of above-mentioned specification, those skilled in the art of the present invention can still make changes and modifications to above-mentioned embodiment, therefore, the scope of the present invention is not limited to the specific embodiments disclosed and described above, and all those modifications and changes to the present invention are within the scope of the present invention as defined in the appended claims. Besides, although some specific terminologies are used in the specification, it is merely as a clarifying example and shall not be constructed as limiting the scope of the present invention in any way.

Claims
  • 1. A thick film element having a coated substrate with high heat conductivity, comprising: a carrier;a thick film coating deposited on the carrier; anda covering layer overlaid on the coating;wherein the thick film coating is a heating material, and the thick film coating is heated by an electrical heating;wherein the carrier, the thick film coating and the covering layer are selected from a material that fulfills every of following equations:
  • 2. The thick film element according to claim 1, wherein the heat conductivity coefficient λ3 of the carrier is higher than or equal to 3 W/m·k, the heat conductivity coefficient λ1 of the covering layer is smaller than or equal to 3 W/m·k; and 10≤a≤104, 104≤b≤106, 10≤c≤103.
  • 3. The thick film element according to claim 2, wherein an area of the covering layer is larger than an area of the thick film coating, a region between the carrier and the covering layer not having the thick film coating is bound by printing or sintering.
  • 4. The thick film element according to claim 1, wherein the carrier and the thick film coating are bound by printing coating, spraying or sintering, and the thick film coating and the covering layer are bound by printing, sintering, or gluing.
  • 5. The thick film element according to claim 1, wherein an area of the thick film coating is smaller than or equal to an area of the covering layer or an area of the carrier.
  • 6. A method of using a thick film element, comprising the step of: applying the thick film element in a coating product having a single-sided heating substrate, wherein the thick film element has a coated substrate with high heat conductivity and comprises: a carrier; a thick film coating deposited on the carrier; and a covering layer overlaid on the thick film coating, wherein the thick film coating is a heating material, and the thick film coating is heated by an electrical heating, wherein the carrier, the thick film coating and the covering layer are selected from a material that fulfills every of following equations:
  • 7. The method of using the thick film element according to claim 6, wherein the heat conductivity coefficient λ3 of the carrier is higher than or equal to 3 W/m·k, the heat conductivity coefficient λ1 of the covering layer is smaller than or equal to 3 W/m·k; and 10≤a≤104, 104≤b≤106, 10≤c≤103.
  • 8. The method of using the thick film element according to claim 7, wherein an area of the covering layer is larger than an area of the thick film coating, a region between the carrier and the covering layer not having the thick film coating is bound by printing or sintering.
  • 9. The method of using the thick film element according to claim 6, wherein the carrier and the thick film coating are bound by printing coating, spraying or sintering, and the thick film coating and the covering layer are bound by printing, sintering, or gluing.
  • 10. The method of using the thick film element according to claim 6, wherein an area of the thick film coating is smaller than or equal to an area of the covering layer or an area of the carrier.
Priority Claims (1)
Number Date Country Kind
201610075017.2 Feb 2016 CN national
PCT Information
Filing Document Filing Date Country Kind
PCT/CN2016/077439 3/26/2016 WO
Publishing Document Publishing Date Country Kind
WO2017/133067 8/10/2017 WO A
US Referenced Citations (10)
Number Name Date Kind
5068517 Tsuyuki Nov 1991 A
5705793 Kitaichi et al. Jan 1998 A
20020158328 Hiramatsu et al. Oct 2002 A1
20090008142 Shimizu Jan 2009 A1
20090199994 Amano Aug 2009 A1
20140332518 Lesmeister Nov 2014 A1
20150163862 Chabach Jun 2015 A1
20150373782 Kang Dec 2015 A1
20160249413 Lim Aug 2016 A1
20160270152 Duce Sep 2016 A1
Foreign Referenced Citations (6)
Number Date Country
1320010 Oct 2001 CN
201936869 Aug 2011 CN
103546998 Jan 2014 CN
104395143 Mar 2015 CN
104425053 Mar 2015 CN
2004022485 Jan 2004 JP
Non-Patent Literature Citations (1)
Entry
https://www.physicsclassroom.com/Class/thermalP/u18l1f.cfm, Henderson, Tom (Year: 1996).
Related Publications (1)
Number Date Country
20180332667 A1 Nov 2018 US