Abstract:A new class of lightweight carbon fiber reinforced plastic (CFRP)-the lightweight ablator series for transfer vehicle systems (LATS)-has recently been developed. The LATS is fabricated by heating and pressurizing a material in which resin is impregnated in the laminated carbon fiber felt. A characteristic required to ensure the excellence of a conventional lightweight CFRP ablator of the LATS is the simplicity of the resin impregnation process. Since dried bulk density can be easily controlled, this manufactur… Show more
“…The char density for each ablator model is calculated by means of the following relation based on the measurement of virgin and charred materials. 7) 7 . 0 v ch (7) The emissivity of the char surface was set to be 0.85.…”
Section: Arc-heated Testmentioning
confidence: 99%
“…7) 7 . 0 v ch (7) The emissivity of the char surface was set to be 0.85. 8,12) The reference value of thermal conductivity of the virgin material kvref is constructed of the measured value of the LATS materials with the density of about 300 kg/m 3 , using a steady-state method with the temperature range from room temperature (RT) to 573 K (300 o C), combined with the literature data 4) of the low density (about 300 kg/m 3 ) ablator (PICA) multiplied by a constant value, C*kvPICA(T), where kvPICA(T) is the thermal conductivity of the PICA and C is a constant value that is determined so that the two data are smoothly connected.…”
Section: Arc-heated Testmentioning
confidence: 99%
“…Recently, a lightweight ablator named LATS (Lightweight Ablator series for Transfer vehicle Systems) with the densities of about 300-700kg/m 3 has been developed. 6,7) The LATS is a carbon phenolic ablator fabricated by impregnating a phenolic resin into a felt made of carbon fibers. The material properties of the LATS ablator were measured and arc-heated tests of the ablator samples with various densities were carried out.…”
The effects of density, thickness and heat load upon the heat shield performance of the lightweight phenolic carbon ablators named LATS (Lightweight Ablator series for Transfer vehicle Systems) were examined quantitatively for both arc-heated test and re-entry heating conditions using a one-dimensional ablation analysis code. Thermal conductivity values of the ablator were tuned based on the arc-heated test results by matching the calculated temperatures to the measured data. Main findings are: (1) For both heating conditions, the heat shielding performance of the ablator has the same tendencies with respect to parameters of the ablator density, thickness and heat load.(2) The dependency of the back surface temperature upon the ablator density is small especially for a large ablator thickness. (3) The surface recession decreases with the increase of the density. However, the mass loss increases almost linearly with the increase of the density. (4) The ablator necessary thickness, with which the maximum back surface temperature equals to the pre-determined allowable temperature value, is nearly constant as the density changes. The ablator necessary mass increases almost linearly, with the increase of the density. (5) In considering the mechanism of nearly equal necessary thickness of the ablator, it is very important that the thermal diffusivity does not vary much with different densities of the LATS ablator. (6) From the point of the reduction of the ablator weight, the selection of a lower density ablator is more advantageous than that of a higher density ablator.
“…The char density for each ablator model is calculated by means of the following relation based on the measurement of virgin and charred materials. 7) 7 . 0 v ch (7) The emissivity of the char surface was set to be 0.85.…”
Section: Arc-heated Testmentioning
confidence: 99%
“…7) 7 . 0 v ch (7) The emissivity of the char surface was set to be 0.85. 8,12) The reference value of thermal conductivity of the virgin material kvref is constructed of the measured value of the LATS materials with the density of about 300 kg/m 3 , using a steady-state method with the temperature range from room temperature (RT) to 573 K (300 o C), combined with the literature data 4) of the low density (about 300 kg/m 3 ) ablator (PICA) multiplied by a constant value, C*kvPICA(T), where kvPICA(T) is the thermal conductivity of the PICA and C is a constant value that is determined so that the two data are smoothly connected.…”
Section: Arc-heated Testmentioning
confidence: 99%
“…Recently, a lightweight ablator named LATS (Lightweight Ablator series for Transfer vehicle Systems) with the densities of about 300-700kg/m 3 has been developed. 6,7) The LATS is a carbon phenolic ablator fabricated by impregnating a phenolic resin into a felt made of carbon fibers. The material properties of the LATS ablator were measured and arc-heated tests of the ablator samples with various densities were carried out.…”
The effects of density, thickness and heat load upon the heat shield performance of the lightweight phenolic carbon ablators named LATS (Lightweight Ablator series for Transfer vehicle Systems) were examined quantitatively for both arc-heated test and re-entry heating conditions using a one-dimensional ablation analysis code. Thermal conductivity values of the ablator were tuned based on the arc-heated test results by matching the calculated temperatures to the measured data. Main findings are: (1) For both heating conditions, the heat shielding performance of the ablator has the same tendencies with respect to parameters of the ablator density, thickness and heat load.(2) The dependency of the back surface temperature upon the ablator density is small especially for a large ablator thickness. (3) The surface recession decreases with the increase of the density. However, the mass loss increases almost linearly with the increase of the density. (4) The ablator necessary thickness, with which the maximum back surface temperature equals to the pre-determined allowable temperature value, is nearly constant as the density changes. The ablator necessary mass increases almost linearly, with the increase of the density. (5) In considering the mechanism of nearly equal necessary thickness of the ablator, it is very important that the thermal diffusivity does not vary much with different densities of the LATS ablator. (6) From the point of the reduction of the ablator weight, the selection of a lower density ablator is more advantageous than that of a higher density ablator.
“…The material properties of the LATS ablator were measured and arc-heated tests of the ablator samples with various densities were carried out. 9,10) Ablation analysis with respect to the arc-heated tests was also carried out using a onedimensional analysis code and the measured and calculation results agreed well. 10,11) Investigations concerning the effects of heat load and ablator density upon the necessary thickness tne and necessary mass mne of the LATS ablator were carried out using a one-dimensional ablation analysis code.…”
Section: Introductionmentioning
confidence: 99%
“…9) The LATS is a carbon phenolic ablator fabricated by impregnating a phenolic resin into a felt made of carbon fibers. The material properties of the LATS ablator were measured and arc-heated tests of the ablator samples with various densities were carried out.…”
The effects of heat load, ablator density, and backup structure, etc. upon the heat shield performance of the lightweight phenolic carbon ablators named LATS were investigated using a one-dimensional ablation analysis code. The ablator density was assumed to be from about 260 to 1000kg/m 3 . Heat flux time histories of a rectangular pattern were assumed, where cases of constant heating duration time and constant accumulated heat load (up to 600MJ/m 2 ) were considered. The heating level was assumed to be from 1 to 10MW/m 2 , which means that the ablator surface is in the region of diffusion control oxidation/sublimation. The materials of the backup wall are assumed to be aluminum, stainless steel and high density CFRP. Main findings are: (1) For a low heat flux q with the same heating duration time tq, the necessary thickness, with which the maximum back surface temperature equals to the pre-determined allowable temperature, is nearly constant as the density v changes. On the other hand, the necessary thickness increases largely when q is larger and v is smaller. The ablator necessary mass increases with the increase of v and q for the same tq.
In this study, carbon aerogel based lightweight composite ablators (CALCAs) with different densities and microstructures were prepared using the vacuum impregnation method. The mechanical strength and morphology of CALCAs were investigated. Ablation-insulation performance of the samples was also evaluated by an oxyacetylene flame test with a constant heating rate of 2.5 MW/m 2 . Moreover, the structural evolution during the ablation was studied and the ablation mechanism of CALCAs was proposed. The porous insulators showed good compressive strength (3.2-9 MPa) and low thermal conductivity (lower than 0.35 W/mK). Besides the tunable density, the low recession rate (as low as 0.117 mm/s), and good ablation-insulation performance (175 C at 25 mm and 125 at 35 mm in-depth), these lightweight porous heat shielding composites are promising candidates to use as the thermal protection systems for aerospace applications.
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