Irradiation of graphite impregnated with furfuryl alcohol

Irradiation of graphite impregnated with furfuryl alcohol

543 CARBON Carbon 1966.Vol. 3. Printed in Great Britain. Irradiationof Graphite Impregnated with Furfiuyl Alcohol* (Received 14 December 1964; in re...

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543

CARBON Carbon 1966.Vol. 3. Printed in Great Britain.

Irradiationof Graphite Impregnated with Furfiuyl Alcohol* (Received 14 December 1964; in revised form24 November 1965) DIMENSIONAL changes induced by fast neutrons in graphite impregnated with furfuryl alcohol are reported in this note. The impregnation treatment is a process used to reduce the gas permeability of commercial graphite.(*) The process is based on introducing a thermosettingmonomer into the pores of the graphite, solidifying it by heating, and finally decomposing it to a carbon residue by further heating. This series is termed an “impregnation cycle” and is repeated a number of times until the desired permeability is obtained. A final heat treatment at greater than 2650°C is usually made. The monomer used in the work reported here was a mixture of ten moles of furfuryl alcohol to one mole of maleic anhydride. Theresiduewascarbonixed and heat-treated independent of the base stock and was shown, by conventional X-ray methods, to be a nongraphitixing carbon.

‘This work was supported by the U.S. Atomic Energy Commission under Contract AT(O4-3)-167, Project Agreement No. 12.

Figure 1 shows the effects of a series of impregnations on the pore structure of a commercial graphite. The den&y of the graphite ranged from 1.75 to 1.85 g/cm*, and the impregnation process raised this value by 4-7 %, depending on the carbon pickup. The irradiation experiments were carried out in a series of capsules in the core of the General Electric Test Reactor (GETR). The average irradiation temperatures were estimated by comparing the dimensional contractions of several samples of a reference needle coke graphite (NPR) with the contractions of a set of samples from the same material that were irradiated in an instrumented capsule.(*) Fast neutron exposures were calculated from fast flux data supplied by the Physics Group at the GETR. The irradiation data are shown in Tables 1 and 2. The HLM-85 base stock and impregnated material both appear to be more isotropic than the needle coke graphite on the basis of the contraction data from Capsule Experiments 311-9, 10 and 11. The dimensional stability was affected only slightly, if at all, by the 4-7 % increase in density in the impregnated carbon. After a short irradiation at 450” or 75O”C, little difference in dimensional stability was observed among the two corn-, mercially impregnated graphites (UC and HLM-85) and a conventional needle coke graphite (NPR). Thermal. expansion changes were noted in the samples which were cut perpendicular to extrusion but not in the samples cut parallel to extrusion.

-BASE STOCK 0 ONE IMPREGNATION TO 4 X 10-2CM2/SEC

0

. 0 0 l

THREE IMPREGNATIONS TO 2X 10-3CM2/SEC GRAPHlTlZATlON OFABOVE TO 4 X 10-3CM2/SEC FOURTH IMPREGNATION TO 4X IO-*CM2/SEC FIFTH IMPREGNATION TO 7XIO-5 CM2/SEC GRAPHITIZATION OF ABOVE TO IX IO-* CM2/SEC

0

-J 0.01

I .o

0.1 PORE

FIG. 1. Effect of five impregnation

DIAMETER

10.0

100

(+I

cycles on pore structure stock.

of commercial

graphite base

LETTERS

544

TO

THE

EDITOR

TABJX 1. DIMENBIONAL CHANGBS Irradiation Sample and treatment Temp.

(‘C)

conditions

Dimensional change,

Exposure, nvt X 10-‘I, E~0.18 MeV

M/L Parallel to extrusion

( %) Perpendicular to extrusion

HLM-85,

base stock

625-775

0.7

+0.12

+0.06

HLM-8.5,

impregnated

3 times

62.5-775

0.7

-0.10*0.02

-0.05

HLM-85,

impregnated

4 times

-0.10

+0.13

625-775

0.7

NPR, needle coke

62.5-775

0.7

HLM-85.

base stock

450-800

4

HLM-85,

impregnated

3 times

450-800

HLM-85,

impregnated

4 times

450-800

NPR, needle coke HLM-85,

base stock

HLM-85,

impregnated

HLM-85,

impregnated

HLM-85,

impregnated

311-9 *to.05

311-9 311-9

-0.04

311-9

-0.96

-0.36

311-10

4

-0.98

&O.OOS -0.25

4

-1.22

-0.54

311-10

450-800

4

-1.59

-0.49

31110

575-700

4

-0.91

-0.64

311-11

3 times

575-700

4

-0.92

-0.64*o.a2

31111

4 times

575-700

4

-0.90

-0.67

311-11

575-700

4

-1.04

-0.65

425-475

1

-0.22jro.02

-0.22

NPR, needle coke 5 times

0.00

Capsule experiment number

&to.07

f0.005

311-10

311-11 fO.02

311-7

UC, impregnated

425-475

1

-0.34*0.00

-0.28*0.06

311-7

NPR, needle coke

425-475

1

-0.22*0.05

-0.191to.01

311-7

675-800

1

-0.12*0.01

-0.08~0.02

311-8

UC, impregnated

675-800

1

-0.09~0.01

+0.01

311-8

NPR, needle coke

675-800

1

-0.03

+0.07*0.19

HLM-IS,

impregnated

5 times

f0.02

f0.08

311-8

TABLE 2. THQWAL EXPANSION Irradiation

Thermal expansion coefficient “C x lo@, RT” to lOOO=C

conditions

Sample and treatment Temp.

CC)

HLM-85,

impregnated

-

HLM-85,

impregnated

425-475

HLM-85,

impregnated

HLM-85,

base stock

4.50-800 -

HLM-85,

base stock

450-800

HLM-85,

base stock

450-800

Exposure,

E>O.l8

nvt X 10-*I, MeV

Parallel to extrusion

1 1

Perpendicular to extrusion

-

3.47

-

4.25

-

4.00

2.87

4.04

1

2.80

4.21

1

2.91

4.41

-

lRT = room temperature. REFERENCES TULLY G. R., JR.,and DIBSBLHOR~TB. F., A Process for making graphite less permeable to gases at high Report GA-2318. temperatures, p. 91, USAEC General Atomic Division, General Dynamics Corporation (February 1963). HXLM J. W., The H-4, H-5, and H-6 irradiation graphiteexperiments : irradiation of N-reactor Interim report No. 1, p. 99, USAEC Report HW81250A, Hanford Atomic Products Operation (October 1964).

General AtwmksDivision General Qvnamics Corporation John JAY H@ki~~~~toty for

Purr

&Jn D@J,

and

Applied Science

Cariforn~

G. B. ENGL~ B. F. DI~BBLHOXJJT G. R. TJJLLY Jr. w. P. WALLACE