NJC
Paper
2
.5 Characterisation
indication of the mechanical property of the shale, were deter-
mined according to the following equation:
The apparent viscosities of copolymer solutions were measured
with a Brookfield DV-III + Pro viscometer (Brookfield, USA).
FT-IR spectra were measured with KBr pellets using a WQF-520
Fourier transform infrared spectrometer (Beijing Rayleigh
Analytical Instrument Corporation, China) in the optical range
3
FM ꢂ 10
IH ¼
ꢂ 100%
(2)
A
where the indentation hardness (IH) value is an indication of the
mechanical property of the shale (MPa), FM is the maximum
load before the rock is broken (kN), and A is the contact area
ꢀ1
1
13
of 400–4000 cm by averaging 32 scans. H NMR and C NMR
spectra were recorded by a Bruker AV III-400 NMR spectrometer
2
2
(
mm ). Here, A is 4.446 mm .
(Bruker, Switzerland) in D O and CDCl . Copolymer intrinsic
2 3
viscosity was measured by an Ubbelohde viscometer (Shanghai
Sikeda Scientific Instruments Incorporation, China) at 30 ꢁ
3
. Results and discussion
0.1 1C.
3.1 Synthesis of PAAT
2
.6 X-ray diffractometry (XRD)
The effects of the synthetic conditions on the copolymerisation of
AM, AA and TCDAP were investigated, and the intrinsic viscosity
and the viscosity-average molecular weight were measured. The
results are listed in Table 1 (for details, see Tables S1, S2 and Fig. S1
in ESI†). The structure of PAAT was characterised by FT-IR and
The hybrid MMT mixtures were prepared by adding 0.5 g MMT
to 1 g samples (KCl, ILs, PAAT and PAAT–ILs complex solutions)
at different concentrations. The hybrid mixture suspensions
were kept wet for 2 h. A part of the hybrid MMT mixtures was tested
directly by XRD, and others were dried to constant weight at 40 1C
in vacuum and then tested by XRD. The d-spacing of MMT was
investigated by small-angle XRD diffractometry (X’Pert PRO MPD
1
H NMR spectroscopy, and the results are presented in Fig. 2. The
stretching vibration peaks of –NH– and the CQO bond in the
ꢀ
1
ꢀ1
amide groups appeared at 3435.64 cm
and 1675.85 cm
,
ꢀ1
ꢀ1
respectively. The peaks at 1173.49 cm and 1049.28 cm corre-
(PANalytical B.V., Netherlands)) with a Cu Ka radiation target at
ꢀ1
spond to the stretching vibration of –SO –, suggesting the success-
2
4
0 mA and 40 kV. The scan rate was 1 deg min , the step size
ful copolymerisation of TCDAP monomer. The distinct peaks
around 1.54 ppm and 2.03–2.15 ppm can be assigned to the
was 0.05 degrees, and the scattering angle (2y) ranged from 2 to 8
degrees.
–
CH
at 3.74 ppm is due to the proton of –CH
shift value at 2.49 ppm is attributable to the –CH
Ar–CH in TCDAP, while the peaks at 7.42 ppm and 7.71 ppm,
2
– and –CH– in the polymeric chain, respectively. The peak
–N–CH –. The chemical
protons of
2
.7 Anti-swelling ratio test
2
2
3
Bentonite, which was mainly composed of Na-MMT, was used
due to its remarkable hydration in water. First, 0.5 g bentonite
was soaked in 10 mL sample solution for 2 h at room temperature.
Subsequently, the bentonite phase and the solution phase were
separated by a YuHua model TG-16 supercentrifuge (YuHua
Company, China) at 1500 r min for 15 min. The anti-swelling
ratio of bentonite was then calculated according to the following
equation:
–
3
denoted as d and e in Fig. 2(b), respectively, are attributable
to the protons of the benzene rings. These results verify the
successful preparation of the copolymer PAAT.
ꢀ
1
3.2 Effect of different PAAT–ILs on d-spacing of Na-MMT
The swelling inhibitions of different PAAT–ILs complexes were
investigated by comparing the d-spacing of MMT compared
with water–ILs (see Table S3 and Fig. S2, ESI†). It was found in
our previous works that polymer solutions slightly affected the
d-spacing of Na-MMT with the increasing concentration of
V2 ꢀ V1
B ¼
ꢂ 100%
(1)
V2 ꢀ V0
where B is the anti-swelling ratio (%), V is the volume of swollen
bentonite in distilled water (mL), V is the volume of swollen
bentonite in kerosene (mL), and V is the volume of swollen
bentonite in the sample solution (mL).
29
2
polymer solution. The d-spacing data of MMT in PAAT–ILs
0
are summarised in Table S3 (ESI†). The results indicated that
compared with water–KCl and water–ILs, the PAAT–ILs exhibited
1
significant anti-swelling capacities; for instance, the PAAT–HmimBF
complex resulted in a the smaller d-spacing of 13.16 Å. In addition,
PAAT–ILs with short chain substituents (HmimBF , emimBF
4
2
.8 Temperature resistance test
4
4
The effect of temperature on the apparent viscosities of sample
solutions was tested by using a Haake RS 600 rotational
rheometer (Haake, Germany) at a steady shear rate of 170 s
and AllymimBF ) exhibited excellent clay inhibition of MMT. The
4
d-spacing of MMT enlarged with increasing number of alkyl
Table 1 The optimum synthetic conditions and characteristics of PAAT
ꢀ
1
to simulate injection rates in the range of 30–130 1C.
2
.9 Indentation hardness measurement
Apparenat
Intrinsicb
Molecular
weight
ꢀ1
b
The indentation hardnesses of shale cores were studied by soaking Sample
viscosity (mPa s)
viscosity (mL g
)
6
the cores in solutions of the different samples at 80 1C for 24 h. The
core strength data of the shale were measured with an RTR-1000
rapid triaxial rock testing system (GCTS, USA) in comparison to
PAAT
352.6
1372.00
6.70 ꢂ 10
a
b
The concentration of copolymer was 1 wt%. The intrinsic viscosity
and viscosity-average molecular weight were determined according to
deionised water and KCl. The indentation hardness (IH) values, an ref. 26–28.
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New J. Chem.