Table 10. Mold size and dimensions of tamping rods for the particle index test. (After ASTM
D 3398-93.)
Aggregate
Aggregate size
specimen
Mold
Mold
Rod
Rod
Mass of
(mm)
Mold/Rod
size
diameter
height
diameter
length
rod
Passing Retained
designation
(kg)
(mm)
(mm)
(mm)
(mm)
(g)
203.2 0.2
237.0 0.2
21.2 0.2
814 0.2
2204 10
38.1
25.4
A
13.6
152.4 0.2
177.8 0.2
15.9 0.2
610 0.2
930 10
25.4
19.0
B
13.0
152.4 0.2
177.8 0.2
15.9 0.2
610 0.2
930 10
19.0
12.7
B
13.0
101.6 0.2
118.5 0.2
10.6 0.2
406.9 0.2
276 3
12.7
9.5
C
4.0
101.6 0.2
118.5 0.2
10.6 0.2
406.9 0.2
276 3
9.5
4.75
C
4.0
Huang (1965) modified the test method to
Bindra and Al-Sanad (1983) conducted tests on
measure the actual volume of the compacted
aggregates that ranged from natural aggregates to
aggregate mass. This involved a special device
blast furnace slags. They also looked at the effect of
called a volumeter, which fitted exactly over the
different gradations (open graded to dense graded)
mold. The volumeter was made up of a bottom
and concluded from their study that gradation did
thin flexible membrane and a standpipe. The pro-
not affect the weighted particle index value. It
cedure for compacting the sample remained the
should be noted that the gradation study included
same, except that at the end of the last layer, a
both the coarse and fine fractions. The weighted
flexible membrane was placed on top of the sur-
particle index for a given gradation is the weighted
face and water was poured through the stand-
mean of the percent retained in each sieve multi-
pipe to a prescribed height. The idea here is that
plied by the particle index for that size. The proce-
when water is introduced on top of the mem-
dure for determining the weighted particle index is
brane, the thin membrane will deform to match
presented in ASTM D 3398 (1996). Bindra and Al-
the surface. Knowing the volume of the mold and
Sanad (1983) also concluded from their study that
the volume of water in the volumeter, the actual
the particle index for smooth-surfaced, rounded
volume of the aggregate mass is calculated. Using
aggregates averaged around 6.5, and for crushed,
this method for volume measurement, more re-
high angularity, rough-textured aggregates, the av-
producible results were obtained (Huang 1965).
erage was around 17.5.
In addition to modifying the method for measur-
They also proposed a new method for calculat-
ing the volume of the compacted aggregates,
ing the volume of the aggregate mass in the mold.
Huang modified the test to determine particle in-
Instead of using the volumeter device developed
dex of fine aggregates (passing #4 and retained
by Huang (1965), they proposed a sand replace-
on the #200 sieve).
ment technique. This method involves placement
Bindra and Al-Sanad (1983) modified the par-
of a thin flexible membrane on top of the aggregate
ticle index test to test coarse aggregates up to 50-
surface. Sand (passing the #25 and retained on the
mm maximum size in their study. In this case,
#50 sieve) is then poured onto the surface of the
coarse aggregates are designated as any material
membrane to the top of the mold. The net weight of
larger than 2.36 mm (#8 sieve). The test method is
sand required to fill to the rim of the mold is ob-
similar to the procedure developed by Huang
tained and the volume to fill the mold is obtained.
(1965) with several exceptions. The mold used is
The volume of the compacted aggregate mass is the
cylindrical in shape and the dimensions and
difference between the volume of the mold and the
weight of the mold and tamping rod sizes are dif-
volume of sand required to fill the mold. This
method appears to be easier and less cumbersome
ferent. Details on the dimensions and weights of
than the volumeter method.
the mold and tamping rods are shown in Table 11.
Table 11. Dimensions of mold and tamping rods. (After
Bindra and Al-Sanad 1983.)
Inside
Inside
Diameter of
Length of
Weight of
Aggregate
diameter
height
tamping
tamping
tamping
size
of mold
of mold
rod
rod
rod
(mm)
(mm)
(mm)
(mm)
(mm)
(g)
2050
250.0
291.6
26.00
1045
4120
2.3620
152.4
177.8
15.88
610
930
12