Lecture 1

NPTEL- Advanced Geotechnical Engineering

Dept. of Civil Engg. Indian Institute of Technology, Kanpur 1

Module 1

SOIL AGGREGATE (Lectures 1 to 4)

Topics

1.1 INTRODUCTION

1.2 WEIGHT – VOLUME RELATIONSHIP

1.2.1 Basic Definitions

1.2.2 General Range of Void Ratio and dry Unit Weight Encountered in

Granular Soil

1.2.3 Relative Density and Relative Compaction

1.3 CLAY MINERALS 1.3.1 Composition and Structure of Clay Minerals

1.3.2 Specific Surface of Clay Minerals

1.3.3 Cat ions Exchange Capacity

1.3.4 Nature of Water in Clay

1.3.5 Flocculation and Dispersion of Clay Particles

1.4 CONSISTENCY OF COHESIVE SOILS 1.4.1 Atterberg Limits

1.4.2 Liquidity Index

1.4.3 Activity

1.5 SOIL CLASSIFICATION 1.5.1 Unified Soil Classification System

1.5.2 Theory of Compaction and Proctor Compaction Test

1.5.3 Harvard Miniature Compaction Device

1.5.4 Effect of Organic Content on Compaction of Soil

1.6 EFFECTIVE STRESS 1.6.1 Effective Stress Concept in Saturated Soils

1.6.2 Critical Hydraulic Gradient and Boiling

PROBLEMS

REFERENCES



Chapter 1

Lecture 1

Soil Aggregate -1

Topics

1.1 INTRODUCTION



1.2.2 General Range of Void Ratio and dry Unit Weight Encountered in

Granular Soil


1.1 INTRODUCTION Soils are aggregates of mineral particles, and together with air and/or water in the void spaces they form

three-phase systems. A large portion of the earth’s surface is covered by soils, and they are widely used as

construction and foundation materials. Soil mechanics is the branch of engineering that deals with the

engineering properties of soil and its behavior under stresses and strains.



Figure 1a shows a soil mass that has a total volume V and a total weight, W. to develop the weight-volume

relationships, the three phases of the soil mass, i.e., soil solids, air, and water, have been separated in figure

1b.

Figure 1 Weight-volume relationships for soil aggregate



𝑤 = 𝑊𝑠 + 𝑊𝑤 (1.1)

And, also,

𝑉 = 𝑉𝑠 + 𝑉𝑠 + 𝑉𝑎 (1.2)

𝑉𝑢 = 𝑉𝑤 + 𝑉𝑎 (1.3)

Where

𝑊𝑠 = weight of soil solids

𝑊𝑤 = weight of water

𝑉𝑠 = volume of the soil solids

𝑉𝑤 = volume of water

𝑉𝑎 = volume of air

The weight of air is assumed to be zero. The volume relations commonly used in soil mechanics are void

ratio, porosity, ad degree of saturation.

Void ratio e defined as the ratio of the volume of voids to the volume of solids:

𝑒 =𝑉𝑢

𝑉𝑠 (1.4)

Porosity n is defined as the ratio of the volume of voids to the total volume:

𝑛 =𝑉𝑢

𝑉 (1.5)

Also, 𝑉 = 𝑉𝑠 + 𝑉𝑢

And so

𝑛 =𝑉𝑢

𝑉𝑠+𝑉𝑢=

𝑉𝑢 /𝑉𝑠

𝑉𝑠+/𝑉𝑠 +𝑉𝑢 /𝑉𝑠=

𝑒

1+𝑒 (1.6)

Degree of saturation 𝑆𝑟 is the ratio of the volume of water to the volume of voids and is generally expressed

as a percentage:

𝑆𝑟 % =𝑉𝑤

𝑉𝑤× 100

The weight relations used are moisture content and unit weight. Moisture content w is defined as the ratio of

the weight of water to the weight of water to the weight of soil solids, generally expressed as a percentage:

𝑤 % =𝑊𝑊

𝑊𝑠× 100 (1.8)

Unit weight 𝛾 is the ratio of the total weight to the total volume of the soil aggregate:



𝛾 =𝑊

𝑉 (1.9)

This is sometimes referred to as moist unit weight since it includes the weight of water and the soil solids. If

the entire void space is filled with water ((i.e., 𝑉𝑎 = 0), it is a saturated soil; Eq. (1.9) will then give use the

saturated unit weight 𝛾𝑠𝑎𝑡 .

The dry unit weight 𝛾𝑑 is defined as the ratio of the weight of soil solids to the total volume:

𝛾𝑑 =𝑊𝑠

𝑉 (1.10)

Useful weight-volume relations can be developed by considering a soil mass is which the volume of soil

solids is unity, as shown in figure 1.2. Since 𝑉𝑠 = 1, from the definition of void ratio given in Eq. (1.4) the

volume of voids is equal to the void ratio, e. the weight of soil solids can be given by

𝑊𝑠 = 𝐺𝑠𝛾𝑤𝑉𝑠 = 𝐺𝑠𝛾𝑤 (𝑠𝑖𝑛𝑐𝑒 𝑉𝑠 = 1)

Where 𝐺𝑠 is the specific gravity of soil solids, and 𝛾𝑤 is the unit weight of water (62.4𝑙𝑏/𝑓𝑡3 , 𝑜𝑟 9.81 𝑘𝑁/𝑚3).

From Eq. (1.8), the weight of water is𝑊𝑤 = 𝑤𝑊𝑠 = 𝑤𝐺𝑠𝛾𝑤 . So the moist unit weight is

𝛾 =𝑊

𝑉=

𝑊𝑠+𝑊𝑤

𝑉𝑠+𝑉𝑢=

𝐺𝑠𝛾𝑤 +𝑤𝐺𝑠𝛾𝑤

1+𝑒=

𝐺𝑠𝛾𝑤 (1+𝑤)

1+𝑒 (1.11)

The dry unit weight can also be determined from figure 1.2 as

Figure 1.2 Weight-volume relations for 𝑉𝑠 = 1



𝛾𝑑 =𝑊𝑠

𝑉=

𝐺𝑠𝛾𝑤

1+𝑒 (1.12)

The degree of saturation can be given by

𝑆𝑟 =𝑉𝑤

𝑉𝑢=

𝑊𝑤 /𝛾𝑤

𝑉𝑢=

𝑤𝐺𝑠𝛾𝑤 /𝛾𝑤

𝑒=

𝑤𝐺𝑠

𝑒 (1.13)

For saturated soils, 𝑆𝑟 = 1. So, from Eq. (1.13),

𝑒 = 𝑤𝐺𝑠 (1.14)

By referring to Figure 1.3, the relation for the unit weight of a saturated soil can be obtained as

𝛾𝑠𝑎𝑡 =𝑊

𝑉=

𝑊𝑠+𝑊𝑤

𝑉=

𝐺𝑠𝛾𝑤 +𝑒𝛾𝑤

1+𝑒 (1.15)

Basic relations for unit weight such as Eqs. (1.11), (1.12), and (1.15) in terms of porosity n can also be

derived by considering a soil mass that has a total volume of unity as shown in figure. 1.4. In this case (for

V=1), from Eq. (1.5) 𝑉𝑢 = 𝑛, So, 𝑉𝑠 = 𝑉 − 𝑉𝑢 = 1 − 𝑛

Figure 1.3 Weight-volume relation for saturated soil with 𝑉𝑠 = 1



The weight of soil solids is equal to (1 − 𝑛)𝐺𝑠𝛾𝑤 , and the weight of water

𝑊𝑤 = 𝑤𝑊𝑠 = 𝑤(1 − 𝑛)𝐺𝑠𝛾𝑤 . Thus the moist unit weight is

𝛾 =𝑊

𝑉=

𝑊𝑠+𝑊𝑤

𝑉=

1−𝑛 𝐺𝑠𝛾𝑤 +𝑤(1−𝑛)𝐺𝑠𝛾𝑤

1

= 𝐺𝑠𝛾𝑤 1 − 𝑛 (1 + 𝑤) (1.16)

The dry unit weight is

𝛾𝑑 =𝑊𝑠

𝑉= (1 − 𝑛)𝐺𝑠𝛾𝑤 (1.17)

If the soil is saturated (figure 1.5).

𝛾𝑠𝑎𝑡 =𝑊𝑠+𝑊𝑤

𝑉= 1 − 𝑛 𝐺𝑠𝛾𝑤 + 𝑛𝛾𝑤 = 𝐺𝑠 − 𝑛(𝐺𝑠 − 𝑛) 𝛾𝑤 (1.18)

Figure 1.4 Weight-volume relation with 𝑉 = 1



Several other functional relationships are given in Table 1.1

Table 1.1 Functional relationships of various soil properties for saturated soils

Jumikis, A.R., Soil Mechanics, 1962, pp. 90-91, D. Van Nostrand Company, Inc., Princeton, New Jersy

Sought quantities Quantities

𝛾𝑤 and:

Specific

gravity 𝐺𝑠

Dry unit weight

𝛾𝑑

Saturated unit

weight 𝛾𝑠𝑎𝑡

Saturated

moisture

content, %

Porosity n Void ratio e

𝐺𝑠: 𝛾𝑑 1 −

1

𝐺𝑠

𝛾𝑑 + 𝛾𝑤 1

𝛾𝑑

−1

𝐺𝑠 𝛾𝑑

𝛾𝑑 1 −𝛾𝑑

𝐺𝑠 𝛾𝑑

𝐺𝑠 𝛾𝑑

𝛾𝑑

− 1

𝐺𝑠: 𝛾𝑠𝑎𝑡 𝛾𝑠𝑎𝑡 − 𝛾𝑤

𝐺𝑠 − 1𝐺𝑠

𝐺𝑠𝛾𝑤 − 𝛾𝑠𝑎𝑡

(𝛾𝑠𝑎𝑡 − 𝛾𝑤 )𝐺𝑠


(𝐺𝑠 − 1)𝐺𝑠


𝛾𝑠𝑎𝑡 − 𝛾𝑤

𝐺𝑠: 𝑤 𝐺𝑠

1 + 𝑤𝐺𝑠

𝛾𝑤 1 + 𝑤

1 + 𝑤𝐺𝑠

𝐺𝑠𝛾𝑤 𝑤𝐺𝑠

1 + 𝑤𝐺𝑠

𝑤𝐺𝑠

𝐺𝑠: 𝑛 𝐺𝑠(1 − 𝑛)𝛾𝑤 [𝐺𝑠

− 𝑛 𝐺𝑠 − 1 ]𝛾𝑤

𝑛

𝐺𝑠(1 − 𝑛)

𝑛

1 − 𝑛

𝐺𝑠: 𝑒 𝐺𝑠

1 + 𝑒𝛾𝑤

𝐺𝑠 + 𝑒

1 + 𝑒𝛾𝑤

𝑒

𝐺𝑠

𝑒

1 + 𝑒

𝛾𝑑 ; 𝛾𝑠𝑎𝑡 𝛾𝑑

𝛾𝑤 + 𝛾𝑑 − 𝛾𝑠𝑎𝑡

𝛾𝑠𝑎𝑡

𝛾𝑑

− 1 𝛾𝑠𝑎𝑡 − 𝛾𝑑

𝛾𝑤

𝛾𝑠𝑎𝑡 − 𝛾𝑑

𝛾𝑤 + 𝛾𝑑 − 𝛾𝑠𝑎𝑡

𝛾𝑑 ; 𝑤 𝛾𝑑

𝛾𝑤 − 𝑤𝛾𝑑

(1 + 𝑤)𝛾𝑑 𝑤𝛾𝑑

𝛾𝑤

𝑤𝛾𝑑

𝛾𝑤 − 𝑤𝛾𝑑

Figure 1.5 weight-volume relationship for saturated soil with 𝑉 = 1



𝛾𝑑 ; 𝑛 𝛾𝑑

(1 − 𝑛)𝛾𝑤

𝛾𝑑 + 𝑛𝛾𝑤 𝑛𝛾𝑤

𝛾𝑑

𝑛

1 − 𝑛

𝛾𝑑 ; 𝑒 (1 + 𝑒)𝛾𝑑

𝛾𝑤

𝑒𝛾𝑤

1 + 𝑒+ 𝛾𝑑

𝑒

1 + 𝑒

𝛾𝑤

𝛾𝑑

𝑒

1 + 𝑒

𝛾𝑠𝑎𝑡 ; 𝑤 𝛾𝑠𝑎𝑡

𝛾𝑤 − 𝑤(𝛾𝑠𝑎𝑡 − 𝛾𝑤 )

𝛾𝑠𝑎𝑡

1 + 𝑤

𝑤𝛾𝑠𝑎𝑡

1 + 𝑤 𝛾𝑤

𝑤𝛾𝑠𝑎𝑡

𝛾𝑤 − 𝑤(𝛾𝑠𝑎𝑡 − 𝛾𝑤 )

𝛾𝑠𝑎𝑡 ; 𝑛 𝛾𝑠𝑎𝑡 − 𝑛𝛾𝑤

(1 − 𝑛)𝛾 𝛾𝑠𝑎𝑡 − 𝑛𝛾𝑤 𝑛𝛾𝑤

𝛾𝑠𝑎𝑡 − 𝑛𝛾𝑤

𝑛

1 − 𝑛

𝛾𝑠𝑎𝑡 ; 𝑒 1 + 𝑒 𝛾𝑠𝑎𝑡

𝛾𝑤

− 𝑒 𝛾𝑠𝑎𝑡 − 𝑛𝛾𝑤 𝑒𝛾𝑤

𝛾𝑠𝑎𝑡 + 𝑒(𝛾𝑠𝑎𝑡 − 𝛾𝑤 )

𝑒

1 + 𝑒

𝑤; 𝑛 𝑛

1 − 𝑛 𝑤

𝑛

𝑤𝛾𝑤 𝑛

1 + 𝑤

𝑤𝛾𝑤

𝑛

1 − 𝑛

𝑤; 𝑒 𝑒

𝑤

𝑒

(1 − 𝑒_𝑤𝛾𝑤

𝑒

𝑤

1 + 𝑤

1 + 𝑒𝛾𝑤

𝑒

1 + 𝑒

From Eq. (1.12), the dry unit weight is

𝛾𝑑 =𝐺𝑠𝛾𝑤

1+𝑒=

2.68 (9.81)

1+0.8= 14.61 𝑘𝑁/𝑚3

From Eq. (1.13), the degree of saturation is

𝑆𝑟 % =𝑤𝐺𝑠

𝑒× 100 =

0.24 (2.68)

0.8× 100 = 80.4%

Part (b):From Eq. (1.14), for saturated soils,

𝑒 = 𝑤𝐺𝑠 , or 𝑤 % =𝑒

𝐺𝑠× 100 =

0.8

2.68× 100 = 29.85%

From Eq. (1.15), the saturated unit weight is

𝛾𝑠𝑎𝑡 =𝐺𝑠𝛾𝑤 +𝑒𝛾𝑤

1+𝑒=

9.81 (2.68+0.8)

1+0.8= 18.97 𝑘𝑁/𝑚3

1.2.2 General Range of Void Ratio and Dry Unit Weight Encountered in

Granular Soils

The loosest and the densest possible arrangements that we can obtain from these equal spheres are,

respectively, the simple cubic and pyramidal type of packing as shown in figure 1.6. The void

corresponding to the simple cubic type of arrangement is 0.91; that for the pyramidal type of arrangement is

0.34. In the case of natural granular soils, particles are neither of equal size nor perfect spheres. The small-

sized particles may occupy void spaces between the larger ones, which will tend to reduce the void ratio of

natural soils are compared to that for equal spheres.



(a) (b)

Figure 1.6 Simple cubic (a) and pyramid (b) types of arrangement of equal spheres.

Table 1.2 gives some typical values of void ratios and dry unit weights encountered in granular soils.

Table 1.2 typical values of void ratios and dry unit weights for granular soils

Dry unit weight 𝛾𝑑

Void ratio e

Minimum

Maximum

Soil type Maximum Minimum 𝑘𝑁/𝑚3 𝑘𝑁/𝑚3

Gravel 0.6 0.3 16 20

Coarse sand 0.75 0.35 15 19

Fine sand 0.85 0.4 14 19

Standard 0.8 0.5 14 17

Gravelly

sand

0.7 0.2 15 22

Silty sand 1 0.4 13 19

Silty sand

and gravel

0.85 0.15 14 23


Relative density is a term generally used to describe the degree of compaction of coarse-grained soils.

Relative density 𝐷𝑟 is defined as

𝐷𝑟 =𝑒𝑚𝑎𝑥 −𝑒

𝑒𝑚𝑎𝑥 −𝑒𝑚𝑖𝑛 (1.19)

Where

𝑒𝑚𝑎𝑥 = 𝑚𝑎𝑥𝑖𝑚𝑢𝑚 𝑝𝑎𝑠𝑠𝑖𝑏𝑙𝑒 𝑣𝑜𝑖𝑑 𝑟𝑎𝑡𝑖𝑜

𝑒𝑚𝑖𝑛 = 𝑚𝑖𝑛𝑖𝑚𝑢𝑚 𝑝𝑜𝑠𝑠𝑖𝑏𝑙𝑒 𝑣𝑜𝑖𝑑 𝑟𝑎𝑡𝑖𝑜



𝑒 = 𝑣𝑜𝑖𝑑 𝑟𝑎𝑡𝑖𝑜 𝑖𝑛 𝑛𝑎𝑡𝑢𝑟𝑎𝑙 𝑠𝑡𝑎𝑡𝑒 𝑜𝑓 𝑠𝑜𝑖𝑙

Equation (1.19) can also be expressed in terms of dry unit weight of the soil:

𝛾𝑑(𝑚𝑎𝑥 ) =𝐺𝑠𝛾𝑤

1+𝑒𝑚𝑖𝑛

𝑜𝑟 𝑒𝑚𝑖𝑛 =𝐺𝑠𝛾𝑤

𝛾𝑑(𝑚𝑎𝑥 )− 1 (1.20)

Similarly,

𝑒𝑚𝑎𝑥 =𝐺𝑠𝛾𝑤

𝛾𝑑(𝑚𝑖𝑛 )− 1 (1.21)

And 𝑒 =𝐺𝑠𝛾𝑤

𝛾𝑑 − 1 (1.22)

The results of the sieve analysis are plotted in figure 1.8.

The grain-size distribution can be used to determine some of the basic soil parameters such as the effective

size, the uniformity coefficient, and the coefficient of gradation. The effective size of a soil is the diameter

through which 10% of the total soil mass is passing ad is referred to as 𝐷10 . The uniformity coefficient 𝐶𝑢 is

defined as

𝐶𝑢 =𝐷60

𝐷10 (1.27)

Where 𝐷60 is the diameter through which 60% of the total soil mass is passing. The coefficient of gradation

𝐶𝑐 is defined as

𝐶𝑐 =(𝐷30 )2

𝐷60 (𝐷10 ) (1.28)

Where 𝐷30 is the diameter through which 30% of the total soil mass is passing.

The uniformity coefficient and the coefficient of gradation for the sieve analysis shown in table 1.5 are also

shown in figure 1.8.

Figure 1.8 Grain size distributions



A soil is called a well-graded soil if the distribution of the grain sizes extends over a rather large range. In

that case, the value of the uniformity coefficient is large. Generally, a soil is referred to as well graded if 𝐶𝑢

is larger than about 4 to 6 and 𝐶𝑐 between 1 and 3. When most of the grains in a soil mass are of

approximately the same size – i.e., 𝐶𝑢 is close to 1 – the soil is called poorly graded. A soil might have a

combination of two or more well-graded soil fractions, and this type of soil is referred to as a gap-graded

soil.

For fine-grained soils, the technique used for determination of the grain sizes is hydrometer analysis. This is

based on the principle of sedimentation of soil grains. When soil particles are dispersed in water, they will

settle at different velocities depending on their weights, shapes, and sizes. For simplicity, it is assumed that

all soil particles are spheres, and the velocity of a soil particle can be given by Stokes law as

𝑉 =𝛾𝑠−𝛾𝑤

18𝜂𝐷2 (1.29)

Where 𝑉 = 𝑣𝑒𝑙𝑜𝑐𝑖𝑡𝑦 = 𝑑𝑖𝑠𝑡𝑎𝑛𝑐𝑒/𝑡𝑖𝑚𝑒 = 𝐿/𝑡

𝛾𝑤 , 𝛾𝑠 = 𝑢𝑛𝑖𝑡 𝑤𝑒𝑖𝑔𝑕𝑡 𝑜𝑓 𝑤𝑎𝑡𝑒𝑟 𝑎𝑛𝑑 𝑠𝑜𝑖𝑙 𝑝𝑎𝑟𝑡𝑖𝑐𝑙𝑒𝑠, 𝑟𝑒𝑠𝑝𝑒𝑐𝑡𝑖𝑣𝑒𝑙𝑦

𝜂 = 𝑎𝑏𝑠𝑜𝑙𝑢𝑡𝑒 𝑣𝑖𝑠𝑐𝑜𝑠𝑖𝑡𝑦 𝑜𝑓 𝑤𝑎𝑡𝑒𝑟

𝐷 = 𝑑𝑖𝑎𝑚𝑡𝑒𝑟 𝑜𝑓 𝑡𝑕𝑒 𝑠𝑜𝑖𝑙 𝑝𝑎𝑟𝑡𝑖𝑐𝑙𝑒𝑠

In the laboratory, hydrometer tests are generally conducted in a sedimentation cylinder, and 50g of oven-

dried soil is used. The sedimentation cylinder is 18 in (457.2 m) high and 2.5 in (63.5 mm) in diameter, and

it is marked for a volume of 1000 ml. a 125-ml solution of 4% sodium hexametaphosphate in distilled water

is generally added to the specimen as the dispersing agent. The volume of the dispersed soil suspension is

brought up to the 1000 ml mark by adding distilled water. After through mixing, the sedimentation cylinder

is placed inside a constant-temperature bath. The hydrometer is then placed in the sedimentation cylinder

and readings are taken to the tip of the meniscus (figure 1.10) at various elapsed times.

When the hydrometer is placed in the soil suspension at a time t after the start of sedimentation, it measures

the liquid density in the vicinity of its bulb at a depth L (figure 1.10). the liquid density is a function of the

amount of soil particles present per unit volume of the suspension at that depth. ASTM 152Hydrometers are

calibrated to read the amount in grams of soil particles in suspension per 1000 ml (for

𝐺𝑠 = 2.65 𝑎𝑡 𝑎 𝑡𝑒𝑚𝑝𝑒𝑟𝑎𝑡𝑢𝑟𝑒 𝑜𝑓 200𝐶). Also, at a time t the soil particles in suspension at depth L will

have diameters smaller than those calculated by eq. (1.29), since the larger particles would have settled

beyond the zone of measurement. Hence, the percent of soil finer than a given diameter D can be calculated.

Since the actual conditions under which the test is conducted may be different from those for which the

hydrometers are calibrated(𝐺𝑠 = 2.65, 𝑡𝑒𝑚𝑝𝑒𝑟𝑎𝑡𝑢𝑟𝑒 𝑜𝑓 200𝐶), it may be necessary to make corrections to

the observed hydrometer readings. For further details regarding the corrections, the reader should refer to a

soils laboratory manual (e.g.,Bowles, 1978).



Figure 1.10 Hydrometer analysis.

Lecture 1

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