Civil Engineering / Direct Shear Test
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LABORATORY 20 · CIVIL ENGINEERING

Direct Shear Test lab report

A worked direct shear test lab report with sample observation tables, regression plots, calculations, and error analysis.

WORKED EXAMPLE · BENCHMARK OBSERVATIONS

A complete example civil engineering laboratory report.

Simulated demonstration data.

This report illustrates formal civil engineering data reduction, instrument calibration tares, and structural parameter estimation. Replace its observations with your own experimental telemetry when preparing a civil engineering laboratory report submission.

Student: __________________Student ID: __________________Course: __________________Date: __________________Partner: __________________Instructor: __________________

1. Title and aim

Direct Shear Box Test on Cohesionless Sand (Internal Friction Angle & Dilatancy). Determine the shear strength parameters—angle of internal friction (ϕ) and apparent cohesion (c)—of cohesionless sand under consolidated drained conditions according to ASTM D3080 / BS 1377-7.

2. Abstract

Six controlled civil engineering laboratory observations were systematically evaluated across operational settings Normal Stress = 50.0 kPa to Normal Stress = 250.0 kPa for Direct Shear Box Test on Cohesionless Sand (Internal Friction Angle & Dilatancy). Ordinary least-squares regression yielded an empirical Internal Friction Tangent tan(ϕ) of 0.6250 ratio (difference from theoretical reference = 0.0000%). The empirical telemetry conclusively validates the fundamental civil engineering continuum and constitutive formulation with R² = 1.000000. The investigation demonstrates stable structural and physical behavior, measurement reproducibility, and strict adherence to international ASTM, AASHTO, and ISO standards.

3. Apparatus and fixed settings

4. Theory and graph choice

Shear strength is the foundational mechanical property governing the stability of all geotechnical structures, including shallow footings, retaining walls, cut slopes, and earth dams. Unlike cohesive clays, dry cohesionless sands derive their shear resistance purely from inter-particle friction and interlocking dilatancy between mineral grains. Standardized under ASTM D3080, the direct shear test utilizes a horizontally split brass or stainless steel shear box (typically 60 x 60 mm square, 20 to 25 mm depth). A sand specimen reconstituted to target relative density is placed in the box between porous stones and perforated grid plates. A constant normal compressive stress σ_n is applied vertically via a counterbalanced lever arm or pneumatic piston. The lower half of the shear box is driven horizontally at a controlled slow displacement rate (0.2 to 1.0 mm/min) while the upper half is restrained against a calibrated proving ring or load cell that measures shear force T. As horizontal shear displacement proceeds, shear stress τ = T / A increases to a peak failure stress τ_f. According to the classical Mohr–Coulomb failure criterion, peak shear strength relates linearly to normal stress: τ_f = c + σ_n · tan(ϕ), where ϕ is the angle of internal friction and c is cohesion (c ≈ 0 for clean sand). In this laboratory, direct shear tests are performed across normal stresses from 50 to 250 kPa to evaluate the Mohr-Coulomb failure envelope and calibrate friction tangent tan(ϕ).

τ_f = 0.6250 · σ_n + 5.0000

The governing physical or constitutive relationship was linearized into the coordinate form y = mx + b. Here, the independent coordinate x represents Applied normal stress σ_n (kPa), and the dependent coordinate y represents Peak shear stress at failure τ_f (kPa). The gradient m directly determines Internal Friction Tangent tan(ϕ), while the intercept b accounts for baseline tare values or reference offsets. Linear transformation enables robust parameter estimation via ordinary least squares without non-linear numerical divergence. Plotting transformed observation pairs displays structural stiffness, material strength multipliers, soil shear envelopes, or hydraulic ratings directly as linear slopes.

5. Method

  1. Assemble top and bottom halves of the 60 x 60 mm shear box; secure with vertical alignment pins; place base plate, porous stone, and lower grid plate into box; record initial dimensions.
  2. Weigh required dry sand mass to achieve target relative density (D_r = 65%); place sand into box in three layers; tamp gently to achieve exact 20.0 mm specimen height.
  3. Place upper grid plate, porous stone, and loading pad on top of sand; seat assembly into water carriage on the direct shear machine.
  4. Apply target normal load (50, 100, 150, 200, or 250 kPa) via the lever hanger; remove vertical alignment pins; advance separation screws to create a 0.5 mm gap between box halves to eliminate metal-to-metal friction.
  5. Start horizontal drive motor at 0.5 mm/min; log shear force T, horizontal displacement Δx, and vertical dilatancy Δz at 15-second intervals until peak load is passed.
  6. Repeat tests on fresh identical sand specimens at all normal stresses; plot peak shear stress τ_f versus normal stress σ_n to extract friction angle ϕ and cohesion c.

6. Observations and calculation table

All civil engineering observations use strictly controlled 64-bit IEEE 754 precision buffers. Residuals are computed relative to the ordinary least-squares regression line.

Table 1. Six simulated observations; x and y represent transformed civil engineering metrics.
No.Normal Stress σ_n (kPa)Peak Shear Stress at Failure τ_f (kPa)Applied normal stress σ_n (kPa)Peak shear stress at failure τ_f (kPa)Fitted yResidual
150.036.2550.000036.250036.25000.0000
2100.067.5100.000067.500067.50000.0000
3150.098.75150.000098.750098.75000.0000
4200.0130.0200.0000130.0000130.00000.0000
5250.0161.25250.0000161.2500161.25000.0000

Download the sample observations (CSV) ↓

7. Worked calculation for one observation

For input Normal Stress = 50.0 kPa: Measured Peak Shear Stress at Failure τ_f = 36.2500 kPa. Transformed coordinates: independent x = 50.0000, dependent y = 36.2500.

8. Graph, gradient and final calculation

17.5026.0058.1288.0098.75150.00139.38212.00180.00274.00Applied normal stress σ_n (kPa)Peak shear stress at failure τ_f (kPa)

Circular markers represent empirical structural observations. The solid line represents the ordinary least-squares linear fit.

x̄ = 150.0000; ȳ = 98.7500
Σ(x − x̄)² = 25000.0000
Σ(x − x̄)(y − ȳ) = 15625.0000
m = Σ(x − x̄)(y − ȳ) / Σ(x − x̄)² = 0.62500000
b = ȳ − mx̄ = 5.00000000
y = 0.6250 · x + 5.0000 ⟹ Target Internal Friction Tangent tan(ϕ) = 0.6250 ratio (theoretical = 0.6250)

9. Uncertainty and comparison

Percentage difference = |estimate − theoretical value| / |theoretical value| × 100 = 0.0000%.

For n = 6 observations, Σresidual² = 0.0000; s² = Σresidual²/(n − 2). Gradient standard error = √[s²/Σ(x − x̄)²] = 0.0000. Intercept standard error = √[s²(1/n + x̄²/Σ(x − x̄)²)] = 0.0000.

Propagating the fit parameters yields a fit standard error of 1.000e-05 ratio, with an ideal coefficient of determination R² = 1.000000.

In civil engineering structural materials testing, geomechanics verification, and hydraulics modeling, empirical uncertainties arise from material microstructural heterogeneity, aggregate packing variations, transducer electronic drift (64-bit IEEE 754 precision digital acquisition), and environmental temperature fluctuations. The ordinary least-squares regression across n = 6 standardized test intervals yields unbiased minimum-variance estimators for both slope and intercept. Because the underlying mechanics—including Hooke's elasticity law, Darcy's porous transport, Bernoulli energy conservation, and Mohr-Coulomb shear strength—adhere strictly to continuum physical principles, residual dispersions remain tightly bounded, yielding an ideal coefficient of determination R² ≥ 0.999999 and confirming the theoretical formulation. Systematic errors (such as machine frame compliance, load cell tare offsets, and temperature drifts) are eliminated using certified calibration standards and differential tare subtraction. Uncertainties in derived moduli, shear strength parameters, and transport coefficients are evaluated via multivariate error propagation.

10. Result and discussion

Internal Friction Tangent tan(ϕ) = 0.6250 ratio
Theoretical reference value: 0.6250 ratio

The empirical laboratory observations provide rigorous quantitative verification of Direct Shear Box Test on Cohesionless Sand (Internal Friction Angle & Dilatancy). In civil engineering mechanics of materials, structural analysis, geotechnical engineering, and hydraulics, physical systems are governed by macroscopic equilibrium, compatibility, and constitutive relationships. Across all six observation trials, the empirical slope m = 0.6250 confirms the theoretical model with near-zero residual variance. Furthermore, comparison with established civil engineering benchmarks (Timoshenko & Gere; Terzaghi & Peck; Chow; Neville; and ASTM standards) underscores vital infrastructure design principles including structural safety factors, serviceability deflection limits, and environmental durability. Residual analysis confirms homoscedastic dispersion without systematic non-linear curvature, validating the underlying model assumptions.

11. Precautions and limitations

The civil engineering physical models apply within the specified calibrated operational window (50.0 to 250.0 kPa). Medium dense quartz river sand (relative density D_r = 65%). Mohr–Coulomb parameters: internal friction angle ϕ = 32.0° (tan ϕ = 0.6249 ≈ 0.6250), apparent cohesion intercept c = 5.0 kPa.

12. Conclusion

This laboratory investigation quantitatively verified the mathematical formulation and physical behavior of Direct Shear Box Test on Cohesionless Sand (Internal Friction Angle & Dilatancy). Through rigorous tracking across six observation points, we confirmed an empirical Internal Friction Tangent tan(ϕ) of 0.6250 ratio matching the theoretical reference 0.6250 ratio within 0.0000% error. The investigation demonstrates why this civil engineering testing method serves as an indispensable cornerstone in infrastructure design, structural safety assurance, and construction quality control.

In-Depth Technical Supplement & Structural Engineering Derivation

1. Objective & Practical Significance

The primary objective of this geotechnical engineering laboratory investigation is to evaluate the consolidated drained shear strength parameters—angle of internal friction ($\phi$) and apparent cohesion ($c$)—of clean medium-dense river sand using the direct shear box apparatus according to ASTM D3080 / BS 1377-7. By testing across five normal stress plateaus ($\sigma_n = 50, 100, 150, 200,$ and $250\text{ kPa}$) and executing linear regression on the Mohr–Coulomb failure envelope, we calibrate the friction tangent $\tan(\phi)$ for retaining wall and foundation stability design.

2. Governing Transport Equations & Phenomenological Relations

According to the Mohr–Coulomb failure criterion, peak shear stress $\tau_f$ relates linearly to applied normal stress $\sigma_n$:

\[ \tau_f = \tan(\phi) \cdot \sigma_n + c \]

where $\tan(\phi) = 0.6250$ (friction angle $\phi = 32.00^\circ$) and $c = 5.0000\text{ kPa}$ is the apparent cohesion intercept.

3. Experimental Apparatus & Instrumentation Specification

Testing utilized an automated motorized direct shear apparatus equipped with a precision $60.0 \times 60.0\text{ mm}$ square brass shear box (nominal shear area $A = 3600.0\text{ mm}^2 = 0.0036\text{ m}^2$, specimen depth $20.0\text{ mm}$). Normal stress was applied via a $10:1$ counterbalanced dead-weight lever hanger. Horizontal shear force was measured with an S-type electronic load cell ($5.0\text{ kN}$ capacity, precision $\pm 1.0\text{ N}$). Horizontal and vertical displacements were logged with digital LVDTs ($0.001\text{ mm}$ resolution). The test material was dry quartz sand (uniformity coefficient $C_u = 2.4$, $D_{50} = 0.45\text{ mm}$, specific gravity $G_s = 2.65$, prepared at relative density $D_r = 65\%$).

4. Standard Operating Procedure & Measurement Protocols

For each test, $115.2\text{ g}$ of dry sand was tamped into the shear box to achieve dry density $\rho_d = 1.60\text{ g/cm}^3$. Normal stresses of $50, 100, 150, 200,$ and $250\text{ kPa}$ were applied. Vertical alignment pins were removed, and box clearance screws adjusted to establish a $0.5\text{ mm}$ gap. The horizontal drive was engaged at a constant displacement rate of $0.5\text{ mm/min}$. Shear load and dilatancy were logged until shear displacement reached $6.0\text{ mm}$, well past peak failure stress.

5. Safety Analysis, Hazard Mitigation & Personal Protection

Lever-arm weight hangers carry heavy cast iron masses up to $90\text{ kg}$, presenting crushing hazards if dropped. Operators wore steel-toed footwear and loaded masses carefully onto hanger trays. Horizontal drive pinch points were shielded during motor travel.

6. Raw Experimental Observations & Systematic Data Records

Simulated demonstration data. The following systematic observations were recorded across the direct shear test series on nominal area $A = 0.0036\text{ m}^2$:

TrialNormal Stress σ_n (kPa)Normal Force N (N)Peak Shear Force T (N)Peak Shear Stress τ_f (kPa)Vertical Dilatancy Δz (mm)
150.0180.0130.536.25+0.42 (Dilation)
2100.0360.0243.067.50+0.35 (Dilation)
3150.0540.0355.598.75+0.28 (Dilation)
4200.0720.0468.0130.00+0.21 (Dilation)
5250.0900.0580.5161.25+0.15 (Dilation)

7. Quantitative Mathematical Analysis & Regression Models

Linear regression of peak shear stress $\tau_f$ versus normal stress $\sigma_n$ yields:

\[ \tau_f = 0.62500 \cdot \sigma_n + 5.00000 \]

with an extraordinary coefficient of determination $R^2 = 1.000000$. The experimental slope $\tan(\phi) = 0.62500$ matches the reference benchmark ($0.6250$) with zero relative deviation ($0.00\%$). Calculating the angle of internal friction:

\[ \phi = \arctan(0.62500) = 32.005^\circ \approx 32.00^\circ \]

The apparent cohesion intercept $c = 5.00\text{ kPa}$ reflects minor boundary friction and interlock resistance at low stresses.

8. Rigorous Error Analysis & Uncertainty Propagation

Uncertainties include load cell precision $\delta T = \pm 2.0\text{ N}$, normal load accuracy $\delta N = \pm 2.0\text{ N}$, and shear box dimensions $\delta A / A = \pm 0.3\%$. Propagating into $\tan(\phi)$:

\[ \frac{\delta \tan(\phi)}{\tan(\phi)} = \sqrt{ \left( \frac{\delta \tau}{\Delta \tau} \right)^2 + \left( \frac{\delta \sigma_n}{\Delta \sigma_n} \right)^2 } = \pm 0.85\% \]

The reported friction angle is $\phi = 32.00 \pm 0.25^\circ$.

9. Engineering Discussion & Phenomenological Interpretation

All specimens displayed pronounced peak shear strength followed by post-peak strain-softening toward critical state. Positive vertical displacement measurements ($\Delta z > 0$) confirmed significant dilatancy as densely packed sand grains climbed over adjacent particles during shear. As normal stress increased from $50$ to $250\text{ kPa}$, confining pressure suppressed dilatancy from $+0.42\text{ mm}$ to $+0.15\text{ mm}$, consistent with Rowe's stress-dilatancy theory.

10. Geotechnical Foundation & Retaining Wall Applications

In geotechnical engineering, the calibrated friction angle $\phi = 32.0^\circ$ directly determines foundation bearing capacity factors under Terzaghi's equation ($N_\gamma \approx 30.2, N_q \approx 23.2$) and dictates the Rankine active earth pressure coefficient:

\[ K_a = \frac{1 - \sin(32^\circ)}{1 + \sin(32^\circ)} = \frac{1 - 0.5299}{1 + 0.5299} = \frac{0.4701}{1.5299} = 0.307 \]

ensuring accurate sizing of cantilever retaining wall stems and footing widths.

11. Self-Assessment Conceptual Questions & Model Answers

Q1: Why is the direct shear test unsuitable for evaluating undrained shear strength of saturated clays?
A1: The direct shear box cannot be hermetically sealed; drainage cannot be prevented during shearing, meaning pore water pressure escapes uncontrollably, preventing the establishment of true undrained conditions.

Q2: What is the physical origin of the critical state friction angle $\phi_{cv}$?
A2: At large shear strains ($> 10\%$), initial packing density is erased; particle interlocking vanishes, and shear resistance is governed solely by continuous inter-particle tumbling and sliding at constant volume.

12. Concluding Summary & Verified Engineering Metric

The direct shear box investigation successfully characterized the shear strength of cohesionless sand under consolidated drained conditions. The verified friction tangent $\tan(\phi) = 0.6250$ ($R^2 = 1.000000$) and angle of internal friction $\phi = 32.00^\circ$ provide an authoritative geotechnical benchmark for earthwork stability and foundation design.