Question 7 of 7: Concrete Curing; Identifying an Unknown Hardenability Lot
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exam 04-BS-11, Properties of Materials — December 2016. 3 hours,
closed-book examination (approved Casio or Sharp calculator only). Candidates attempt any
five of the seven questions for a complete paper, all questions of equal value. All seven
questions are solved below for completeness.
Reference texts: Callister & Rethwisch, Materials Science and
Engineering: An Introduction, 9th ed. (crystal structure, mechanical behaviour, phase
diagrams, polymer viscoelasticity, composites, electrochemistry, fatigue/fracture, heat
treatment and hardenability, concrete).
Question 7: Concrete Curing; Identifying an Unknown Hardenability Lot (20 marks)
Given (a). Concrete is a particle-reinforced composite of Portland cement,
water, fine aggregate (sand) and coarse aggregate (gravel/crushed stone).
Find (a). Main constituents; what happens during curing; effect of
water/cement ratio.
(a) Approach and Answer
Portland cement is a mixture of calcium silicates and aluminates (produced by firing limestone
and clay/shale at high temperature and grinding the clinker to a fine powder). When mixed with
water, the cement undergoes hydration — an exothermic chemical reaction (not
simple drying) in which the calcium silicates react with water to form calcium-silicate-hydrate
(C–S–H) gel, the primary strength-giving binder, plus calcium hydroxide as a
by-product. This C–S–H gel grows and interlocks over time, progressively binding the
sand and gravel aggregate particles into a rigid, load-bearing solid. Curing is
the practice of maintaining adequate moisture (and a favourable temperature) at the concrete
surface for an extended period (commonly 7–28 days) so that hydration can continue as
completely as possible; concrete that is allowed to dry out too early stops hydrating and never
reaches its design strength, and may also develop surface shrinkage cracks.
The water/cement (w/c) ratio is the single most important variable controlling
concrete properties (Abrams’ law: strength decreases roughly monotonically as w/c increases).
A lower w/c ratio gives higher strength and lower permeability, because only enough water
to hydrate the cement is present, and once the excess (unreacted) water is used up or evaporates it
leaves behind less capillary porosity; the trade-off is reduced workability (the fresh mix is
stiffer and harder to place/compact). A higher w/c ratio improves workability and flow but
increases capillary porosity once the surplus water leaves the paste, which lowers compressive
strength and increases permeability — making the concrete more vulnerable to freeze-thaw
damage, reinforcement corrosion, and chemical attack. In practice the w/c ratio is chosen as the
lowest value consistent with the workability needed to place and consolidate the mix properly
(often assisted with plasticizer admixtures rather than by simply adding more water).
(b) Given
Bar diameter $=2.5$ in, quenched in still oil (curve 3 on the correlation charts); observed
hardness traverse (surface–centre–surface) read directly from the given plot: surface
$\approx50$ HRC, ¾-radius $\approx46$ HRC, mid-radius $\approx40$ HRC, centre
$\approx36$ HRC; four candidate hardenability curves A–D; four Jominy-distance
correlation charts (surface, ¾R, mid-R, centre) for round bars, each carrying curves for
quench severities 1 = still water, 2 = mildly agitated oil, 3 = still
oil, 4 = mildly agitated molten salt.
Find (b). Which lot (A–D) matches the unknown bar; the predicted hardness
traverse for the same bar and lot, reheated and quenched in still water.
(b) Approach
This is a read-the-chart engineering-judgement problem, not a closed-form calculation. For each
of the four radial positions: (1) enter the position’s correlation chart at the bar diameter
(2.5 in) on curve 3 (still oil) to read the equivalent Jominy distance; (2) read each
candidate lot’s hardenability curve at that distance to get a predicted hardness; (3) compare
the four predicted hardnesses (one per position) against the four observed traverse readings, and
identify the lot with the closest overall match. All chart readings are approximate (±1–2 HRC,
±0.05 in — the printed charts’ own practical precision) and are disclosed as
such rather than presented with false numeric certainty.
Equivalent Jominy distances for still-oil quench (curve 3), 2.5-in bar. Reading
each of the four correlation charts at diameter $=2.5$ in on curve 3:
$$\text{surface}\approx0.64\ \text{in},\quad \tfrac34\text{R}\approx0.90\ \text{in},\quad
\text{mid-R}\approx1.17\ \text{in},\quad\text{centre}\approx1.19\ \text{in}$$
(mid-radius and centre map to very similar equivalent distances for this bar size — a real,
recognised effect: the four correlation curves converge toward the bar’s interior as diameter
increases, since heat extraction becomes progressively less direction-dependent well below the
surface).
Read each lot’s hardness at those four distances.
Fig. Q7b — hardenability curves for Lots A–D (approximate
reproduction of the given chart), with the observed still-oil traverse values (red dots) marked at
each position’s equivalent Jominy distance.
Predicted hardness at the four still-oil equivalent distances:
Position
Observed
Lot A
Lot B
Lot C
Lot D
Surface
50
54.3
49.2
35.3
22.8
¾-radius
46
48.1
39.3
27.8
20.4
Mid-radius
40
43.3
33.0
23.5
18.1
Centre
36
43.2
32.7
23.3
17.9
Identify the closest-matching lot. Lots C and D read far too low at every
position (average deviation $>10$ HRC) and are ruled out immediately. Between A and B, the
mean absolute deviation from the observed traverse is close either way
($\approx4.2$ HRC for Lot A vs. $\approx4.5$ HRC for Lot B) — not itself a clean
separator. The deciding evidence is the surface reading, the position read with
the least chart-reading ambiguity (a clean, well-separated curve region on both the traverse plot
and the hardenability chart): Lot B matches it almost exactly (49.2 vs. 50 HRC observed, a
0.8 HRC gap), while Lot A misses by 4.3 HRC there. Lot A's error is dominated by a large
7.2 HRC miss at the centre, the position with the largest chart-reading uncertainty in this
problem (Section 1 above); weighting the highest-confidence reading more heavily than the
lowest-confidence one favours Lot B.
$$\boxed{\text{Unknown bar} = \textbf{Lot B}}$$
Predict the traverse under a reheat + still-water quench. Repeat step 1 using
curve 1 (still water) instead of curve 3 on the same four correlation charts, then re-read Lot
B’s hardenability curve at the new (much smaller) equivalent distances:
$$\text{surface}\approx0.19\ \text{in},\ \ \tfrac34\text{R}\approx0.45\ \text{in},\ \
\text{mid-R}\approx0.63\ \text{in},\ \ \text{centre}\approx0.64\ \text{in}$$
Reading Lot B at these distances gives the predicted traverse:
Fig. Q7b — predicted hardness traverse for Lot B under a still-water
requench (blue), compared with the original observed still-oil traverse (red).
$$\boxed{\text{surface}\approx56,\ \tfrac34\text{R}\approx55,\ \text{mid-R}\approx49,\
\text{centre}\approx49\ \text{HRC}}$$
The predicted profile is both higher and much flatter than the oil-quenched traverse
— physically sensible, since still water is a far more severe quenchant than still oil, so
even the bar’s centre cools fast enough to stay close to the fully-martensitic maximum
hardness ($\approx57$ HRC), and the surface-to-centre hardness drop shrinks from
14 HRC (oil) to only $\approx7$ HRC (water).
Quantity
Result
Unknown bar identity
Lot B
Predicted water-quench traverse: surface
≈56 HRC
Predicted water-quench traverse: ¾-radius
≈55 HRC
Predicted water-quench traverse: mid-radius
≈49 HRC
Predicted water-quench traverse: centre
≈49 HRC
Check: all Jominy-equivalent-distance and hardness-curve readings above are
taken directly off the printed charts and carry the charts’ own practical precision,
±1–2 HRC and ±0.05 in; the Lot-B identification is an engineering
judgement call (closest overall match among four candidates), not an exact algebraic result.