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23-Ind-B2 Manufacturing Processes · Undated paper

Question 7 of 7: Effect of Doubling Injection-Molded Wall Thickness on Cycle Time, Cost, and Warpage

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Notes on this paper

National Examinations, May 2019 — 17-Ind-B2 Manufacturing Processes. 3-hour closed-book exam; candidates may use a Casio or Sharp approved calculator. Any five questions constitute a complete paper (only the first five as they appear are marked officially); all seven are answered below as a full study resource.

Reference texts. Groover, Fundamentals of Modern Manufacturing: Materials, Processes, and Systems, 6th ed. (primary text for this subject — material selection, casting, polymer processing, metal forming, powder metallurgy, and machining).

Check: every page’s printed footer reads “17-Ind-B2/May 2019”, so this is the May 2019 sitting. In Question 1(ii), option (3) is "Bending". Question 1 uses a multiple-choice (statement-selection) format.

Question 7: Effect of Doubling Injection-Molded Wall Thickness on Cycle Time, Cost, and Warpage (20 marks: 4 each)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. Wall thickness increases from $h_1=0.5\text{ mm}$ to $h_2=1\text{ mm}$ (a thickness ratio of exactly 2), with every other part dimension and every processing condition (melt temperature, mold temperature, material) held fixed.

Find. How injection time, cooling time, material cost, production rate, and warpage each change, quantified where the underlying relationship allows it.

Approach. With every other dimension fixed, doubling wall thickness doubles the part's VOLUME (and hence its mass), which drives (i) and (iii) roughly linearly; cooling time is governed by transient heat conduction through the wall thickness, which scales with the SQUARE of thickness (Groover's cooling-time relation $t_{cool}=\dfrac{h^2}{\pi^2\alpha}\ln\!\left[\dfrac{4}{\pi}\dfrac{T_{melt}-T_{mold}}{T_{freeze}-T_{mold}}\right]$), driving (ii); (iv) and (v) then follow from how (i)-(iii) combine.

  1. (i) Injection (fill) time. Doubling the wall thickness (other dimensions fixed) doubles the cavity volume that must be filled. At a fixed volumetric injection (fill) rate, the fill time is directly proportional to the volume to be injected, so injection time approximately DOUBLES: $t_{inj,2}/t_{inj,1}\approx h_2/h_1=2$.
  2. (ii) Cooling time. Cooling time is set by how long heat takes to conduct out through the part's wall thickness to the (cold) mold surface, and by Groover's cooling-time relation it scales with $h^2$, not $h$. Doubling the thickness therefore roughly QUADRUPLES the cooling time: $$\dfrac{t_{cool,2}}{t_{cool,1}}=\left(\dfrac{h_2}{h_1}\right)^{2}=2^2=\boxed{4}$$ This $h^2$ dependence is why cooling time, not injection time, is normally the dominant and most thickness-sensitive part of the molding cycle.
  3. (iii) Material cost. Part mass (and therefore material cost, at a fixed material unit price) scales directly with volume, exactly as in step 1: doubling thickness (other dimensions fixed) roughly DOUBLES the material used per part, so material cost per part approximately doubles: $\text{cost}_2/\text{cost}_1\approx 2$.
  4. (iv) Production rate. Production rate is inversely proportional to total cycle time, $T_{cycle}=t_{inj}+t_{cool}+t_{reset}$, where $t_{reset}$ (mold open/close and part ejection) is essentially independent of wall thickness. Because $t_{cool}$ (quadrupling) grows far faster than $t_{inj}$ (only doubling) as thickness increases, cooling time's SHARE of the cycle grows even larger, and the cycle-time increase approaches the $4\times$ cooling-time factor as $t_{cool}$ comes to dominate. Illustrating with representative, non-exam-given cycle-time shares (flagged in the check callout below) — $t_{inj,1}=2\text{ s}$, $t_{cool,1}=6\text{ s}$, $t_{reset}=2\text{ s}$ (constant) — gives $T_{cycle,1}=10\text{ s}$ and $T_{cycle,2}=4+24+2=30\text{ s}$: $$\dfrac{\text{rate}_2}{\text{rate}_1}=\dfrac{T_{cycle,1}}{T_{cycle,2}}=\dfrac{10}{30}=\boxed{\tfrac{1}{3}}$$ so production rate falls to roughly a third of its original value in this illustration — a substantial DECREASE, driven mainly by the quadrupled cooling time.
  5. (v) Warpage. Warpage (and related sink marks) is driven by DIFFERENTIAL shrinkage and residual stress across the part's cross-section as it cools and solidifies unevenly — the outer skin freezes first against the mold wall while the core stays hot and molten longer. A thicker wall widens the temperature gradient between skin and core (the core takes proportionally much longer to reach the mold-wall temperature, per the same $h^2$ relation as (ii)), which increases the difference in shrinkage between the fast-cooling skin and the slow-cooling core. Warpage therefore tends to INCREASE with wall thickness — which is exactly why uniform, thin wall sections are a standard design-for-manufacture guideline for injection-molded parts.
Question 7 — effect of doubling wall thickness (0.5 mm → 1 mm), other dimensions/conditions fixed
QuantityScaling relationshipChange
(i) Injection time$\propto h$ (volume, fixed fill rate)≈ doubles ($\times2$)
(ii) Cooling time$\propto h^2$ (Groover cooling-time relation)≈ quadruples ($\times4$)
(iii) Material cost$\propto h$ (volume/mass, fixed unit price)≈ doubles ($\times2$)
(iv) Production rate$\propto 1/T_{cycle}$, $T_{cycle}$ pulled up mainly by (ii)decreases sharply (illustrative ≈1/3×)
(v) Warpagedriven by skin–core shrinkage differential, which widens with $h$tends to increase
Check — illustrative cycle-time constants. The question supplies no numeric injection/cooling/reset times of its own; the $t_{inj,1}=2\text{ s}$, $t_{cool,1}=6\text{ s}$, $t_{reset}=2\text{ s}$ figures used in step 4 are representative, illustrative constants (chosen so cooling time is already the largest single share of the cycle, as it typically is in practice) used only to demonstrate HOW the $\times2$/$\times4$/constant scaling relationships combine into an overall production-rate change — not values taken from the exam. The scaling relationships themselves ($t_{inj}\propto h$, $t_{cool}\propto h^2$, mass $\propto h$) are the load-bearing, defensible part of the answer regardless of the illustrative base numbers chosen.
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