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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
McGill University – Department of Mining and Materials Engineering Undergraduate Design Course MIME 452
Scale-Up of Industrial Processes
Robert P. Harrison, Ph.D.
Revision 1 / March 10, 2016
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Congratulations!
• You just received a patent for your novel production method
• On paper, the cost-per-tonne is lower than for the conventional process
• Demonstrated at lab scale only…
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
“Scale-Up”
1. Introduction (10 min.)
2. Theory and its Limitations (15 min.)
3. The Empirical Approach (15 min.)
4. Industrial Case Studies (15 min.)
5. Critical Role of Engineers (5 min.)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
“Scale-Up”
1. Introduction
2. Theory and its Limitations
3. The Empirical Approach
4. Industrial Case Studies
5. Critical Role of Engineers
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Example of Scale-Up: NASA Wind Tunnel Tests
• Let’s start with something a bit more familiar…
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Scale-Up: Big Picture
Everyday Experience
Theory (Physics & Math)
50+ Years of Real
Projects
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
HEAT TRANSFER: Baking a Cake
• If you double a cake recipe, it no longer works – Middle underbaked
• Increase temperature or baking time? – Edges overbaked
• This is a heat-transfer problem: – Radiation – Convection – Conduction
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Original recipe
Doubling all the amounts
Conduction
Radiation
Convection
Baking a Cake
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
MASS TRANSFER: Upper Size Limit for Insects
• Insects cannot grow above a certain size, because their cells get oxygen directly from the air, which must diffuse through pores located on the outside of their bodies
Image by Piotr Jaworski
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Water Droplets
• You can suspend 1 mL of water from your fingertip, but not 100 mL from your elbow
• The drop of water on your fingertip might eventually detach and fall to the ground, but the water droplets in fog never fall down
• Fog is visible, but water vapour is invisible
Why is that?
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Water at Different Scales
Diameter: 10-1 m 1 Litre
The surface tension of water is ~70 mJ/m2, insufficient to maintain such a large droplet (Area ∝ R2, Volume ∝ R3)
Diameter: 10-2 m Raindrop Small enough to hold together…falls to the ground
. Diameter: 10-4 m Fog droplet
Small enough to be buoyed by air movement…water has refractive index of 1.33 so fog is visible (interface)
Diameter: 10-10 m Water vapour Invisible…no interface, just another molecule in the air
.
Single molecule
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
“Scale-Up”
1. Introduction
2. Theory and its Limitations
3. The Empirical Approach
4. Industrial Case Studies
5. Critical Role of Engineers
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Emergent Properties
• The atomic scale never changes • Properties like viscosity and surface tension are
“emergent properties” – Like traffic patterns emerging from the capabilities of a single
vehicle
• Clusters of clusters of clusters of clusters of molecules – Different for each macroscopic scale
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
The Age of Nanotechnology
August 2010: German team captured images of an individual electron
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
We Know the Forces
• According to physicists there are only four forces:
– Gravity – Electrical – Strong Nuclear – Weak Nuclear
Only occur inside an atom’s nucleus… for process engineers, exponential radioactive decay is good enough
Charles-Augustin de Coulomb (1736-1806)
Sir Isaac Newton (1642-1727)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Forces
• According to physicists there are only four forces:
– Gravity – Electrical – Strong Nuclear – Weak Nuclear
Things falling.
Everything else: • Combustion • Chemical reactions • Viscosity • Surface tension • Phase changes • Colour • Biochemistry • Solidness of objects • You-name-it…
Note that this includes
magnetism (a result of Relativity)
Albert Einstein (1879-1955)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Starlings on Ot Moor, England
Play VIDEO http://www.youtube.com/watch?v=XH-groCeKbE
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Metaphor for Molecules: A Flock of Starlings • There is no leader…each bird is reacting to the 6-7 birds that
surround it • Too fast to be “thinking”…this must be pure instinct based on
simple rules • The flock has a constant density (centre vs. edge)…there
seems to be an ideal distance between the birds, much like the average distance between molecules in a liquid
• There is a clear demarcation between flock and empty air…similar to surface tension…maybe each bird is avoiding exposure to predators?
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Differential Equations
Newton’s Laws of Motion
Maxwell’s Equations
Ohm’s Law
Fourier’s Law Fick’s Law
Coulomb’s Law
Laws of Thermodynamics
Newton’s Law of Gravity
Wave Equations
Faraday’s Law
Conservation Laws
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Deceptively modern-looking diagrams from Newton’s Philosophiae Naturalis Principia Mathematica (1687)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Great News!
1. We know all about the particles. 2. We understand the forces involved. 3. We know how groups of particles behave. 4. We have Differential Equations for all the most important
physical phenomena.
First problem: Most Differential Equations are intractable
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Why Not Use a Computer?
• Numerical Methods…computing power limitations – Cake: 1025 molecules – Chemical reactions: femtoseconds
• Quantum Physics
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
O. Smirnova, “Spectroscopy: Attosecond Prints of Electrons”, Nature, Vol. 466, 2010, 700‑702 (image credit: Christian Hackenberger, Ludwig Maximilians University of Munich)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Why Not Use a Computer?
• Numerical Methods…computing power limitations – Cake: 1025 molecules – Chemical reactions: femtoseconds
• Quantum Physics – Probabilistic
• Chaos Theory – Physical systems are extremely sensitive to initial conditions
We are already in deep waters…
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Example of a “Chaotic” System: Drinking Bird Toy
https://www.youtube.com/watch?v=Yk71GY02diY
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Simple Example of Chaos Theory
• Absurdly simple example of Chaos Theory:
XN+1 = 4*XN*(1-XN)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Simple Example of Chaos Theory
• Absurdly simple example of Chaos Theory:
XN+1 = 4*XN*(1-XN)
• The so-called “Butterfly Effect”
– Disturbance of 10-16 introduced at iteration #25…totally different behaviour by iteration #85
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Chaos Theory Example
Disturbance of 10-16
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
“Scale-Up”
1. Introduction
2. Theory and its Limitations
3. The Empirical Approach
4. Industrial Case Studies
5. Critical Role of Engineers
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Symmetry in Physics
Mirror image Different location
Different time
Monday Tuesday
Get the same result
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Symmetry does NOT apply to scale
A larger clock would run too slowly (pendulum)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
The trouble with engineers is they believe anything that’s
written in a book.
- British physicist Derek L. Livesey (1923-1992)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Extrapolating from Laboratory Data
Central Question: Can the correlations found in the laboratory be extrapolated
to the industrial scale? Recovery (%)
Throughput (kg/h)
Lab Scale Commercial
Scale
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Extrapolating from Laboratory Data
Recovery (%)
Throughput (kg/h)
Lab Scale
Pilot Scale
Commercial Scale
We need to test.
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
From Perry’s Handbook, 6th Ed.
“It is generally accepted that the design of a commercial-scale chemical reactor, which is at the heart of a chemical plant, cannot be accomplished by a purely theoretical approach alone.
”A satisfactory scale-up procedure may require a
stepwise empirical approach in which the size of the reactor is increased successively, with a desired commercial size as the goal.
“A purely empirical method would be time-consuming and
expensive…a number of alternative semi-empirical methods have been proposed.”
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Demo Plant
Commercial
At each scale get different behaviour: heat and mass transfer, conduction vs. convection, laminar flow vs. turbulent, etc.
Study different problems at different scales
600 kg/h 6 t/h 60 t/h
x 10 x 10 Lab
1 kg
x 10
Pilot Plant
Idea Inspired thinking
Test-tube / batchwise
Large enough to provide adequate
platform for scale-up
Fully integrated; essentially a miniature
commercial plant
Full-size plant
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
The “Scale-Up Factor”
• To process engineers this means the ratio of the throughputs = larger ÷ smaller – Note that to mechanical engineers this can refer to length (cube root of
volume)
• Typically 5 to 15, but highly variable
• Some examples in the assigned reading…
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Scale-Up Techniques
• Geometric similarity vs. non-geometric
– Area ∝ L2 – Volume ∝ L3
• Chemical similitude…fooling the atoms! – The similar variable – Dimensionless groups
• Fluid dynamics at different scales
– Computer modelling
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
The “Similar” Variable
• Simple example: Mixer
• Possible choices of similar variable – Impeller tip speed – Power per unit volume – Torque per volume – Equal solids suspension – Blend time – …
• Comes down to judgement
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Equipment Challenges
• Easy in lab…hard at full scale – Thickness of walls won’t support weight
• Health & Safety – Small leaks or power surges in the lab → human hazard at
full scale
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Lab vs. Commercial
• Homogenous • Steady state • Equilibrium • Pure • Laminar • Measurable • Visible
• Heterogeneous • Non steady state • Convection • Turbulent flows • Dead zones • Accumulation • Heat loss • Difficult to see/measure
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Example of Pilot Plant
USDA Pilot plant for Biofuel Research (http://www.arserrc.gov/ccse/EngineeringSupportGroup.htm)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
“Scale-Up”
1. Introduction
2. Theory and its Limitations
3. The Empirical Approach
4. Industrial Case Studies
5. Critical Role of Engineers
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Industrial Case Studies for Students
• Seven examples of scale-up failures and successes – Drawn from over 50 years of full-scale industrial projects
• Fictionalized as Projects A through G
• When classifying the projects, failure was defined as: – 10% over budget – Start-up three months late, or – Longer than one year to reach design capacity.
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Summary of 7 Case Studies
Project Categ. Outcome Key steps
skipped Length of
development steps (years)
A NP Success None 12 B NP Success None 11 C NP Success None 17 D NC Success None 2 E NP Failure Demo 2 F NP Failure Demo 2 G NP Failure None 9.5 NP = new process, NC = novel combination of established unit operations The length of time spent on the development steps was time spent directly on each phase, excluding engineering work carried out between stages
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Homework Questions
1. Name two common characteristics of the successful case studies.
2. Identify two common characteristics of the failures.
3. What differences did you notice between a new process and a novel combination of established unit operations?
4. Why do you think that Projects E and F obtained financing but were poorly planned, whereas Project G was well planned but did not obtain financing?
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
In General: Common Characteristics of the Successful Case Studies
• All key development steps were addressed • The length of time spent directly on the development steps for a
new process was over ten years (Shorter development times are sufficient for novel combinations of established unit operations)
• The scale-up factors for a new process from the demonstration to commercial plant were in the order of ten (Larger scale-up factors are allowable for novel combinations of established unit operations)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
In General: Common Characteristics of the Failures
• Skipping the demonstration phase • Spending only two years on the key development
steps • Financing problems
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Project A (Successful)
Project E (Failure)
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
“Scale-Up”
1. Introduction
2. Theory and its Limitations
3. The Empirical Approach
4. Industrial Case Studies
5. Critical Role of Engineers
52
Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
The Human World
• $$$ • Deadlines • Hierarchies • Personalities • Market Trends • Politics
Human beings have the last word
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
The Physical World
Mother Nature has the last word
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Human Nature
It’s a fact of human nature that the easiest person to fool is yourself
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Science is a Disbelief System
royalsociety.org
• The Royal Society – Published Newton’s Principia – Motto is Nullius in Verba
– “Take nobody’s word for it”
• A truly scientific approach assumes:
– All books are wrong! – Everyone you ever met was lying!
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Why are scientists and engineers so critical to decision-making?
RMS Titanic
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Robert P. Harrison, Ph.D. Department of Materials Engineering March 10, 2016
Why are scientists and engineers so critical to decision-making?
RMS Titanic