- •Contents
- •Foreword
- •Preface
- •1 Materials in the Lab
- •2 Measurement
- •3 Joints, Stopcocks, and Glass Tubing
- •4 Cleaning Glassware
- •5 Compressed Gases
- •6 High and Low Temperature
- •7 Vacuum Systems
- •8 The Gas-Oxygen Torch
- •APPENDIX
- •Appendix A Preparing Drawings for a Technician
- •Index
- •Foreword
- •Preface
- •For the Second Edition
- •Please note:
- •1 Materials in the Lab
- •1.1 Glass
- •1.1.1 Introduction
- •1.1.2 Structural Properties of Glass
- •1.1.3 Phase Separation
- •1.1.4 Devitrification
- •1.1.5 Different Types of Glass Used in the Lab
- •1.1.6 Grading Glass and Graded Seals
- •1.1.7 Separating Glass by Type
- •1.1.9 Stress in Glass
- •1.1.11 Tempered Glass
- •1.1.13 Limiting Broken Glass in the Lab
- •1.1.14 Storing Glass
- •1.1.15 Marking Glass
- •1.1.16 Consumer's Guide to Purchasing Laboratory Glassware
- •1.2 Flexible Tubing
- •1.2.1 Introduction
- •1.2.2 Physical Properties of Flexible Tubing
- •1.3 Corks, Rubber Stoppers, and Enclosures
- •1.3.1 Corks
- •1.3.2 Rubber Stoppers
- •1.3.3 Preholed Stoppers
- •1.3.4 Inserting Glass Tubing into Stoppers
- •1.3.5 Removing Glass from Stoppers and Flexible Tubing
- •1.3.6 Film Enclosures
- •1.4 O-Rings
- •1.4.2 Chemical Resistance of O-Ring Material
- •1.4.3 O-Ring Sizes
- •2 Measurement
- •2.1 Measurement: The Basics
- •2.1.1 Uniformity, Reliability, and Accuracy
- •2.1.2 History of the Metric System
- •2.1.3 The Base Units
- •2.1.4 The Use of Prefixes in the Metric System
- •2.1.5 Measurement Rules
- •2.2 Length
- •2.2.1 The Ruler
- •2.2.2 How to Measure Length
- •2.2.3 The Caliper
- •2.2.4 The Micrometer
- •2.3 Volume
- •2.3.1 The Concepts of Volume Measurement
- •2.3.2 Background of Volume Standards
- •2.3.4 Materials of Volumetric Construction #1 Plastic
- •2.3.5 Materials of Volumetric Construction #2 Glass
- •2.3.6 Reading Volumetric Ware
- •2.3.7 General Practices of Volumetric Ware Use
- •2.3.8 Calibrations, Calibration, and Accuracy
- •2.3.9 Correcting Volumetric Readings
- •2.3.10 Volumetric Flasks
- •2.3.11 Graduated Cylinders
- •2.3.12 Pipettes
- •2.3.13 Burettes
- •2.3.14 Types of Burettes
- •2.3.15 Care and Use of Burettes
- •2.4 Weight and Mass
- •2.4.1 Tools for Weighing
- •2.4.2 Weight Versus Mass Versus Density
- •2.4.3 Air Buoyancy
- •2.4.5 Balance Location
- •2.4.6 Balance Reading
- •2.4.7 The Spring Balance
- •2.4.8 The Lever Arm Balance
- •2.4.9 Beam Balances
- •2.4.10 Analytical Balances
- •2.4.11 The Top-Loading Balance
- •2.4.12 Balance Verification
- •2.4.13 Calibration Weights
- •2.5 Temperature
- •2.5.1 TheNature of Temperature Measurement
- •2.5.2 The Physics of Temperature-Taking
- •2.5.3 Expansion-Based Thermometers
- •2.5.4 Linear Expansion Thermometers
- •2.5.5 Volumetric Expansion Thermometers
- •2.5.7 Thermometer Calibration
- •2.5.8 Thermometer Lag
- •2.5.9 Air Bubbles in Liquid Columns
- •2.5.10 Pressure Expansion Thermometers
- •2.5.11 Thermocouples
- •2.5.12 Resistance Thermometers
- •3.1 Joints and Connections
- •3.1.1 Standard Taper Joints
- •3.1.2 Ball-and-Socket Joints
- •3.1.3 The O-Ring Joint
- •3.1.4 Hybrids and Alternative Joints
- •3.1.5 Special Connectors
- •3.2 Stopcocks and Valves
- •3.2.1 Glass Stopcocks
- •3.2.2 Teflon Stopcocks
- •3.2.3 Rotary Valves
- •3.2.4 Stopcock Design Variations
- •3.3.1 Storage and Use of Stopcocks and Joints
- •3.3.2 Preparation for Use
- •3.3.3 Types of Greases
- •3.3.4 The Teflon Sleeve
- •3.3.5 Applying Grease to Stopcocks and Joints
- •3.3.6 Preventing Glass Stopcocks and Joints from Sticking or Breaking on a Working System
- •3.3.7 Unsticking Joints and Stopcocks
- •3.3.8 Leaking Stopcocks and Joints
- •3.3.9 What to Do About Leaks in Stopcocks and Joints
- •3.3.10 General Tips
- •3.4 Glass Tubing
- •3.4.1 The Basics of Glass Tubing
- •3.4.2 Calculating the Inside Diameter (I.D.)
- •3.4.3 Sample Volume Calculations
- •4 Cleaning Glassware
- •4.1 The Clean Laboratory
- •4.1.1 Basic Cleaning Concepts
- •4.1.2 Safety
- •4.1.3 Removing Stopcock Grease
- •4.1.4 Soap and Water
- •4.1.5 Ultrasonic Cleaners
- •4.1.6 Organic Solvents
- •4.1.7 The Base Bath
- •4.1.8 Acids and Oxidizers
- •4.1.9 Chromic Acid
- •4.1.10 Hydrofluoric Acid
- •4.1.11 Extra Cleaning Tips
- •4.1.12 Additional Cleaning Problems and Solutions
- •4.1.13 Last Resort Cleaning Solutions
- •5 Compressed Gases
- •5.1 Compressed GasTanks
- •5.1.1 Types of Gases
- •5.1.2 The Dangers of Compressed Gas
- •5.1.3 CGA Fittings
- •5.1.4 Safety Aspects of Compressed Gas Tanks
- •5.1.5 Safety Practices Using Compressed Gases
- •5.1.6 In Case of Emergency
- •5.1.7 Gas Compatibility with Various Materials
- •5.2 The Regulator
- •5.2.1 The Parts of the Regulator
- •5.2.2 House Air Pressure System
- •5.2.4 How to Use Regulators Safely
- •5.2.6 How to Purchase a Regulator
- •6 High and Low Temperature
- •6.1 High Temperature
- •6.1.1 TheDynamics of Heat in the Lab
- •6.1.2 General Safety Precautions
- •6.1.3 Open Flames
- •6.1.4 Steam
- •6.1.5 Thermal Radiation
- •6.1.6 Transfer of Energy
- •6.1.7 Hot Air Guns
- •6.1.8 Electrical Resistance Heating
- •6.1.9 Alternatives to Heat
- •6.2 Low Temperature
- •6.2.1 TheDynamics of Cold in the Lab
- •6.2.2 Room Temperature Tap Water (=20°C)
- •6.2.8 Safety with Slush Baths
- •6.2.9 Containment of Cold Materials
- •6.2.10 Liquid (Cryogenic) Gas Tanks
- •7 Vacuum Systems
- •7.1 How to Destroy a Vacuum System
- •7.2.1 Preface
- •7.2.2 How to Use a Vacuum System
- •7.2.4 Pressure, Vacuum, and Force
- •7.2.5 Gases, Vapors, and the Gas Laws
- •7.2.6 Vapor Pressure
- •7.2.7 How to Make (and Maintain) a Vacuum
- •7.2.8 Gas Flow
- •7.2.9 Throughput and Pumping Speed
- •7.3 Pumps
- •7.3.1 The Purpose of Pumps
- •7.3.2 The Aspirator
- •7.3.3 Types and Features of Mechanical Pumps
- •7.3.4 Connection, Use, Maintenance, and Safety
- •7.3.5 Condensable Vapors
- •7.3.6 Traps for Pumps
- •7.3.7 Mechanical Pump Oils
- •7.3.8 The Various Mechanical Pump Oils
- •7.3.9 Storing Mechanical Pumps
- •7.3.11 Ultra-High Vacuum Levels Without Ultra-High
- •7.3.12 Diffusion Pumps
- •7.3.13 Attaching a Diffusion Pump to a Vacuum System
- •7.3.14 How to Use a Diffusion Pump
- •7.3.15 Diffusion Pump Limitations
- •7.3.17 Diffusion Pump Maintenance
- •7.3.18 Toepler Pumps
- •7.4 Traps
- •7.4.1 The Purpose and Functions of Traps
- •7.4.2 Types of Traps
- •7.4.3 Proper Use of Cold Traps
- •7.4.4 Maintenance of Cold Traps
- •7.4.5 Separation Traps
- •7.4.6 Liquid Traps
- •7.5 Vacuum Gauges
- •7.5.2 The Mechanical Gauge Family
- •7.5.4 The Liquid Gauge Family
- •7.5.5 The Manometer
- •7.5.6 The McLeod Gauge
- •7.5.7 How to Read a McLeod Gauge
- •7.5.8 Bringing a McLeod Gauge to Vacuum Conditions
- •7.5.10 The Tipping McLeod Gauge
- •7.5.11 Condensable Vapors and the McLeod Gauge
- •7.5.12 Mercury Contamination from McLeod Gauges
- •7.5.13 Cleaning a McLeod Gauge
- •7.5.14 Thermocouple and Pirani Gauges
- •7.5.15 The Pirani Gauge
- •7.5.16 Cleaning Pirani Gauges
- •7.5.17 The Thermocouple Gauge
- •7.5.18 Cleaning Thermocouple Gauges
- •7.5.19 The lonization Gauge Family
- •7.5.20 The Hot-Cathode Ion Gauge
- •7.5.21 Cleaning Hot-Cathode Ion Gauges
- •7.5.24 The Momentum Transfer Gauge (MTG)
- •7.6 Leak Detection and Location
- •7.6.1 AllAbout Leaks
- •7.6.3 False Leaks
- •7.6.4 Real Leaks
- •7.6.5 Isolation to Find Leaks
- •7.6.6 Probe Gases and Liquids
- •7.6.7 The Tesla Coil
- •7.6.8 Soap Bubbles
- •7.6.9 Pirani or Thermocouple Gauges
- •7.6.10 Helium Leak Detection
- •7.6.11 Helium Leak Detection Techniques
- •7.6.13 Repairing Leaks
- •7.7 More Vacuum System Information
- •7.7.1 The Designs of Things
- •8 The Gas-Oxygen Torch
- •8.1.2 How to Light a Gas-Oxygen Torch
- •8.1.3 How to Prevent a Premix Torch from Popping
- •8.2.2 How to Tip-Off a Sample
- •8.2.3 How to Fire-Polish the End of a Glass Tube
- •8.2.4 Brazing and Silver Soldering
- •Appendix
- •A.2 Suggestions for Glassware Requests
- •B.1 Introduction
- •B.2 Polyolefins
- •B.3 Engineering Resins
- •B.4 Fluorocarbons
- •B.5 Chemical Resistance Chart
- •C.1 Chapter 1
- •C.4 Chapter 4
- •C.5 Chapter 5 & Chapter 6
- •C.6 Chapter 7
- •C.7 Chapter 8
- •D.1 Laboratory Safety
- •D.2 Chemical Safety
- •D.3 Chapter 1
- •D.4 Chapter 2
- •D.5 Chapter 3
- •D.6 Chapter 4
- •D.7 Chapter 5 and the Second Half of Chapter 6
- •D.8 Chapter 7
- •D.9 Chapter 8
- •Index
Glass 1.1 |
5 |
years, one of the rods was released from the strain: within 48 hours it returned to its original shape.
R.C. Plumb offers an excellent theory as to why old windows are sometimes thicker on the bottom than on top. He reports that the old technique of manufacturing windows involved collecting a large amount of melted glass at the end of a metal blowpipe, blowing a vase, and attaching the vase bottom to a solid metal rod called a ponty. The end that was blown into is now removed, leaving an open end pointing away from the glassblower. By reheating and then rapidly spinning the hot (soft) vase, the glassblower would use centrifugal force to make the open end flair out, thus transforming the vase into a flat circular pane up to five feet in diameter. From this pane (or "table," as it was called), the glassblower would cut square sections. The sections would have varying thicknesses depending on how far from the center of the "table" they were cut.
Plumb does not offer a strong reason as to why he believes the thicker sections were placed on the bottom. He states, "It would certainly make good sense to install the glass with the thick edge down!" I am unaware of anyone acknowledging if any windows have ever been found to be thicker on the top than on the bottom. It is conceivable that if any such windows were ever noticed, they were disregarded because they did not fit into the pre-expected pattern of being thicker on the bottom.
Because of the belief that glass may sag under its own weight, there has been concern about the storage of glass tubing and rods at an angle. The only danger to glass being stored at an angle is fear of damage to the ends of the glass. Otherwise, there is no problem with storing glass vertically, at an angle, or on its side.
1.1.3 Phase Separation
Pure quartz glass, lead glass, borosilicate glass, or any other type of glass that is clear is in phase. In-phase glass is completely homogeneous throughout. Glass that has any cloudy nature to its appearance can easily be discerned as being out of phase or has phase separation. The cloudy nature is due to inseparable phase (or materials) from the glass phase. As mentioned, glass is glass because it cools too fast for the molecules to align themselves into their crystalline structure. If there are nucleating agents that can enhance the growth of crystals or if the glass is held at too hot a temperature for too long, some crystallization will occur.
Sometimes phase separation can be visually desirable such as that which occurs in opaline glass. By placing an earth alkali fluoride or phosphate material on the surface of the glass, the quickly generated fine-crystalline surface disperses light so efficiently that an opal glow is created. Photosensitive glass is an excellent example of a more practical/commercial use of phase separation. This phase separation is activated by ultraviolet light; and once the ultraviolet light is removed, the glass rephases to the glassy state.
Phase separation is not always a surface phenomenon. The glass that is eventually changed into a pyroceramic material has a nucleating agent mixed throughout
6 Materials in the Lab
the original vitreous material. After the object has been formed and examined, it is slowly baked through its phase separation in an oven.
Vycor®, a high-temperature glass that often can be substituted for quartz glass, is also made by a phase separation process (see page 16).
The phase separation producing opalescence and photosensitivity are produc- tion-created. That is, during the production of the glass, the phase separation occurs. The phase separation that occurs with pyroceramic material and Vycor requires baking the glass at high temperatures for an extended time. This elevated temperature provides the time for the molecules to align and/or separate themselves in a crystalline pattern.
Unfortunately, not all phase separation is desirable. When borosilicate glass is heated for too long near its annealing temperature, a phase separation will occur. This tends to exhibit itself throughout the glass, but can only be observed with an electron microscope. Despite it not being observable to the naked eye, the ramifications of this separation are considerable. The glass separates itself into two phases: One is rich in silicic acid, while the other is rich in alkali borate.5 The result of this change is that the glass has much greater sensitivity to chemical attack.
The significance of the chemical attack sensitivity can best be demonstrated by heat exchangers that must deal with high-temperature water. There are several issues and conditions that come together for this effect:
1.Heat exchangers aremade of thick glass.
Because thick glass requires a longer annealing process, there is a greater opportunity for phase separation to occur.6
2. Due to the manufacturing process,they must go throughthe annealing process several times.
Phase separation is a result of the total length of time the glass is held to high temperatures, not the length of time at any one setting.
3. Glasses with high alkali content are more susceptible to chemical attack.
Water is not generally thought of as a caustic material, but it can be to less chemically resistant glass (e.g., lead and soda-lime glass). Even soda-lime glass that has too great a percentage of soda is more chemically vulnerable than a soda-lime glass with a lower percentage of soda. Generally, borosilicate glass is generally very resistant to water. However, if the alkali concentration is too high (due to phase separation) and this glass is subjected to high-temperature water (more corrosive than room temperature water), greater glass erosion can be expected.
Glass 1.1 |
7 |
Because the thick glass (of a heat exchanger) that had been annealed several times is now confronting hot water,* it is more likely to fail (corrode and break) than other borosilicate glassware.
Aside from being initiated by sitting in hot ovens for too long a period of time, phase separation can also occur when a glass is worked too long or too often. This is why glass can only be repaired a limited number of times. After too many repairs, glass devitrifies (or recrystallizes, a symptom of phase separation) while being worked (see next section), and this devitrification does not disappear by heating. There are five items to consider for limiting the possibility, or degree of phase separation due to annealing operations1^
1. All annealing procedures to which an article is subjected before completion must be added together.
2.The number of annealing steps should be kept as small as possible
3.Since the level of the annealing temperature and the duration of the annealing method tend in the same direction (i.e., phase separation), these should be limited whenever possible.
4.The annealing temperature should not exceed 550°C.
5.Each separate annealing period should not exceed 30 minutes. Should an article have to be annealed several times, the sum of all annealing periods should not exceed two hours.
Regardless of the heating processes, phase separation will occur if the glass was not cleaned prior to annealing. Salts (from finger prints), silicone grease, water spots, and other contamination can "burn into" the glass, creating nucleation points from which phase separation will originate.
1.1.4 Devitrification
Devitrification is the recrystallization of glass. Glass that is devitrified appears frosty (translucent) and is no longer transparent. Devitrified glass is structurally
(Direction |
|
(Direction |
of motion) |
Flexing the glass |
of motion) |
|
Devitrification on |
Tension |
surface of glass |
Fig. 1.2 Creating devitrification in glass. |
|
'Extremely hot water, by its very nature, is significantly more corrosive than room temperature water which compounds the problem.
trThis list is provided by Glass Warehouse, with permission.
8 Materials in the Lab
weaker and is more vulnerable to chemical attack. If a glass is held within its crystallization temperature* for a sufficiently long time, phase separation occurs and the atoms have time to align themselves into a crystalline structure. Once the temperature is allowed to drop, the glass becomes increasingly more viscous, until it cannot further devitrify.
There are several ways to force glass to devitrify (whether devitrification is desired or not). One technique is to heat the glass until it begins to soften, then mechanically work, or flex, the glass while it cools. Eventually a whitish frost will appear on the surface in the region of compression (see Fig. 1.2).
The risk of devitrification rises the longer a glass is kept in a softened or melted state, and it is also linked to how dirty the glass is. Devitrification typically begins as a surface phenomenon, using either dirt or some other surface defect as a nucleation point.7 The devitrification process may be assisted by variations in the exterior composition (which is typically different from the interior) of a glass object.8 These variations may be the result of flame-working the glass, surface contamination, or chemical attack.
Devitrification can often be removed by reheating a glass up to its melting temperature and avoiding any mechanical action while it recools to a rigid state. However, if a glass is overworked or dirty when originally flame-heated, removal of the devitrification may be impossible. If glass has been held too long at an annealing temperature or has been repaired too often, it may not be possible to remove the devitrification.
Mechanical stress is not a requirement for devitrification. The phenomenon is also common in quartz glass furnace tubes maintained at high temperatures for extended periods of time. Devitrification of silica occurs at increasing rates from 1000°C to 1710°C, which is the crystallization temperature and melting point range of B-cristobalite.1^ Insufficient surface cleaning and very slow cool-down times typically facilitate devitrification on these tubes. Early-stage devitrification on a quartz glass furnace tube may be removed by a hydrofluoric acid dip. This cleaning procedure can remove only surface cristobalite. Devitrification deeper than surface level cannot be removed.
The best way to limit or prevent devitrification on quartz glass is to ensure that it is maintained scrupulously clean: No fingerprints, oils, dirt, or chemicals of any
*The specific crystallization temperature is not commonly identified, but typically is between the annealing and softening points.
^-Cristobalite is transparent. We do not normally consider devitrified glass as a transparent material. However, once fused silica has cooled below 250°C, 6-cristobalite is transformed into a-cristo- balite. This substance is the white opaque material we usually associate with devitrified silica. When fused silica is reheated into the devitrification range, the a-cristobalite turns back into 6-cristobalite. However, because a-cristobalite has many fissures and cracks, the opacity remains when it is reheated back into fi-cristobalite.