Subject: Re: Eight Features of an Ideal Intro Stat Course (Response to comments by Ronan M. Conroy) To: EdStat E-mail List and sci.stat.edu Newsgroup From: Donald B. Macnaughton <donmac@matstat.com> Date: Tuesday February 6, 2001 Cc: Ronan M Conroy ----------------------------------------------------------------- In a 99/5/9 post I suggest that relationships between variables are more interesting for students than univariate distributions. Referring to this point, Ronan Conroy writes (on 99/5/10) > This is a fundamental point. Ampere, in a crucial development > in the philosophy of science, pointed out that science does not > study things in themselves, but the relationships between their > attributes. The "things" Ronan refers to are what I call "entities". The "attributes" are (essentially) what I call "properties" or "vari- ables". (I discuss why I recommend the word "entity" over other candidate words in a paper [1998, app. E.1]. I recommend the word "prop- erty" over the word "attribute" because word frequency statistics suggest that beginners are more familiar with the former word [Breland and Jenkins 1997]. I discuss my view of the relation- ship between the words "property" and "variable" in a paper [1998, app. E.2].) I fully agree with Ronan's point that science (together with all the other branches of empirical research) generally studies rela- tionships between properties (or relationships between attributes or relationships between variables). I discuss this idea further in a paper (1999, sec. 3.4). André-Marie Ampère (Andre-Marie Ampere, 1775-1836) emphasized the concept of a relationship between a certain type of entities -- entities he called "phenomena" (Williams 1970, 1989; Hofmann 1996). Since both variables and properties can be conceptually viewed as "phenomena", Ampère was clearly close to the concept of 'relationship between variables'. Probably Ampère viewed "phenomena" as being equivalent to what modern speakers of English refer to as "variables". However, I have been unable to confirm this because Ampère wrote in French, and my French is weak, and I have not found any English transla- tions of Ampère's detailed philosophical writing. So I have been unable to directly study his philosophical writing to see how he characterized his concept of 'phenomena'. Do any readers have further information about Ampère's characterization of phenomena or about translations of his philosophical writing? * * * Ampère brilliantly recognized and described the scientific method (Williams 1989). The method (which is also called the hypothetico-deductive method of science) consists of the follow- ing four steps: 1. A researcher frames (i.e., invents) a new hypothesis about some area of experience. (The researcher frames the hypothe- sis on the basis of knowledge of earlier research, intuition, and logic.) 2. A researcher (perhaps the same researcher) then deduces or in- fers an empirically testable implication of the hypothesis. 3. A researcher (perhaps the same) then performs an empirical re- search project to test whether the implication is actually present in the area of experience. 4. If evidence of the implication is found (and in the absence of a reasonable alternative explanation), the community with prime interest in the area of experience will (by informal consensus) accept (or will be more inclined to accept) the hy- pothesis framed in step 1 as being correct. Ampère's description of the scientific method is important be- cause most modern scientific research (and most other empirical research) proceeds formally according to this method. (I discuss the formal and informal aspects of the progress of science in appendix A.) Examination of instances of the use of the scientific method sug- gests that the implication in step 2 can usually be usefully viewed as a statement of a relationship between variables in some population of entities. Thus the key statistical concept of 're- lationship between variables' plays a central role in the scien- tific method. * * * Ampère's empirical interests were in part in the branch of phys- ics known as electrodynamics, which he founded (Williams 1989). Perhaps his most important contribution in electrodynamics is the discovery of the following relationship between variables: The magnetic force between small elements of two cur- rent-carrying conductors is inversely proportional to the square of the distance between them and is directly proportional to the product of the currents. (Ampère also described how the three angles that define the relative directions of the two conductors affect the size of the force.) The force described in this relationship is important because it is the force that drives almost all electric motors. Scientists have recognized the importance of Ampère's work in electrodynam- ics by naming the unit of electric current, the ampere, in his honor. * * * Ampère's contributions lead to questions about the history of re- lationships between variables. Researchers have been formally studying such relationships for centuries (with differing degrees of emphasis in different eras). For example, the Pythagorean theorem describes a formal relationship between variables that was discovered by Pythagoras in the 6th century BCE. Going back further still, humans (without being aware of it) have been informally using relationships between "variables" since when we began to reason. The aphorisms "haste makes waste" and "power corrupts" are good examples of informal statements of re- lationships between variables. The use of relationships between variables is not limited to hu- mans and may also exist in animals. That is, we could build plausible models of some animal reasoning in terms of an animal (unconsciously) learning about simple relationships between "variables" that reflect properties of its habitat. The animal uses the knowledge of the relationships to aid in its survival. For example, an animal might learn a relationship between the time of day and the likely location of prey. Such a learning ap- proach to survival enables an animal to adjust as quickly as pos- sible (sometimes within seconds or minutes) to unpredictable changes in its habitat, such as changes due to a fire, a flood, or an epidemic among its prey. These changes invariably cause new relationships between variables to arise. It is in an ani- mal's survival interest to learn as quickly as possible about all relationships that have response variables that affect its sur- vival or reproductive capability. Viewing learning as learning about relationships between vari- ables is also reflected in the literature of machine learning. For example, Vapnik, in the first sentence in the first chapter of his book The Nature of Statistical Learning Theory, writes In this book we consider the learning problem as a prob- lem of finding a desired dependence using a limited num- ber of observations (2000). Vapnik goes on to show that the "dependence" he refers to is a dependence (i.e., a relationship) between a single response vari- able and zero or more predictor variables. * * * Ampère studied relationships between variables in the field of physics which (together with chemistry, astronomy, and engineer- ing) is one of the physical sciences. As I discuss in a paper, most empirical research in the physical sciences can be usefully viewed as studying relationships between variables (1999, app. B). When physical scientists study relationships, the standard sta- tistical concepts of 'population' and 'sample' are often fuzzy or not present. This is because in the physical sciences any "sen- sible" sample of entities will often perform quite well as a rea- sonable sample from the (implicit) population. For example, Isaac Newton's law of cooling states that the rate of cooling of a physical object when it is hotter than its envi- ronment is proportional to its excess temperature. The model equation for this relationship between variables is r = k * deltaT where r is the rate of cooling (in degrees per unit of time) deltaT is the excess temperature of the physical object above the ambient temperature and k is a constant. (k is constant within any given physical object, but varies from one physical object to the next.) Newton derived this relationship from empirical research in which he measured the excess temperature and computed the rate of cool- ing at several times in a sample of relatively hot physical ob- jects. In all the cases in the sample he found strong evidence that this specific relationship between variables was present. Thus Newton generalized the findings to his law. Because the law has been repeatedly verified, physicists believe it applies to all macroscopic physical objects in the population of physical objects at all times. (It is possible [and may be known] that the constant k in Newton's law of cooling is not a perfect constant. Instead, k may be better viewed as varying slightly as a function of tem- perature, excess temperature, or possibly other variables. All relationships between variables may be refined as measurement technology improves.) Newton's discovery of the law of cooling illustrates how in em- pirical research in the physical sciences we may not need to pay much attention to the population and sample -- the relationship between variables under study is exactly the same throughout a very broad population. On the other hand, in most other areas of empirical research (including the biological and social sciences) the definitions of the population and sample are important be- cause in these areas a relationship between variables may change substantially if we change to a slightly different population or sample. * * * If we use the instruments and procedures Newton used to investi- gate the law of cooling, we find that the error variation in the relationship in research data reflecting the law is negligible. Thus when Newton discovered the relationship he did not need to use statistical methods to study the relationship. Instead, he could see strong support for his conclusion that the relationship reflected in the law is present by merely scanning his research data, or by a few simple mathematical operations on the data, or by plotting the data on scatterplots. More generally, because of the (usually) low error variation in relationships between variables studied in the physical sciences, physical scientists often do not use statistical methods beyond standard graphics to study relationships between variables. (To fit model equations they sometimes use homegrown algebra and sometimes statistical methods.) On the other hand, in other ar- eas of empirical research the error variation is usually large enough that the use of statistical methods greatly simplifies the study of relationships between variables. In addition, statisti- cal methods can reliably detect subtle phenomena in data that may otherwise go unnoticed. * * * Researchers in the physical sciences may have difficulty if they omit using statistical methods -- witness the cold fusion contro- versy. The key issue in this controversy can be usefully viewed as whether certain unexpected relationships between variables are present in a cold fusion cell. A cold fusion cell is an electrolytic cell with a palladium cath- ode and often with a platinum anode and containing a solution of deuterium (heavy water) and lithium deuteroxide. The original cold fusion researchers reported that, under certain conditions, if a cold fusion cell was connected to a source of electric cur- rent, the heat energy output (response variable) was substan- tially greater than the electrical energy input (predictor vari- able). Such a relationship between variables contradicts ac- cepted physical theory. The original researchers believed that the (perceived) unexpected extra energy output of the cell was due to the nuclear reaction of fusion taking place in the cathode -- nuclear fusion gives off heat. Were it true that nuclear fu- sion was occurring in these cells, it would have been extremely important because it would suggest that we could use cold fusion as a new safe and inexpensive source of energy. Some researchers reported that (using their own cold fusion cells) they were able to replicate the relationship between vari- ables reported by the original researchers. But many other re- searchers reported that they were unable to replicate the rela- tionship (and were unable to demonstrate other implied relation- ships between variables). In the end, the weight of evidence led most physical scientists to conclude that the claimed new phenom- ena (which can be usefully viewed as relationships between vari- ables) are not present (Huizenga 1993). The cold fusion controversy lasted several years and consumed a substantial amount of physical scientists' resources. As sug- gested by the government panel that investigated cold fusion, the high resource consumption may have been partly because some re- searchers involved in the controversy were not using proper sta- tistical methods to determine whether the claimed new relation- ships between variables were present (Energy Research Advisory Board 1989, app. 2.C). If the original cold fusion researchers had used proper statisti- cal methods for detecting relationships (i.e., statistical tests, a proper taking account of negative results, and experimental de- sign considerations), it seems likely that the repeated high or borderline p-values would have quickly alerted them to the fact that that the sought-after relationships between the variables were probably not present. Or if the relationships were present, they were not properly detectable with the current experimental methods, and thus further "more powerful" research must be per- formed before a responsible positive conclusion could be drawn. This might have saved the original researchers considerable em- barrassment and might have saved the physical science community substantial costs. Omission of the use of statistical methods is not the only possi- ble cause of the cold fusion errors. As also discussed by the Energy Research Advisory Board panel, some of the mistaken posi- tive conclusions may have arisen through errors that were made in the measurement methods the original researchers used -- errors that caused the measured net energy output of some cold fusion cells to be over-estimated (1989, sec. II, app. 2.C). Cold fusion research is associated with the sub-domain of chemis- try called "electrochemistry". But regardless of whether the do- main is chemistry, or medicine, or psychology, or any other area of empirical research, a researcher can marry statistical methods with proper measurement methods in the domain. This marriage, when tempered with the proper cautions, yields optimal empirical procedures to detect and study relationships between variables. > An attribute is the relationship between a measurement process > and the thing to be measured, Ronan gives a definition of the concept of 'attribute' or 'prop- erty'. He defines the concept in terms of three other concepts, namely, 'relationship', 'measurement process', and 'entity' (i.e., "thing to be measured"). Ronan uses the concept of 'measurement process' to define the concept of 'property'. Thus he appears to view the concept of 'measurement process' as being more fundamental than the concept of 'property'. Ronan's view does not seem to be contradictory, but it is different from mine. I view the concepts of 'entity' and 'property' as being verbally undefined, just like the con- cepts of 'mass', 'length', 'time', and 'temperature' are usually verbally undefined in physics. (Mass, length, time, and temperature are all properties of enti- ties. Mass and length are properties of physical objects. Time [duration or point in time] can be viewed as a property of events or a property of "reality" [the entity that contains all other entities]. Temperature can be viewed as a property of environ- ments. The ways of measuring these properties are clearly de- fined in physics, but the concepts themselves are verbally unde- fined. I discuss some possible objections to these points in ap- pendix B.) The concepts of 'mass', 'length', 'time', and 'temperature' are verbally undefined in physics because it is not possible to ver- bally define every concept in a field without introducing unde- sirable circularity. Therefore, physicists have been forced to choose certain of their concepts to be verbally undefined. It makes sense to choose the simplest concepts in a field to be ver- bally undefined and then, when possible, to define the more com- plicated concepts in terms of the simpler undefined concepts. Hence the concepts of 'mass', 'length', 'time', and 'temperature' are verbally undefined in physics. Dictionaries generally give definitions of the four undefined concepts because such definitions provide the most benefit for dictionary users. However, examination of the definitions and examination of the definitions of the terms used in the definien- tia invariably reveals (of necessity) that the set of definitions associated with any of the four concepts is circular. Thus with- out outside help we cannot use these definitions to explain or understand the four concepts. Thus although the four concepts have dictionary definitions, they are (due to the circularity of the definitions) still effectively undefined. If no (non-circular) verbal definition is available for a par- ticular concept, how can we understand it? We can understand a verbally undefined concept through "ostensive" definitions of it. An ostensive definition is one that does not rely on words. In- stead, the definition works through the defining person physi- cally pointing at the thing being defined, or it may work through some other form of direct experience. The direct experience al- lows one to learn the concept without having to use words (except for the word or words naming the concept being defined). For example, although the fundamental properties of 'mass', 'length', 'time', and 'temperature' have no verbal definitions in physics, they have ostensive definitions. These definitions are not given in words and thus do not appear in formal discussion. (The definitions are generally taken for granted in formal dis- cussion.) Instead, the four definitions are given through direct experience -- experience that occurs many times for most people before they are eight years old. For example, consider the property of the mass of a physical ob- ject. (As one learns in high-school physics, this property is basically the same as the property of the weight of a physical object. The difference between these concepts, which is some- times important, is not relevant here.) We can teach the prop- erty of mass to an interested child who does not understand it by handing them various physical objects and saying "heavy", "very heavy", "light", and so on, as appropriate. Children can quickly learn any perceivable property through such ostensive definitions if enough opportunities are available for them to properly dis- criminate different values of the property directly. As infants we learn our first words (e.g., "mommy", "TV", "green") through informal ostensive definitions that occur in the speech and actions of the people around us. Furthermore, most people learn almost all the words they use in their day-to-day conversation through ostensive definitions, not through verbal definitions. Thus ostensive definitions are more basic than ver- bal definitions. In an approach that is identical to the approach taken in phys- ics, I view the concepts of 'entity' and 'property' as verbally undefined fundamental concepts in empirical research (and also verbally undefined fundamental concepts in broader day-to-day hu- man reality). Humans understand these concepts through the many ostensive definitions of them we experience and because the con- cepts are the basis for a substantial part of our thinking. I further discuss the role of the concepts in thinking in the 1999 paper (sec. 3). * * * Ronan's definition introduces the important concept of a "meas- urement process" -- a process that we use to measure the values of a property. For any given property of entities, researchers may view the property as if there is one specific property, but there may be several ways of measuring the value of the property in entities. For example, we can measure a person's weight (or mass) using a standard bathroom scale (which may be a spring balance), or we can use a pan balance in which we balance the person's weight against known weights, or we can use a weight guesser from a car- nival. All these methods are valid methods for measuring a per- son's weight in the sense that they yield estimates that are highly correlated with each other. However, these measures are of different quality in the sense that they have different preci- sion (i.e., high or low random variation about their expected value) and different bias (i.e., expected deviation from the "true" value). * * * The preceding discussion leads to the philosophical question of what it means to speak of the "true" value (at a given time) of a property of an entity. This question breaks into two cases: the case in which a property is represented by a discrete variable and the case in which a property is represented by a continuous variable. With a discrete variable we can certainly speak of and sometimes even know the "true" value of the underlying property. For exam- ple, if we wish to know the number of multiple-choice questions a student answered correctly on a test, we can, if we are careful enough, know the "true" value of this number (which can be use- fully viewed as a property of the student). In the more interesting case of a continuous variable, empirical researchers usually define the "true" value of a property in terms of some commonly-agreed-upon measurement approach because this facilitates communication and understanding. For example, researchers in the physical sciences usually define the "true" values of the properties they study in terms of the definitions and standards provided by the International Bureau of Weights and Measures. To illustrate measurement standards, suppose we decide to measure the mass of physical objects using the kilogram as the unit of mass. The exact formal English version of the definition of the kilogram in the International System of Units (SI) is as follows: The kilogram is the unit of mass; it is equal to the mass of the international prototype of the kilogram (BIPM 2001a). The international prototype of the kilogram is a platinum-iridium cylinder kept under carefully controlled conditions in a labora- tory of the International Bureau of Weights and Measures in Sèvres, France. The national standards organizations of most countries of the world accept the definition that this cylinder has a mass of exactly one kilogram. Using an accurate balance it is possible to make copies the in- ternational prototype of the kilogram so that the copies have masses that are very close to the mass of the prototype. Several such copies and many copies of these copies have been made. From these copies it is possible to create other physical objects that have masses that are known multiples of one kilogram or that are known fractions of one kilogram. After we have obtained appropriate accurate masses we can use them to calibrate other very accurate mass-measuring instruments. (Such instruments, when properly calibrated, are more efficient than using a pan balance with weights.) The "true" mass in kilo- grams of any physical object is the mass we would get if we were to measure the object with a calibrated mass-measuring instrument AND 1. we had made no errors (no matter how small) in making our sec- ondary masses from the international prototype of the kilogram AND 2. we had made no errors (no matter how small) in calibrating the instrument with the secondary masses AND 3. the instrument perfectly interpolates between or extrapolates away from it calibration point(s) AND 4. the instrument has precision (at least) to the level of the mass of subatomic particles. Clearly, none of the four requirements can be satisfied. Thus even with mass -- a fundamental concept of physics -- we cannot determine the true value of this property for a given physical object to perfect precision. Nor does it seem likely that humans ever will determine the "true" mass of an arbitrary physical ob- ject or the true value of any other continuous property. However, if we are careful with our measurement procedures, we can estimate the true value of any property to a very high preci- sion, which is usually all we need. For example, currently the best mass-measuring instruments for small objects can accurately resolve ten or more significant digits of mass (BIPM 2001b). It is hard to imagine situations in which we would need more accu- racy than that. Although we can generally never know the true value of a continu- ous property of an entity, defining such "true" values is a use- ful idealization because it encourages us to strive to accurately measure the values. This leads to more accurate knowledge of re- lationships between variables, which leads to better ability to predict and control. ------------------------------------------------------- Donald B. Macnaughton MatStat Research Consulting Inc donmac@matstat.com Toronto, Canada ------------------------------------------------------- APPENDIX A: FORMALITY AND INFORMALITY IN THE PROGRESS OF SCIENCE In the body of this post I note that most empirical research pro- ceeds formally in terms of the scientific method. However, most empirical research actually proceeds quite differently, with many false starts and with frequent serendipity. But the actual pro- gression of the work is less important because the community with prime interest in a research area usually concentrates its atten- tion on the formal descriptions of empirical research in the area. (The formal descriptions are generally given in terms of the scientific method and often first appear as papers presented at meetings and then as journal articles.) The community concen- trates on formal descriptions because experience has shown that this approach is generally most efficient. In sharp contrast, at what can be viewed as the highest level of scientific thinking, the decision to accept a scientific hypothe- sis is made informally. The decision is made by the scientific community with prime interest in the area. (For example, a deci- sion about a chemical hypothesis is made informally by the commu- nity of chemists.) When scientists decide to accept a hypothe- sis, no formal declaration is ever made that the hypothesis is accepted. Instead, after perhaps a period of debate, scientists in the area simply begin speaking as if the hypothesis is an ac- cepted fact. Why are scientists so informal about the important operation of accepting a scientific hypothesis? Scientists are informal because it is risky to say formally that "such and such is so". This is because we invariably find later (perhaps years or centuries later) that "such and such" is not always "so" the way we had thought, so we must revise our think- ing, sometimes drastically. Knowledge of this leads careful thinkers to never think that something is "so". Thus scientists generally do not make formal declarations about the truth of hy- potheses and instead decide things informally. All decisions are open to revision or reinterpretation if a reasonable alternative explanation is brought forward. APPENDIX B: FURTHER DISCUSSION OF UNDEFINED CONCEPTS IN PHYSICS This appendix discusses some criticisms that might be made of my claim that the properties of 'mass', 'length', 'time', and 'tem- perature' are verbally undefined in physics and also discusses some related ideas. One could argue that the properties of 'mass', 'length', 'time', and 'temperature' are defined by the way they are measured. That is, one could argue that defining the way of measuring mass de- fines the property of 'mass'. However, humans do not generally learn these simple properties through the way they are measured. Instead, we learn them through direct experience. Thus I believe it is useful to distinguish between (a) a person sensing the property of 'mass' by lifting a physical object and (b) measuring the mass of a physical object with some (non-human) measuring instrument. I believe these are best viewed as conceptually different opera- tions, with (a) being the fundamental form, and with (b) being derived from (a) in order to objectify and refine it. Thus although we could define mass in terms of how it is meas- ured, this approach appears to yield a "secondary" definition be- cause the more fundamental concept of mass for humans is in terms of "difficulty of lifting". Thus I believe the concept of mass is best introduced in terms of the well-known (but somewhat vague) concept of the difficulty of lifting a physical object. After this introduction, we can then immediately discuss the various systems humans have invented to help us objectively meas- ure this important property of physical objects. * * * One could also argue that the property of 'mass' can be verbally defined as being equivalent to the concept of 'inertia', which is the resistance of a physical object to being accelerated by an external force. The inertial definition of 'mass' is not circu- lar, although it relies on the concepts of 'physical object', 'length', 'time', 'motion', 'differentiation' (since acceleration is usually a derivative), 'force', and 'frame of reference'. However, although this definition is used in physics (where the physical objects under study cannot always be readily weighed), it does not express the way most humans view weight or mass be- cause the definition requires that we understand mass in terms of what is effectively the concept of 'difficulty of acceleration'. But most humans do not conceptualize mass in these terms. In- stead, as I suggest above, we conceptualize mass in terms of dif- ficulty of lifting. Difficulty of lifting contains a component of acceleration and components of static and moving weight, as you can see by di- rectly sensing the mass of a moderately heavy object, such as a book. In getting a sense of the mass or weight of a book you may hold it still in your hand and sense the tension in the muscles in your arm, or you may raise it at a steady rate, sensing the amount of "work" you have to do to raise it a certain distance, or you may swing it up and down, in part sensing the difficulty of accelerating it against the gravity of the earth. However, sensing mass in terms of difficulty of acceleration is difficult because one must sense two different properties (i.e., force f and acceleration a, both of which will vary during a swing of a book) and then determine the mass by mentally dividing according to Newton's second law: f m = ---. a The complexity of sensing the two varying properties and then di- viding the value of one by the other strongly suggests that dis- criminating differences in the acceleration difficulty of mass is the most difficult of the three components for a human to sense. Since humans appear to understand mass in terms of difficulty of lifting and not in terms of difficulty of acceleration, it makes sense to view the "difficulty of lifting" sense of mass as being fundamental and to view the "difficulty of acceleration" sense as being secondary. This suggests that we should view the concept of 'mass' as being verbally undefined instead of viewing it as being defined by the inertial definition. (The inertial definition of mass is not contradictory, so we are free to adopt it, even though it may be "unnatural". If we do adopt this definition, we have not succeeded in eliminating a verbally undefined concept because the verbally undefined concept of 'mass' has been replaced by the verbally undefined concept of 'force'. For me, this replacement is unsatisfactory because 'force', being often dynamic and somewhat "unattached", is a harder concept to understand than 'mass', which is generally static, and is always directly "attached" to a physical object.) Interestingly, empirical research has shown that the mass of our everyday experience from lifting physical objects (without accel- eration) or from weighing physical objects on a standard weigh scale (which never involves direct acceleration) has a perfect linear relationship with the concept of the inertial mass of a physical object. That is, if object A "weighs" twice as much as object B, we will find that the inertial mass of object A is (to the best of our measurement capability) exactly twice the iner- tial mass of object B. The linear relationship between these two variables is an empirical fact, but need not have been -- it is not (obviously) a necessary fact. Because of the existence of this (to the best of our knowledge) perfect relationship between the two variables in everyday experience, physicists do not dis- tinguish between the two definitions of the property of "mass" when dealing with everyday experience -- both definitions effec- tively define the "same" property. * * * Although humans learn and understand the properties of 'mass', 'length', 'time', and 'temperature' through direct experience, this approach is usually not possible with more complicated prop- erties. In this case, researchers may understand a property in terms of how it is measured because observing the measurement of the values of the property may be the closest we can come to di- rectly experiencing different values of the property. For example, we cannot easily directly experience the property of the electrical resistance of a conductor of electricity. How- ever, we can indirectly intuit this property by measuring (or simply feeling) the heat dissipation when a known voltage is ap- plied across the two ends of the conductor. This is because the heat dissipation by the conductor is inversely proportional to its electrical resistance -- the higher the resistance, the lower the heat dissipation. Alternatively, we can use an ammeter to measure the size of the electric current passing through the con- ductor when a known voltage is applied across the two ends of the conductor. This is because the current is also inversely propor- tional to the resistance -- the higher the resistance, the lower the current, as given by Ohm's law. * * * When I say in the body of this post that (for example) the property of 'mass' is verbally undefined, I am not simply making the point that the standard unit of mass (i.e., the kilogram) is one of the SI base units (Cardarelli 1999, p. 7). The fact that the unit of mass is an SI base unit is a parallel point to my point that the property of 'mass' is verbally undefined. Both points arise due to the basic role of the property of 'mass' or 'weight' in human reality. * * * The National Institute of Standards and Technology (1991) gives an interesting chart showing the relationships among the impor- tant SI units. Paradoxically, these relationships between units are not relationships between properties or variables in the sense I discuss above -- they are perhaps better viewed as rela- tionships between entities (entities that are measurement units). REFERENCES BIPM [Bureau International des Poids et Mesures, International Bureau of Weights and Measures]. 2001a. "SI Base Units." Available at http://www.bipm.fr/enus/3_SI/base_units.html ---- 2001b. "Flexure-strip balances." Available at http://www.bipm.fr/enus/5_Scientific/b_mass/mass_3.html Breland, H. M., and Jenkins, L. M., 1997. English word frequency statistics: Analysis of a selected corpus of 14 million to- kens. New York: College Entrance Examination Board. Cardarelli, F. 1999. Scientific unit conversion 2d ed. London: Springer. Energy Research Advisory Board. 1989. "Cold fusion research". United States Department of Energy report DOE/S--0073. Avail- able at http://www.ntis.gov/search.htm Search for the phrase "cold fusion research" including the quotation marks. Hofmann, J. R. 1996. André-Marie Ampère. Cambridge: Cambridge University Press. Huizenga, J. R. 1993. Cold fusion: The scientific fiasco of the century. Oxford UK: Oxford University Press. Macnaughton, D. B. 1998. "Eight features of an ideal introductory statistics course." Available at http://www.matstat.com/teach/ ---- 1999. "The introductory statistics course: The entity- property-relationship approach." Available at http://www.matstat.com/teach/ National Institute of Standards and Technology. 1991. "Interpre- tation of the SI for the United States and federal government metric conversion policy (NIST Special Publication 814)." United States Department of Commerce, National Institute of Standards and Technology. Available at http://ts.nist.gov/ts/htdocs/200/202/pub814.htm Vapnik, V. N. 2000. The nature of statistical learning theory 2d ed. New York: Springer. Williams, L. P. 1970. "André-Marie Ampère." in Dictionary of Scientific Biography ed. by C. C. Gillispie. New York: Charles Scribner's Sons, pp. 139-147. ---- 1989. "André-Marie Ampère." Scientific American, 260 (1), 90-97. The URL of this page is http://www.matstat.com/teach/p0044.htm
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