March 25, 2000
To facilitate making and understandings of models, scientists have agreed on the definitions of many physical quantities. Scientists know many physical quantities, which are classified into basic and derived. Basic quantities are undefined (unknown), while the derived quantities are defined in terms of the basic. The basic quantities are length, time, mass, charge, temperature, and the amount of substance. Although the basic quantities are undefined, the ratio of basic quantities of the same type is defined. For example, the ratio of masses may be defined as the ratio of gravitational accelerations they create at a fixed distance. A value of a basic quantity is written as a product of the value of the quantity for a specified object (the value is called unit) and a real number. Because the quantities are unknown, we can apply dimensional analysis (essentially checking that the unknown part of a physical quantity (unit) is in a proper form).
Since not defining quantities is bad, as few quantities as possible should be left undefined. From all physical quantities, the real number is the only truly basic and indefinable quantity.  Other scalar physical quantities can and should be defined as real numbers (since no good alternatives exist). Doing so requires a numerical specification of the basic physical quantities. This is best achieved by setting the fundamental physical values to 1. The values probably are c, G, ħ, e (charge of proton), k (Boltzmann's constant), and NA.
When the definitions (and all formulas that follow from them) are not used, the dimensional analysis can be applied completely. Using any of the formulas, however, restricts the application of dimensional analysis.
March 25, 2000
Physical quantities are defined in each physical model. To make understanding of physical models simpler, physicists agreed on definition/perception of the physical quantities common to many models. Therefore, physicists define/introduce physical quantities and they should decide whether defining physical quantities as described in the New Perception of Physical Quantities is better than leaving the physical quantities undefined as currently is.
Defining physical quantities will simplify the calculations since instead of the fundamental (and widely used) physical constants you can use 1. Dimensional analysis can still be completely used in a particular problem unless 1 is used instead of 'the conventional value' of a fundamental physical constant. If 1 is used as value of some fundamental constants but not all, dimensional analysis will be restricted but valid. Therefore, if dimensional analysis is more important than using some of the fundamental physical constants as one, the dimensional analysis can be completely applied by not using 1 as a value of some fundamental physical constants. Thus, the New Perception of Physical Quantities is at least the same and sometimes better than the Classical Perception of Physical Quantities in this aspect.
Another aspect is how natural, simple, and logical the perceptions are. The new perception is simpler than the classical since c, G, ħ, e, k, and NA do not complicate it. The new perception is also more natural since it defines physical quantities. Several other insights support this conclusion. For example, energy and mass are identical from the physical point of view yet different in the classical perception. Recall that Euclidean 4-dimensional space-time is a set of all ordered quadruples of real numbers. It is natural to model our universe by Euclidean space-time. The classical perception prevents it since distance and time are not real numbers in it.
In chemistry, it is very convenient to say that the charge of electron is -1 so that chemists can easily pronounce and write the charges of ions. This is allowed in the New Perception of Physical Quantities but not in the classical.
The final aspect is the validity of physical models as mathematical theories. Since physical quantities are undefined in the classical perception, they cannot be used in any valid physical models (that is mathematical theories which correspond to some events in our world). This defeats the purpose of introducing physical quantities. In the New Perception of Physical Quantities, physical quantities can and should be used.
These arguments show that physicists should choose the New Perception of Physical Quantities instead of what they have now--the Classical Perception of Physical Quantities.
March 25, 2000
In the Classical Perception of Physical Quantities, physical quantities are undefined simply because the definitions do not exist. Some fallacies may, however, resemble definitions. The first and perhaps the most important fallacy is "defining" a physical quantity in terms of undefined quantities. If the "definition" is pursued by trying to define the undefined terms, circular definitions will soon be reached. For Example: "M≡ar2/G, G≡6.67...*10-11m3/(kg*s2), kg≡ M for which ar2 is 6.67m3/s2. M is mass; a is the gravitational acceleration the body creates at distance r from the body." Another fallacy is defining quantities other than the quantity whose definition has to be found. Often, it is defining a quantity proportional to the given one such as the quantity over its units. For example: "Mass is the number of kilograms a body has." A third fallacy is giving information about the quantity in insufficient amount to define it: "Mass is a measure of how strongly an object curves space time."
Exercise: Create the 3 fallacies for temperature. (If you do not know enough about temperature, read several paragraphs before you do the exercise. In several paragraphs, temperature will be defined.)
A stronger statement can be given in the Classical Perception of Physical Quantities: No physical quantities that have dimensions can be defined from a set of physical quantities not containing a component of the dimension. This is a direct implication of dimensional analysis--a quantity cannot be equal to a combination of quantities not containing a component (such as mass) of the quantity.
The New Perception of Physical Quantities provides the framework for defining all physical quantities. Our universe can be represented by a set of all ordered quadruples of real numbers, (x, y, z, t). The New Perception of Physical Quantities provides the scaling between this representation and our universe. Distance, D((x1,y1,z1,t1), (x2,y2,z2,t2)) ≡ ((x2-x1)2+(y2-y1)2+(z2-z1)2). Time, T((x1,y1,z1,t1),(x2,y2,z2,t2)) ≡ |t2-t1|. Proper distance is defined as sqrt(D2-T2) provided that the D>T. Proper time is defined as sqrt(T2-D2) provided that the T>D. As in the Classical Perception of Physical Quantities, r≡(x,y,z), v≡dr/dt, a≡dv/dt.
According to the law of universal gravitation, the product of a (curvature of space-time created by the body) and D2 (D is distance to the body) for each body is independent of location provided that D is much larger than the size of the body and the body is not moving with a relativistic speed. Mass, M≡aD2 for a stationary object. For a moving object, M≡γMo where Mo (called rest mass) is defined as mass of the object if it was stationary, and γ≡sqrt(1-v2). As in the Classical Perception of the Physical Quantities, p≡M*v, F≡dp/dt, ρ≡dM/dV. E≡M, P≡dE/dt.
Temperature (T) of a monatomic ideal gas is defined to be 2/3*E, where E is the average translational kinetic energy of its molecules. Temperature of an object other than a monatomic ideal gas is defined to be the temperature that a monatomic ideal gas would possess if it would be in thermal equilibrium with the object.
Defining electric charge has some difficulties because of the incomplete information known. Perhaps, it should be defined separately in each model. The following is a reasonable definition. It is unclear, however, whether it is a definition or merely a specification that is valid only in some models. Let electric field (E) be defined as the negative of the force that acts on an electron at rest. Let charge, q≡ F/E. Anyway, the New Perception of Physical Quantities allows electric charge to be defined as an experimental quantity (that is determinable by experiment) in any appropriate model.
Some other quantities can be defined as real numbers. The amount of substance is defined as the number of molecules in the given sample. Thus, 1mole=6.0...*1023 and NA=6.0...*1023/mol=1. Consequently, R=NA*k=k=1. Information that can be stored in a system that can have N independent states is defined as log2N.
Real numbers too need to be defined. Several ways exist to do this. The following is a good way to define real numbers: A real number (X) is defined to be an integer (m) or an integer with infinitive sequence of 0 and 1 (f(n)) so that for at least one n, f(n)=1, and there is no n such that f(k)=1 for every k>n. The restrictions on f(n) are necessary to ensure that real numbers that are different by this definition are unequal. X=m+Σ(2-nf(n), n,1, ∞). The equation is not part of the definition of real numbers. It is simply used to connect the definition to some operations that we know on real numbers.
Solution to the exercise: First, we will take some steps in the right direction. Temperature of an object other than a monatomic ideal gas is defined to be the temperature that a monatomic ideal gas would possess if it would be in thermal equilibrium with the object. Consequently, I will give fallacies for monatomic ideal gas. Let E be the average translational kinetic energy of its molecules. Using the first fallacy, let T be "defined' as 2/(3k)*E where k≡1.38...J/K where K≡ 1/273.16 of the temperature at which the triple point of water occurs. Using the second fallacy, temperature is the number of Kelvin thermometers will measure. (Although the fallacy is stated informally, it can be formalized to define T/K.) Using the third fallacy, temperature is a measure of hotness or coldness a body possesses.
Here I will explain how to convert a physical quantity to the "dimensions" you wish it to have. To do so, you multiply it by clGmħneokpNr (subscript 'A' is ommited from n) so that the dimensions are proper. Let the original dimension be X and the needed one--Y. In effect, you need to solve (Y/X)=clGmħneokpNr. The equation can be solved by separating the dimensions into components: length, time, mass, electric charge, temperature, and the amount of substance. Then you will get a separate equation for each component. Solving the system of equations, you will obtain l, m, n, o, p, and r. In a few cases, you will have to perform the procedure several times such as if the quantity is given as a sum of 2 quantities with different dimensions.
Exercise:Convert the sentence
to the Classical Perception of Physical Quantities:
"Evidence shows that the most fundamental length, time, and mass are 1."
Solution: length=1=clGmħneokpNr. Since no component of length, c, G, or ħ is electric charge, temperature or amount of substance, 'o', 'p', and 'r' are 0. 1=clGmħn. D=(D/T)l (D3/(M*T2)m (M*D2/T)n, D1T0M0=Dl+3m+2n T-l-2m-n M-m+n, 1=l+3m+2n and 0=-l-2m-n and 0=-m+n, m=n and 1=l+5n and 0=-l-3n, 1=2n, n=1/2 and m=1/2 and 1=l+2.5, l=-3/2, length is c-3/2G1/2ħ1/2. The time =1=(distance 1)/c= c-5/2G1/2ħ1/2. The mass = 1=clGmħneokpNr. Since no component of mass, c, G, or h is electric charge, temperature, or the amount of substance, o=0, k=0, and r=0. M=clGmħn. M=(D/T)l (D3/(M*T2)m (M*D2/T)n, D0T0M1=Dl+3m+2n T-l-2m-n M-m+n, 0=l+3m+2n and 0=-l-2m-n and 1=-m+n, 0=m+n and n=m+1, 2m+1=0, m=-1/2, n=1/2, l=1/2, the mass is c1/2G-1/2ħ1/2. Thus, the sentence will be: "Evidence shows that the most important length is c-3/2G1/2ħ1/2, time -- c-5/2 G1/2ħ1/2, and mass -- c1/2G-1/2ħ1/2."
Exercise:Find the formula for
proper length and proper time in the Classical Perception of Physical
Answer: Proper length is sqrt(D2-c2T2). Proper time is sqrt(D2-c2T2)/c.
Exercise: What is the value (using no units) of Coulomb's constant (8.988...m/F)?
Answer: 0.007297... .
Dimensional analysis forbids logs
from dimensional quantities. Otherwise, ln(2m3) = ln(2*1m3)=ln
2+ln(1m3). Thus ln(x) would have to be dimensionless. Then, x=eln
x would have to be dimensionless as well leading to contradiction if x
has dimensions. Thus, for example,
∫dV/V≠ ln V+C since ln is not defined for dimensional quantities. This problem does not occur in the New Perception of Physical Quantities, since all quantities are dimensionless.
Dimensions can be formally defined as the sequence of exponents for each basic unit in a quantity. For example, force has dimensions (1, 1, -2, 0, 0, 0) corresponding to mass1*length1* time-2*charge0*temperature0*(amount of substance)0.
The fundamental constants chosen to be one must have linearly independent dimensions. Otherwise, one constant could be expressed from the others causing 2 quantities with the same dimension but different values in SI units be equal--a contradiction. The number of constants must equal the number of dimensions so that all units could be expressed as a combination of these constants. The constants chosen above satisfy the properties.
Sometimes, something that looks like a unit is really a part of the type of quantity. For example: "The distance between the 2 genes on a chromosome is a morgans." "Morgans" specifies distance leading to the quantity type "the probability of crossing over between the 2 genes" and the value a. (Of course, units are parts of physical quantities, 1m≠1.)
 Definitions are sometimes incomplete, may change with new insights, and may differ slightly depending on a scientist.
 Actually, real numbers can be defined in terms of integers. Integer is the basic quantity.