Dimensional Reasoning. “Dimension” is characteristic of the object, condition, or event and is described quantitatively in terms of defined “units”. A physical quantity is equal to the product of two elements: A quality or dimension A quantity expressed in terms of “units” Dimensions
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A physical quantity is equal to the product of two elements:
A quality or dimension
A quantity expressed in terms of “units”
Physical things are measurable in terms of three primitive qualities (Maxwell 1871)
Note: (Temperature, electrical charge, chemical quantity, and luminosity were added as “primitives” some years later.)Dimensions and Measurements
distance s = s0 +vt2 + 0.5at3
constant = p + ρgh +ρv2/2
volume of a torus = 2π2(Rr)2
mDimensional analysis (cont.)
Possible variables: length l [L], mass m [M], gravity g
i.e. period P = f(l , m, g)
Period = [ T ], so combinations of variables must be equivalent to [ T ].
Only possible combination is
Note: mass is not involved
Example: it is meaningless to say that a board is “3” long. “3” what? Perhaps “3 meters” long.
Units can be algebraically manipulated (like dimensions)
Conversions between measurement systems can be accommodated, e.g., 1 m = 100 cm,
Example: in the pendulum, the variables were time [T],
gravity [L/T2], length [L], mass [M] . So, n = 4 k = 3. So, only one dimensionless group describes the system.
where a,b,c,d are coefficients to be determined.
In terms of dimensions:
a - 2c = 0
b + c = 0
d = 0
Arbitrarily choose a = 1. Then b = -1/2, c = 1/2, d = 0.
A star undergoes some mode of oscillation. How does the frequency of oscillation ω depend upon the properties of the star? Certainly the density ρ and the radius R are important; we'll also need the gravitational constant G which appears in Newton's law of universal gravitation. We could add the mass m to the list, but if we assume that the density is constant, then m = ρ(4πR3/3) and the mass is redundant. Therefore, ω is the governed parameter, with dimensions [ω] = T-1, and (ρ; R; G) are the governing parameters, with dimensions [ρ] = ML-3, [R] = L, and [G] = M-1L3T-2 (check the last one). You can easily check that (ρ; R;G) have independent dimensions; therefore, n = 3; k = 3, so the function Φ is simply a constant in this case. Next, determine the exponents:
[ω] = T-1 = [ρ]a[R]b[G]c = Ma-cL-3a+b+3cT-2c
Equating exponents on both sides, we have a - c = 0; -3a + b + 3c = 0; -2c = -1
Solving, we find a = c = 1/2, b = 0, so that ω = C(Gσ)1/2, with C a constant. We see that the frequency of oscillation is proportional to the square root of the density, and independent of the radius.
Example: speed V (m/s) can be made "dimensionless“ by dividing by the velocity of sound c (m/s) to obtain M = V/c, a dimensionless speed known as the Mach number. M>1 is faster than the speed of sound; M<1 is slower than the speed of sound.
Other examples: percent, relative humidity, efficiency
Equations and variables can be made dimensionless, e.g., Cd = 2D/(ρv2A)
Dimensionless equations and variable are independent of units.
Relative importance of terms can be easily estimated.
Scale (battleship or model ship) is automatically built into the dimensionless expression.“Dimensionless” Quantities
Example: Convert a dimensional stochastic variable x to a
to represent its position with respect to a Gaussian curve--N(0,1),
e.g., grades on an exam
The area of any triangle depends on its size and shape, which can be unambiguously identified by the length of one of its edges (for example, the largest) and by any two of its angles (the third being determined by the fact that the sum of all three is π). Thus, recalling that an area has the dimensions of a length squared, we can write:
area = largest edge2 • f (angle1, angle2),
where f is an nondimensional function of the angles.
Now, referring to the figure at right, if we divide a right triangle in two smaller ones by tracing the segment perpendicular to its hypotenuse and passing by the opposite vertex, and express the obvious fact that the total area is the sum of the two smaller ones, by applying the previous equation we have:
c2 • f (α, π/2) = a2 • f (α, π/2) + b2 • f (α, π/2).
And, eliminating f:
c2 = a2 + b2, Q.E.D.
Geometric similarity – linear dimensions are proportional; angles are the same.
Kinematic similarity – includes proportional time scales, i.e., velocity, which are similar.
Dynamic similarity – includes force scale similarity, i.e., equality of Reynolds number (inertial/viscous), Froud number (inertial/buoyancy), Rossby number (inertial/Coriolis), Euler number (inertial/surface tension).Scaling, modeling, similarity
Sometimes it’s necessary to violate geometric similarity: A 1/1000 scale model of the Chesapeake Bay is ten times as deep as it should be, because the real Bay is so shallow that, with proportional depths, the average model depth would be 6mm, too shallow to exhibit stratified flow.Scaling, modeling, similarity