Hysteresis Analysis ©
by: Howard L. Schriefer, BSME, MSE, PE
Hysteresis literally means "belated". In science, hysteresis is the mark of irreversibility because hysteresis results in a return process which differs from the original process. A reversible process is similar to driving from Baltimore, MD to Washington, DC and back on I-95; while an irreversible process would be similar to driving from Baltimore, MD to Washington, DC on I-95, and returning via US 1. Expansion and contraction processes in science are often referred to as reversible or irreversible. This analysis compares processes involving expansion and contraction. Specifically, we are comparing the expansion and subsequent contraction to the contraction and subsequent expansion of a given general sphere having a dimensionless (no assigned units) radius.
Before we begin computing, let us recall from calculus that the change in volume of a sphere with respect to its radius is the derivative of the spherical volume with respect to its radius. Interestingly, this derivative is numerically equal to the current spherical surface of the spherical volume. Since the general sphere we herein consider is dimensionless, we can add or subtract the spherical surface to/from the spherical volume. We want to change the spherical volume by one spherical surface because this is the smallest increment for change. In fact, any change less than one spherical surface would render the sphere "unspherical". Intuitively speaking, adding or subtracting less than one full surface to/from the sphere would result in a bump/dent on an otherwise spherical object.
In this computation, we compare the intermediate steps of the expansion and the contraction of the same original spherical volume, by adding and subtracting, respectively, the spherical surface to/from the spherical volume. Subsequently, we compare the final steps of the contraction and the expansion of the previously expanded and previously contracted spheres by subtracting and adding, respectively, the spherical surface from/to the spherical volume.
DIMENSIONLESS SPHERICAL DIAMETER
PRE-EXPANSION SPHERICAL RADIUS
PRE-CONTRACTION SPHERICAL RADIUS
PRE-EXPANSION SPHERICAL VOLUME
PRE-EXPANSION SPHERICAL SURFACE
POST-EXPANSION SPHERICAL VOLUME
POST-EXPANSION SPHERICAL RADIUS
POST-EXPANSION SPHERICAL SURFACE
SUBSEQUENT CONTRACTION EXPANDED VOLUME
SUBSEQUENT CONTRACTION EXPANDED RADIUS
PRE-CONTRACTION SPHERICAL VOLUME
PRE-CONTRACTION SPHERICAL SURFACE
POST-CONTRACTION SPHERICAL VOLUME
POST-CONTRACTION SPHERICAL RADIUS
POST-CONTRACTION SPHERICAL SURFACE
SUBSEQUENT EXPANSION CONTRACTED VOLUME
SUBSEQUENT EXPANSION CONTRACTED RADIUS
RATIO OF ORIGINAL RADII
RATIO OF EXPANDED RADIUS TO CONTRACTED RADIUS
RATIO OF RADIUS OF SUBSEQUENTLY CONTRACTED RADIUS
AFTER EXPANSION TO RADIUS OF SUBSEQUENTLY EXPANDED
RADIUS AFTER CONTRACTION
Comparison of the intermediate and the final volumes resulting from the above process shows that the two processes represent quite different paths. It can be said that, in this general example, neither the expansion/contraction process of a dimensionless sphere and the contraction/expansion process of a dimensionless sphere return the sphere to its original volume; and furthermore, the process paths are incongruent.
It is also noteworthy that a value greater than 3 (three) is required for positive volume to result in the contraction process. We can deduct from this observation, that while expansion is theoretically limitless, a finite nonzero boundary exists for contraction of a general dimensionless sphere resulting in positive volume. As the radius of the original spherical volume is increased, the incongruencies become less noticeable.
Consequently, we have demonstrated, with simple mathematics, the irreversibility of hysteresis which is observable in heat transfer, thermodynamics, electricity, magnetism, material strain, and other physical processes.
Now consider a sphere which expands by one surface to a volume and then contracts by one surface to a volume. It will be seen that the expansion/contraction process is irreversible. In this case, allow for elimination of units by setting the initial radius at the limit dimensionless value 3. Therefore, any dimensioned linear radius must be divided by 3 in order to find the associated linear scale factor. The transmission/reception pod associated with the radius will then be dimensionless e1/e in cross-sectional radius. The half wavelength for the transmission/reception pod is equal to the radius of its respective sphere.
PRE-EXPANSION SPHERICAL RADIUS = 3
INITIAL SPHERICAL VOLUME
INITIAL SPHERICAL SURFACE
INITIAL SPHERICAL VOLUME
POST-EXPANSION SPHERICAL RADIUS
EXPANSION WAVELENGTH
INITIAL POD MAXIMUM SECTION RADIUS
POST-EXPANSION POD MAXIMUM SECTION RADIUS
POD SECTION STEP
AREA OF POD SECTION STEP
PRE-CONTRACTION SPHERICAL RADIUS
PRE-CONTRACTION SPHERICAL VOLUME
PRE-CONTRACTION SPHERICAL SURFACE
POST-CONTRACTION SPHERICAL VOLUME
POST-CONTRACTION SPHERICAL RADIUS
POST-CONTRACTION SPHERICAL SURFACE
CONTRACTION WAVELENGTH
INITIAL POD MAXIMUM SECTION RADIUS
POST-CONTRACTION POD MAXIMUM SECTION RADIUS
POD SECTION STEP
AREA OF POD SECTION STEP
RATIO OF EXPANDED TO CONTRACTED SECTION STEP AREA
RATIO OF INITIAL TO EXPANDED/CONTRACTED SPHERICAL RADIUS
RATIO OF INITIAL TO EXPANDED/CONTRACTED SPHERICAL SURFACE
RATIO OF INITIAL TO EXPANDED/CONTRACTED SPHERICAL VOLUME
RATIO OF EXPANSION TO CONTRACTION WAVELENGTH