Charles Vernon Coffman
Carnegie Mellon University
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Archive for Rational Mechanics and Analysis | 1989
Charles Vernon Coffman; Moshe Marcus
A foot clamping device for ski boots comprises, inside the boot body a presser member at the foot heel region and a threaded peg extending from the presser member and rotatably engaged in a threaded bush associated with a boss on the outside of the boot body. When the boss is rotated by a strap rigid therewith and constituting a closure element for the boot, the presser member is caused to traverse.
Journal of Mathematical Biology | 1978
Charles Vernon Coffman; Bernard D. Coleman
SummaryThe general theory discussed by Colement in the first paper, I, of this series is here specialized to the case in which the rate, ρ=ρ(x(a,t), a) at which a population loses, through death and dispersal, individuals of agea is convex in the numberx(a, t) of individuals which have agea at timet, while the fecundity functionF in the formula,x(0,t)=F(x(af, t)), is concave inx(af, t); hereaf is the reproductive age. Such an assumption of convexity for ρ(·,a) and −F(·) renders mathematical the idea that when one considers the immediate contribution which an additional individual, of given age, makes to those processes which tend to increase the population, one should find that such an incremental contribution declines as the number of present individuals at the given age increases. It is shown that convexity of ρ(·,a) and −F(·) implies that a given population belongs to one of three classes, regardless of initial conditions: (i) the class of ‘endangered populations’ for whichx(a, t)→0 ast→∞, (ii) the class of populations with a stable, non-zero, stationary age distribution, or (iii) the class of populations which exhibit unbounded growth. The properties of ρ andF which determine the class to which a population belongs are found and discussed in detail. For example, when ρ(0,a)∈0 andF is monotone increasing withF(0)=0, the parameter,
Journal of Functional Analysis | 1980
Charles Vernon Coffman; Carole L Grover
Journal of Functional Analysis | 1973
Charles Vernon Coffman
T = \ln \frac{d}{{dx}}F(0) - \int_0^{a_f } {\frac{\partial }{{\partial x}}} \rho (0,a)da,
Nonlinear Analysis-theory Methods & Applications | 1988
Charles Vernon Coffman
Advances in Applied Mathematics | 1980
Charles Vernon Coffman; Richard James Duffin; Greg Knowles
, introduced in I, plays a central role: whenT is negative the population is of class (i); whenT is positive the population is of either class (ii) or class (iii), and it is then of class (ii) if and only if the parameter,
Journal of Mathematical Biology | 1979
Charles Vernon Coffman; Bernard D. Coleman
Journal of Differential Equations | 1974
Charles Vernon Coffman; Juan Jorge Schäffer
U = \mathop {\lim }\limits_{x \to \infty } \left[ {\ln \frac{d}{{dx}}F(x)} \right] - \int_0^{a_f } {\mathop {\lim }\limits_{x \to \infty } } \frac{\partial }{{\partial x}}\rho (x,a)da,
Journal of Differential Equations | 1975
Charles Vernon Coffman
Transactions of the American Mathematical Society | 1991
Charles Vernon Coffman
obeys the condition −∞≤U<0.