323 karma · joined June 21, 2012
A tourist walking around with their phone in a selfie stick has put preparation and forethought into the endeavor. Before leaving their hotel to see some wonder of the world, they consciously thought, "I'm going to take a bunch of selfies today so I can post them on social media and gain influence because I'm somebody." This attitude represents everything many people blame for giving rise to the modern overcrowded tourist destination experience.
I'm sure there exceptions, and some people just like pictures with themselves in them, but this is the impression it gives off. You asked why people hate selfie sticks, and this is a likely reason.
For the case you suggested above, this is essentially how run-flat tires work. Of course, the sidewall of the tire isn't as stiff as the support ring, but they do provide some support.
You should be able to estimate this contribution by fitting to the curve of area vs pressure at lower pressures. For example, the linear F=PA relationship clearly breaks down at 0 pressure, as F>0 and A>0 when P=0.
Even lasers spread. This guy agrees with me: https://www.quora.com/Is-the-light-from-lasers-reduced-by-th...
Concerning the general question of dimensionality and numbers vs. functions, I'm afraid I still don't understand the fundamental issue. I agree that probability notation isn't the best, but each of those terms can be replaced with a Gaussian (or in the case of the denominator, an integral of the product of two Gaussians). You end up with a function in terms of x_k and the sequence of z's. You can then choose which variables are free or bound and evaluate the function as your application requires. If all variables are bound (the case that you know the measurement z_k, and are evaluating the posterior probability of the state at a given point), all the terms are numbers (yes, densities), and there are no dimensional issues. If you leave x_k free, you end up with two functions in the numerator, and a number in the denominator. Those two functions are Mahalanobis distances (which are scalars) in an exponent, and again, no dimensional issues. In general, such operations with PDFs represent various combinations and manipulations of event spaces that need not be commensurate. Computing the PDF of a coin flip given the distribution of all of the positions and velocities of the molecules of air through which the coin flies requires comparing a two-state PMF to a virtually infinite dimensional PDF. Notationally speaking, no problem.
The equation in question is P(A|B) = P(B|A) P(A) / P(B). In modern Kalman filter literature, this would be stated as something like: P(x_k | z_k) = P(z_k | x_k) P(x_k) / P(z_k). It is generally left as implicit in these sorts of equations that everything is also conditioned on the sequence z_1 to z_{k-1}. In this equation, x_k is a free variable in the state space (possibly multi-dimensional, so a vector), while z_k is the measurement, which is a realization of the random variable distributed as N(H(x_k), R_k). The result is a PDF over the free variable x_k.
So let's tackle the terms one by one:
1. P(z_k | x_k) - this is the probability that we measured z_k, given that the true object is at x_k. This is the aforementioned normal distribution N(H(x_k), R_k).
2. P(x_k) - this is the prior probability of the state estimate, generally after propagation through the motion model from P(x_{k-1} | x_{k-1}). In the Kalman filter, this is also Gaussian, and conveniently has the same mean as the term above (see note below).
3. P(z_k) - this is the denominator that someone else mentioned earlier can be effectively ignored, which is right - you only need it to normalize the numerator. If you must compute it, it can be factored as the integral over the entire state space of P(z_k|x_k)*p(x_k). Given z_k, this is a number, not a function.
4. P(x_k | z_k) - The result, which is a Gaussian PDF. You can arrive at it numerically by plugging in specific values for x_k, in which case (1) and (2) are numbers. Or symbolically, in which case (1) and (2) are functions, and you'll end up with the form of a Gaussian PDF.
Note: The original article quotes a distribution for the product of two Gaussians with arbitrary means. It does not state that this is an approximation, which is exact only in the case of equal means. This is why unbiased measurements are one of the Kalman assumptions.
Copyright and patent are both intended to encourage innovation by providing the originator with a temporary monopoly on the use of works/processes/etc. Both are frequently discussed here in the context of large corporations/publishers using them to stifle the innovation they were designed to encourage.
Trademarks are often used in tandem with copyrights to protect a body of work in different ways - while "Steamboat Willy"s copyright will eventually expire (if it hasn't already), the trademark of the Mickey Mouse character will last indefinitely (so long as Disney protects it).
Distinctive trademarks are also commonly protected by design patents. Yes, they protect the work in different ways, but the two are related in their use and concept.
If you're so against collective terms, I hereby insist that you no longer refer to the "United States", or "European" culture. But I digress.