The Centers for Medicare & Medicaid Services (CMS) formed its no-pay policy

 

The Centers for Medicare & Medicaid Services (CMS) formed its no-pay policy based on the growing work of National Quality Forum (NQF) of “never events.” Meaning, CMS will no longer pay for certain conditions that result from what might be termed poor practice or events that should never have occurred while a patient was under the care of a healthcare professional.

Discuss specific examples of “never events” and their impact in your workplace.
What issues are you considering for your clinical project and why?

Sample Solution

According to the National Quality Forum (NQF), “never events” are errors in medical care that are clearly identifiable, preventable, and serious in their consequences for patients, and that indicate a real problem in the safety and credibility of a health care facility. The criteria for “never events” are listed in Appendix 1. Examples of “never events” include surgery on the wrong body part; foreign body left in a patient after surgery; mismatched blood transfusion; major medication error; severe “pressure ulcer” acquired in the hospital; and preventable post-operative deaths. Clearly, paying for “never events” is not consistent with the goals of Medicare payment reforms. Reducing or eliminating payments for “never events” means more resources can be directed toward preventing these events rather than paying more when they occur. The Deficit Reduction Act represents a first step in this direction, allowing CMS, beginning in FY 2008, to begin to adjust payments for hospital-acquired infections. CMS is interested in working with our partners and Congress to build on this initial step to more broadly address the persistence of “never events.”

But that’s because I deliberately chose a non-disturbing example.  When Einstein invented General Relativity, he had almost no experimental data to go on or a phenomenon to explain, except the precession of Mercury’s perihelion.  And Einstein did not use that data, except at the end.

Einstein came up with the theory of Special Relativity using the following principle: You begin by saying, “It doesn’t seem reasonable to me that you can tell, in an enclosed box, how fast you and the box are going.  Since this number shouldn’t be observable, it shouldn’t exist in any sense.”  You then observe that Maxwell’s Equations invoke a seemingly absolute speed of wave propagation, c, commonly referred to as “the speed of light”.  So, you reformulate your physics in such fashion that the absolute speed of a single object no longer meaningfully exists, and only relative speeds exist.  I am skipping over quite a bit here, obviously, but the point still remains.

Einstein, having successfully done away with the notion of your absolute speed inside an enclosed room, then set out to do away with the notion of your absolute acceleration inside an enclosed box.  It seemed to Einstein that there shouldn’t be a way to differentiate, in an enclosed room, between the room accelerating eastward while the rest of the universe stays still, versus the rest of the universe accelerating westward while the room stays still. And because inertial mass and gravitational masses are exactly equivalent gravity can be viewed as a kind of inertia.  The Earth should then go around the Sun in some equivalent of a “straight line”.  This requires space-time in the vicinity of the Sun to be curved. And of course, the new theory had to obey Special Relativity, and conserve energy, and conserve momentum, etc.

Einstein spent several years grasping the necessary mathematics to describe curved space-time.  Then he wrote down the simplest theory that had the properties Einstein thought it should have—including properties no one had ever observed, but that Einstein thought fit in well with the character of other physical laws.

How impressive was that?

Well, let’s put it this way.  In some fraction of alternate Earths proceeding from 1800, perhaps a sizeable fraction, relativistic physics could have developed in an entirely different way. We can imagine that Newton’s original “interpretation” of the motion as relative to an absolute ether prevailed.  We can imagine that various corrective factors, themselves unexplained, were added on to Newtonian gravitational mechanics to explain the precession of Mercury—attributed, perhaps, to distortions of the ether.  Through the decades, further corrective factors would be added to account for other astronomical observations.  Sufficiently precise atomic clocks in airplanes would reveal that time ran a little faster than expected at higher altitudes and more corrective factors would be invented.

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