This equation tells us which is the best shop to visit on a bank holiday.
This equation tells us where is the best place to go on a first date.
This equation tells you that if you want a certain amount of power, then the higher the voltage you use, the lower the current you need.
See, this equation tells us which is the best late-night junk food, because that's an important thing to know about.
"If you're choosing your career, it matters if you care a little bit more about making a social contribution than you do about mastering some skill set," Christianne Corbett, a co-author of "Solving the Equation," told me.
This equation tells us how the peak arising from a click travels along the cochlea.
The latter equation tells us that along with the vertical magnetic field Sq and tidal horizontal electric fields are continuous across the air sea interface.
The above equation tells us that the exposure in state 1, for example Nuevo Leon, depends on the exposure per municipality in that state and how large this municipality is in relation to the whole state.
The linearity assumption then implies that this holds for arbitrary input signals f. Since H ˆ commutes with both A ˆ and B ˆ, the basic equation tells us that a ∂ ∂ a H W f ( a, t ) = κ H W f ( a, t ) − α W f ( a, t ) − a β ∂ ∂ t H W f ( a, t ) + a κ ∂ ∂ t W f ( a, t ).
Now, it follows from (3.1), above, that there are states of S (too many to count) which are not eigenstates of A, and if we consider what Schrödinger's equation tells us about the joint evolution of S and S* when S is started out in one of these, we find that the state of the pair after interaction is a superposition of eigenstates of [A on S & B on S*].
