By A.S. Kompaneyets

A process Theoretical Physics, quantity 2. Statistical legislation: Statistical Physics, Hydrodynamics and gasoline Dynamics, Electrodynamics of constant Media, actual Kinetics. writer: A. S. Kompaneyets. MIR Publishers, Moscow.

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Extra info for A course of theoretical physics, vol.2: statistical laws

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The new type of objects are constructed by the function symbol 'const', which takes n arguments. The sense in which this type is "new" is that objects constructed by 'consf are not Booleans, numbers, literal atoms, conses, or any previously mentioned shell. , was constructed by 'const'. An object of this new type may be thought of as an n-tuple containing the n arguments passed to 'const' to construct the object. The n accessor function symbols may be used to recover these n components from such an object.

The second, ( p u s h - c o n s t a n t ( n a t 4 ) ) , pushes the natural number 4 onto the temporary stack. The third, ( a d d - n a t ) , pops the topmost two items off the temporary stack, adds them together (expecting both to be naturals), and pushes the result onto the temporary stack. The last instruction returns control to the calling environment. The sum just computed is on top of the stack and is considered the result. In summary, this silly program adds 4 to the value of its second argument and ignores the other arguments.

But it is impossible to deposit anything at a program address (just as it is impossible to transfer control to a data address). The program counter component of a p-state is an object of this type. For example, to start a computation at the first instruction of the program named main, the program counter in the state should be set to (pc (main . 0 ) ) . 7. Subroutines A Piton subroutine name is just a name. To be legal, it must be the name of some program in the program segment. Subroutine names are written ( s u b r name).

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A course of theoretical physics, vol.2: statistical laws by A.S. Kompaneyets
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