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Before we start implementing solutions, let s go over some of the basics involved in concurrency This is far from a complete description of threading in Mac OS X or threading in general For that, you ll need to look elsewhere We just want to explain enough for you to understand what we re doing in this chapter In most modern OSes (including of course Mac OS X), apart from the notion of a process, which contains a running instance of a program stored on disk, there s also the notion of threads of execution Each process can consist of multiple threads, which all run concurrently If there s just one processor core, the OS will switch between executing multiple threads, much like it switches between executing multiple processes If there s more than one core available, the threads will be distributed among them just like processes are.

9 The graph below shows a sequence of alpha and beta decays, labeled 1, 2, 3, and 4 Consult Table 30-1 as needed a Which represent alpha decays, and which represent beta decays b What is the overall change in mass in the sequence In the number of neutrons

A 218 1 3 214 2 212 4

210 80 82 84 Z

10 Use Appendix D to complete the two nuclear equations Include correct subscripts and superscripts for each of the particles a 32P antineutrino 15 b

235U 92

WHERE condition [,]

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All threads in a process share the same executable program code, and the same global data Each thread can also have some data that is exclusive to the thread Threads can make use of a special structure called a mutex (short for mutual exclusion) or a lock, which can ensure that a particular chunk of code can t be run by multiple threads at once This is useful for ensuring correct outcomes when multiple threads access the same data simultaneously, by locking out other threads when one thread is updating a value (in what s called a critical section of your code) For example, let s say your application implements a banking system, where an account balance can be modified as part of a transaction.

11 Write the complete nuclear equation for the beta decay of 34S 16 12 A positron is identical to a beta particle, except that its charge is 1 instead of 1 37K undergoes spontaneous positron 19 decay to form an isotope of argon Identify the isotope of argon by writing a nuclear equation 13 Iodine-131 has a half-life of 80 days If there are 600 mg of this isotope at time zero, how much remains 24 days later 14 Refer to Table 30-2 Given a sample of cobalt-60, a how long a time is needed for it to go through four half-lives b what fraction remains at the end of that time

15 The graph shows the activity of a certain radioisotope over time Deduce its half-life from this data

48 Activity 105 (Bq) 36 24 12

17 One source of a star s energy is the fusion of two deuterons to form an alpha particle plus a gamma ray

Time (h)

16 The mass of a proton and of an antiproton is 100728 u Recall that the conversion of exactly 1 u into energy yields 9315 MeV a Calculate the mass used up when a proton and an antiproton annihilate one another b Calculate the energy released here

In a multi-threaded system, you need to protect the section of code that adds or subtracts from the account balance, to eliminate the possibility that two threads are both messing with it at the exact same time Otherwise, you might have both threads reading the old balance more or less simultaneously, and both threads later writing back their own ideas of the new balance, oblivious to the changes that the.

a Write the nuclear equation for this fusion b Calculate the mass lost in this process c Calculate the energy released in MeV 18 When 1 mol (235 g) of uranium-235 undergoes fission, about 20 1010 kJ of energy are released When 40 g of hydrogen undergoes fusion, about 20 109 kJ are released a For each, calculate the energy yield per gram of fuel b Which process produces more energy per gram of fuel

1

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