In his shocking new work, this celebrated journalist investigates the burgeoning threat of nuclear-weapons technology shifting from the hands of the rich into the hands of the poor. As more unstable, undeveloped nations acquire the ultimate arms, the stakes of state-sponsored nuclear activity have soared to frightening heights.
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WILLIAM LANGEWIESCHE is the author of five previous books, Cutting for Sign, Sahara Unveiled, Inside the Sky, American Ground, and, most recently, The Outlaw Sea. He is currently an international editor for Vanity Fair and was for years a national correspondent for the Atlantic Monthly, where this book originated.
Chapter One THE VANGUARD OF THE POOR Hiroshima was destroyed in a flash by a bomb dropped from a propeller-driven B-29 of the U.S. Army Air Corps, on the warm morning of Monday, August 6, 1945. The bomb was not chemical, as bombs until then had been, but atomic, designed to release the energies that Einstein had described. It was a simple cannon-type device of the sort that today any number of people could build in a garage. It was bulbous and black, about ten feet long, and weighed ninety-seven hundred pounds. It fell nose-down for forty-three seconds and, for maximum effect, never hit the ground. One thousand nine hundred feet above the city it fired a dull gray plug of highly enriched uranium down a steel tube into a receiving lump of the same refined material, creating a combined uranium mass of 133 pounds. In relation to its surface area, that mass was more than enough to achieve “criticality” and allow for an uncontrollable chain of fission reactions, during which subatomic particles called neutrons collided with uranium nuclei, releasing further neutrons, which collided with other nuclei, in a blossoming process of self-destruction. The reactions could be sustained for just a millisecond, and they fully exploited less than two pounds of the uranium atoms before the resulting heat forced a halt to the process through expansion. Uranium is one of the heaviest elements on earth, almost twice as heavy as lead, and two pounds of it amounts to only about three tablespoonfuls. Nonetheless the release of energy over Hiroshima yielded a force equivalent to fifteen thousand tons (fifteen kilotons) of TNT, achieved temperatures higher than the sun’s, and emitted light-speed pulses of lethal radiation. More than 150,000 people died. Their executioner was an ordinary pilot named Paul Tibbets, who was twenty-nine then and is still alive now, in Ohio. He neither abhorred nor enjoyed the kill: he was a flight technician, removed from the slaughter by altitude and speed, and coddled by a pressurized, well-heated cockpit. That morning the sky was quiet, with no sign of enemy opposition. The B-29 cruised thirty-one thousand feet above the city in smooth air. It lurched and nosed upward when the bomb fell clear. Tibbets banked steeply to get away and turned the airplane’s tail on the destruction. When the bomb ignited, now far behind and below, it lit the sky with the prettiest blues and pinks that Tibbets had ever seen. The first shock wave came shimmering through the atmosphere and overtook the airplane from behind, causing a sharp bump measured at 2.5 g’s by a cockpit accelerometer. The bump felt about like the near miss of an antiaircraft burst, or the jolt of crossing a pothole in a jeep. A second shock wave then hit, but it was a reflection off the ground, like an echo of the first, and therefore even less intense. Tibbets tasted the fillings in his teeth. He saw the cloud rising over Hiroshima, and, as must be expected, he felt no regrets. Still, Hiroshima was not good for him. Though he became a brigadier general in the U.S. Air Force, and later the chairman of an executive-jet company, he suffered from the stigma of having killed so many, and he grew bitter about any implication that what he had done was wrong. It was unrealistic and probably unfair to expect him to repent, but over the decades American elites did just that, having first required him to drop the bomb. In his retirement he took to traveling around the country giving talks to war buffs and like-minded reactionaries. He showed up at air shows, I suppose to shake hands. In the 1990s, he waded angrily into a minor controversy about the Smithsonian’s display of the forward section of his airplane, the Enola Gay, and accused the elites of manipulating public opinion for their self-interest. He said he was a pilot and soldier, and by implication a simple man. He sold trinkets on the Internet, including, for $500, a beautifully rendered one-twelfth-scale atomic-bomb model mounted on a (solid, not veneer) mahogany base, and accompanied by an autographed data plate. For those with smaller budgets, he offered a sheet of thirty-six commemorative stamps picturing a B-29 soaring beyond a mushroom cloud, with excellent detail of boiling smoke on the ground. Tibbets may have been bullheaded, but at least he was consistent. When the writer Studs Terkel interviewed him in 2002, eleven months after the September 11 attacks, he did not bemoan the sadness of war or ruminate on the difficulty of facing a stateless foe, but opted true to form for a nuclear response. Against Kabul? Cairo? Mecca? He said, “You’re gonna kill innocent people at the same time, but we’ve never fought a damn war anywhere in the world where they [he meant we] didn’t kill innocent people. If the newspapers would just cut out the shit: ‘You’ve killed so many civilians!’ That’s their tough luck for being there.” Tibbets spoke from experience, and in a narrow sense he was right: it was indeed just tough luck for all the innocents who died under his wings in 1945. Those people, however, did not constitute collateral casualties—any more than the victims in the World Trade Center did. In fact Hiroshima had been chosen primarily as a civilian target and had in part been exempted from conventional firebombing to preserve it for the most dramatic possible demonstration of a nuclear strike. Three days later, the city of Nagasaki was hit by an even more powerful device—a sophisticated implosion-type bomb built around a softball-sized sphere of plutonium, which crossed the weight-to-surface-area threshold of “criticality” when it was symmetrically compressed by carefully arrayed explosives. A twenty-two-kiloton blast resulted. Though much of the city was shielded by hills, about seventy thousand people died. Quibblers claim that a demonstration offshore, or even above Tokyo harbor, might have induced the Japanese to surrender with less loss of life—and that if not, another bomb was ready. But the intent was to terrorize a nation to the maximum extent, and there is nothing like nuking civilians to achieve that effect. It’s too bad, but such is the world we live in. And cities are soft targets. More accurately, they are flammable, dense, and brittle. This goes for New York, with all its high-quality concrete and steel, and even more for the new urban conglomerations of Asia. Beyond this there are significant differences in the dynamics of nuclear blasts, dependent largely on the size of the explosion and the altitude at which it takes place. A Hiroshima-sized terrorist attack at street level in Times Square would shatter midtown Manhattan and raise a cloud of radioactive debris which would settle downwind, lethally, perhaps across Queens. By comparison a North Korean airburst of the same size a half mile above Seoul would cause still larger destruction, but result in less radioactive fallout. These variations, however, become mere details when they are measured against the common result: any city hit by a nuclear bomb will fall badly apart. And a Hiroshima-sized device now lies well within the capacities of any number of nations. When such a device ignites, the nuclear chain reaction endures for a millionth of a second. During that interval, a lethal burst of neutron particles shoots outward, penetrating walls and people in the immediate vicinity, but losing energy within a few hundred yards, as the neutrons collide with the air. Simultaneously, and for seconds afterward, a pulse of electromagnetic gamma rays, similar to light but far more powerful, flows at dangerous levels through the city to a distance of about two miles. All this would be serious enough, but it is just the start. Even in combination, these two forms of radiation (known as the initial radiation) account for only about 5 percent of the energy released by the bomb. Another 10 percent is released well after ignition, by the radioactive residue that may fall to the ground or go drifting off through the atmosphere. But all the rest of the bomb’s energy—85 percent of the yield—is transformed into air-blast and heat. Nuclear bombs of the Hiroshima size destroy cities by smashing and burning them down. These primitive effects kill almost everyone who would otherwise be dying quickly of acute radiation, then spread out to kill many more. They begin within less than a millionth of a second, when the fission process releases massive amounts of invisible X-rays, which at low altitude are absorbed by the air within a few feet. The resulting heat, rising to tens of millions of degrees, raises the pressures within the vaporizing weapon to several million times that of the surrounding atmosphere. Still within the first millionth of a second, an ultrabright fireball forms, consisting of gasified weapons residues and air. The fireball brutally expands and simultaneously rises. Within three seconds of a twenty-kiloton explosion, it reaches its maximum size, about 1,500 feet across. If it touches the ground (whether because the ignition point was on a street, or at less than 750 feet overhead), it vaporizes the earth and all structures that it encounters and begins to loft large quantities of dirt and debris into a violently rising, intensely radioactive column. Rising in that column along with all the ash and earth are hundreds of by-products of the fission, many of which are radio-active, but a good number of which decay so rapidly that they reach the end of their radioactive lives before they settle again to the ground. Rapid decay is a common characteristic of the most radioactive fission by-products. Seven hours after ignition, the emissions of the fallout are approximately one-tenth as strong as at the one-hour mark; after two days, the radioactivity has bled away to mer...
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