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E=MC!! 337<br />

by the best brains of all countries and all times. In solitude,<br />

and yet in cooperative effort as regards the final effect, they<br />

created the spiritual <strong>to</strong>ols for the technical revolutions which<br />

have transformed the life of mankind in the last centuries.<br />

Their system of concepts has served as a guide in the bewildering<br />

chaos of perceptions so that we learned <strong>to</strong> grasp general<br />

truths from particular observations.<br />

What hopes and fears does the scientific method imply for<br />

mankind? I do not think that this is the right way <strong>to</strong> put the<br />

question. Whatever this <strong>to</strong>ol in the hand of man will produce<br />

depends entirely on the nature of the goals alive in this mankind.<br />

Once these goals exist, the scientific method furnishes<br />

means <strong>to</strong> realize them. Yet it cannot furnish the very goals.<br />

The scientific method itself would not have led anywhere, it<br />

would not even have been born without a passionate striving<br />

for clear understanding.<br />

Perfection of means and confusion of goals seem-in my<br />

opinion-<strong>to</strong> characterize our age. If we desire sincerely and<br />

passionately the safety, the welfare, and the free development<br />

of the talents of all men, we shall not be in want of the means<br />

<strong>to</strong> approach such a state. Even if only a small part of mankind<br />

strives for such goals, their superiority will prove itself in the<br />

long run.<br />

E=MC'<br />

From Science-illustrated, New York, April, 1946.<br />

In order <strong>to</strong> understand the law of the equivalence of mass<br />

and energyJ we must go back <strong>to</strong> two conservation or Hbalance"<br />

principles which, independent of each other, held a high place<br />

in pre-relativity physics. These were the principle of the conservation<br />

of energy and the principle of the conservation of<br />

mass. The first of these, advanced by Leibnitz as long ago as<br />

the seventeenth century, was developed in the nineteenth<br />

century essentially as a corollary of a principle of mechanics.<br />

Consider, for example, a pendulum whose mass swings back<br />

and forth between the points A and B. At these points the<br />

mass m is higher by the amount h than it is at C, the lowest<br />

point of the path (see drawing). At C, on the other hand,

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