Abstract
In our final reading selection from Galileo’s Dialogues, we find Salviati, Sagredo and Simplicio in the midst of a discussion of the motion of projectiles. By treating a projectile’s motion as a combination of uniform motion in the horizontal direction, and naturally accelerated motion in the vertical direction, they have discovered that its path forms one of Apollonius’s conic sections: the parabola. But can one determine the speed of the projectile at any and every point along its trajectory? How can it be calculated and what determines the force of impact? These are the questions to which they now turn.
For velocities, just as for intervals of time, there is need of a common standard which shall be understood and accepted by everyone, and which shall be the same for all.
—Galileo Galilei
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- 1.
See page /206/.—[K.K.].
- 2.
Galileo here proposes to employ as a standard of velocity the terminal speed of a body falling freely from a given height. [Trans.].
- 3.
Galileo often uses the same line segment to represent both a distance, a time and even a speed. This may not seem strange if one recognizes that the same number (6 for example) can be used to represent both an amount of time (6 s) and a distance (6 m). Of course Galileo could have drawn two separate diagrams, one for distances and one for time, but he chose a more compact representation.—[K.K.].
- 4.
Galileo must here have meant to say that the speed does not vary in proportion to the height.—[K.K.].
- 5.
See Theorem II, Proposition II.—[K.K.].
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Kuehn, K. (2015). The Speed and Force of a Projectile. In: A Student's Guide Through the Great Physics Texts. Undergraduate Lecture Notes in Physics. Springer, New York, NY. https://doi.org/10.1007/978-1-4939-1366-4_12
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DOI: https://doi.org/10.1007/978-1-4939-1366-4_12
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