Newton had the data listed in Table 6–4, plus the relative sizes of these objects: in terms of the Sun’s radius R , the radii of Jupiter and Earth were 0.0997 R and 0.0109 R . Newton used this information to determine that the average density ρ (= mass/volume) of Jupiter is slightly less than of the Sun, while the average density of the Earth is four times that of the Sun. Thus, without leaving his home planet. Newton was able to predict that the composition of the Sun and Jupiter is markedly different than that of Earth. Reproduce Newton’s calculation and find his values for the ratios ρ J / ρ Sun and ρ E / ρ Sun (the modern values for these ratios are 0.93 and 3.91, respectively).
Newton had the data listed in Table 6–4, plus the relative sizes of these objects: in terms of the Sun’s radius R , the radii of Jupiter and Earth were 0.0997 R and 0.0109 R . Newton used this information to determine that the average density ρ (= mass/volume) of Jupiter is slightly less than of the Sun, while the average density of the Earth is four times that of the Sun. Thus, without leaving his home planet. Newton was able to predict that the composition of the Sun and Jupiter is markedly different than that of Earth. Reproduce Newton’s calculation and find his values for the ratios ρ J / ρ Sun and ρ E / ρ Sun (the modern values for these ratios are 0.93 and 3.91, respectively).
Newton had the data listed in Table 6–4, plus the relative sizes of these objects: in terms of the Sun’s radius R, the radii of Jupiter and Earth were 0.0997 R and 0.0109 R. Newton used this information to determine that the average density ρ(= mass/volume) of Jupiter is slightly less than of the Sun, while the average density of the Earth is four times that of the Sun. Thus, without leaving his home planet. Newton was able to predict that the composition of the Sun and Jupiter is markedly different than that of Earth. Reproduce Newton’s calculation and find his values for the ratios ρJ/ρSun and ρE/ρSun (the modern values for these ratios are 0.93 and 3.91, respectively).
Figure 8.14 shows a cube at rest and a small object heading toward it. (a) Describe the directions (angle 1) at which the small object can emerge after colliding elastically with the cube. How does 1 depend on b, the so-called impact parameter? Ignore any effects that might be due to rotation after the collision, and assume that the cube is much more massive than the small object. (b) Answer the same questions if the small object instead collides with a massive sphere.
2. A projectile is shot from a launcher at an angle 0,, with an initial velocity
magnitude vo, from a point even with a tabletop. The projectile hits an apple atop a
child's noggin (see Figure 1). The apple is a height y above the tabletop, and a
horizontal distance x from the launcher. Set this up as a formal problem, and solve
for x. That is, determine an expression for x in terms of only v₁, 0, y and g.
Actually, this is quite a long expression. So, if you want, you can determine an
expression for x in terms of v., 0., and time t, and determine another expression for
timet (in terms of v., 0.,y and g) that you will solve and then substitute the value of
t into the expression for x. Your final equation(s) will be called Equation 3 (and
Equation 4).
Draw a phase portrait for an oscillating, damped spring.
Biology: Life on Earth with Physiology (11th Edition)
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