Chapter 35: Problem 28
Find the value of \(g\), the gravitational acceleration at Earth's surface, in light-years per year per year, to three significant figures.
Chapter 35: Problem 28
Find the value of \(g\), the gravitational acceleration at Earth's surface, in light-years per year per year, to three significant figures.
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Get started for freeTwo identical nuclei are accelerated in a collider to a kinetic energy of \(621.38 \mathrm{GeV}\) and made to collide head on. If one of the two nuclei were instead kept at rest, the kinetic energy of the other nucleus would have to be 15,161.70 GeV for the collision to achieve the same center-of-mass energy. What is the rest mass of each of the nuclei?
In an elementary-particle experiment, a particle of mass \(m\) is fired, with momentum \(m c,\) at a target particle of mass \(2 \sqrt{2} m .\) The two particles form a single new particle (in a completely inelastic collision). Find the following: a) the speed of the projectile before the collision b) the mass of the new particle c) the speed of the new particle after the collision
Using relativistic expressions, compare the momentum of two electrons, one moving at \(2.00 \cdot 10^{8} \mathrm{~m} / \mathrm{s}\) and the other moving at \(2.00 \cdot 10^{3} \mathrm{~m} / \mathrm{s}\). What is the percent difference between nonrelativistic momentum values and these values?
A proton has a momentum of \(3.0 \mathrm{GeV} / c\). With what velocity is it moving relative to a stationary observer? a) \(0.31 c\) c) \(0.91 c\) e) \(3.2 c\) b) \(0.33 c\) d) \(0.95 c\)
\- 35.87 Although it deals with inertial reference frames, the special theory of relativity describes accelerating objects without difficulty. Of course, uniform acceleration no longer means \(d v / d t=g,\) where \(g\) is a constant, since that would have \(v\) exceeding \(c\) in a finite time. Rather, it means that the acceleration experienced by the moving body is constant: In each increment of the body's own proper time, \(d \tau,\) the body experiences a velocity increment \(d v=g d \tau\) as measured in the inertial frame in which the body is momentarily at rest. (As it accelerates, the body encounters a sequence of such frames, each moving with respect to the others.) Given this interpretation: a) Write a differential equation for the velocity \(v\) of the body, moving in one spatial dimension, as measured in the inertial frame in which the body was initially at rest (the "ground frame"). You can simplify your equation by remembering that squares and higher powers of differentials can be neglected. b) Solve the equation from part (a) for \(v(t),\) where both \(v\) and \(t\) are measured in the ground frame. c) Verify that \(v(t)\) behaves appropriately for small and large values of \(t\). d) Calculate the position of the body, \(x(t),\) as measured in the ground frame. For convenience, assume that the body is at rest at ground-frame time \(t=0\) and at ground-frame position \(x=c^{2} / g\). e) Identify the trajectory of the body on a space-time diagram (a Minkowski diagram, for Hermann Minkowski) with coordinates \(x\) and \(c t,\) as measured in the ground frame. f) For \(g=9.81 \mathrm{~m} / \mathrm{s}^{2},\) calculate how much time it takes the body to accelerate from rest to \(70.7 \%\) of \(c\), measured in the ground frame, and how much ground-frame distance the body covers in this time.
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