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Mechanics Berkeley Physics

Charles Kittel, Walter D. Knight, Malvin A. Ruderman, A. Carl Helmholz, Burton J. Moyer

Chapter 14

Principle of Equivalence - all with Video Answers

Educators


Chapter Questions

01:46

Problem 1

Pendulum in terms of gravitational and inertial masses. Show that the frequency of a pendulum of length $L$ is griven by
$$
v=\frac{\omega}{2 \pi}=\frac{1}{2 \pi}\left(\frac{M_{g} g}{M_{i}} \frac{g}{L}\right)^{!}
$$
where $M_{e}, M_{i}$ are the gravitational and inertial masses. (Bessel in the early days made careful pendulum observations and showed that $M_{g}$ was equal to $M_{i}$ within 1 part in $\left.6 \times 10^{4} .\right\}$

Hunza Gilgit
Hunza Gilgit
Numerade Educator
00:50

Problem 2

Cracitational red shift. Find an expression for the gravitational red shift in which you do not use the assumption that $\Delta_{V} / v \ll 1 .$ Neglect any effects associated with the curvature of space.) Start with $h \Delta v=-\left(h v / c^{2}\right)\left(M_{\mathrm{s}} G / r^{2}\right) \Delta r$, and inte grate over $d r$ from $R_{s}$ to infinity, and over $d v$ from $v$ to $v^{\prime}$.
$$
A n s, v^{\prime}=v e^{-G M_{w} / R x^{2}}
$$

Julian Wong
Julian Wong
Numerade Educator
02:48

Problem 3

Red shift from our galaxy. Estimate the gravitational red shift for light leaving the center of our galaxy, as observed far outside the galaxy. (Treat the distribution of mass as uniform within a sphere of radius 10,000 parsecs. The mass of the galaxy is $\sim 8 \times 10^{44} \mathrm{~g}$. Ans. $\Delta v / v=-3 \times 10^{-6}$

Harper Auman
Harper Auman
Numerade Educator
05:02

Problem 4

Radio galaxy. In 1962 an intense extraterrestrial source of radio radiation was optically identified as a starlike object with an angular radius of approximately $\frac{1^{\prime \prime}}{2}$ of are, It was at first thought to be a star in our galaxy giving off radio waves, but subsequently its spectrum was obtained and its spectral lines were found to be very considerably red-shifted. For instance, an atomic oxygen line with wavelength $\lambda$ normally $3.727 \times 10^{-5} \mathrm{~cm}$ was identified at $\lambda=5.097 \times 10^{-5} \mathrm{~cm} .$ One
explanation took it to be an exceedingly massive star with a spectrum gravitationally red-shifted. If this hypothetical radio star is in our galaxy, its distance must be less than $10^{22} \mathrm{~cm}$ from the earth. ${ }^{1}$
(a) Calculate from the angular diameter and the red shift, the mass and mean density of the star under this hypothesis, assuming the distance to be $10^{22} \mathrm{~cm}$. Is this a reasonable explanation of this object? Ans. Mass is $1.0 \times 10^{44} \mathrm{~g}$, mean density is $1.7 \times$ $10^{-6} \mathrm{~g} / \mathrm{cm}^{3} .$ This does not seem reasonable, as the mass is about $0.1$ of the total mass of our galaxy (use the result of Prob. 2).
(b) An alternative suggestion was that it might be a peculiar "radio galaxy," with its red shift following the usual recessional red-shift relation given in Chap. 10. Calculate its distance on this second hypothesis. Ans. $6 \times 10^{9}$ light yr $\left(5.6 \times 10^{27} \mathrm{~cm}\right)$
(c) Does the radio-galaxy hypothesis conform with this expectation? Ans. Yes; it has a radius of about $10^{22} \mathrm{~cm}$. This is in the usual range of galactic radii.

Kyle Godbey
Kyle Godbey
Numerade Educator
01:14

Problem 5

Black hole. What would the radius of the sun have to be in order for it to be a black hole [see (Eq. $14.10)]$ ? Compare the density it would then have to the density of a nucleus.

Narayan Hari
Narayan Hari
Numerade Educator