DATA Supernova! (a) Equation (16.30) can be written as f R = f S ( 1 − υ c ) 1 / 2 ( 1 + υ c ) − 1 / 2 where c is the speed of light in vacuum, 3.00 × 10 8 m/s. Most objects move much slower than this ( υ / c is very small), so calculations made with Eq. (16.30) must be done carefully to avoid rounding errors. Use the binomial theorem to show that if υ ≪ c , Eq. (16.30) approximately reduces to f R = f S [1 − ( υ / c )] . (b) The gas cloud known as the Crab Nebula can be seen with even a small telescope. It is the remnant of a supernova, a cataclysmic explosion of a star. (The explosion was seen on the earth on July 4, 1054 C.E.) Its streamers glow with the characteristic red color of heated hydrogen gas. In a laboratory on the earth, heated hydrogen produces red light with frequency 4.568 × 10 14 Hz; the red light received from streamers in the Crab Nebula that are pointed toward the earth has frequency 4.586 × 10 14 Hz. Estimate the speed with which the outer edges of the Crab Nebula are expanding. Assume that the speed of the center of the nebula relative to the earth is negligible. (c) Assuming that the expansion speed of the Crab Nebula has been constant since the supernova that produced it, estimate the diameter of the Crab Nebula. Give your answer in meters and in light-years. (d) The angular diameter of the Crab Nebula as seen from the earth is about 5 arc-minutes ( 1 arc-minute = 1 60 degree ). Estimate the distance (in light-years) to the Crab Nebula, and estimate the year in which the supernova actually took place.
DATA Supernova! (a) Equation (16.30) can be written as f R = f S ( 1 − υ c ) 1 / 2 ( 1 + υ c ) − 1 / 2 where c is the speed of light in vacuum, 3.00 × 10 8 m/s. Most objects move much slower than this ( υ / c is very small), so calculations made with Eq. (16.30) must be done carefully to avoid rounding errors. Use the binomial theorem to show that if υ ≪ c , Eq. (16.30) approximately reduces to f R = f S [1 − ( υ / c )] . (b) The gas cloud known as the Crab Nebula can be seen with even a small telescope. It is the remnant of a supernova, a cataclysmic explosion of a star. (The explosion was seen on the earth on July 4, 1054 C.E.) Its streamers glow with the characteristic red color of heated hydrogen gas. In a laboratory on the earth, heated hydrogen produces red light with frequency 4.568 × 10 14 Hz; the red light received from streamers in the Crab Nebula that are pointed toward the earth has frequency 4.586 × 10 14 Hz. Estimate the speed with which the outer edges of the Crab Nebula are expanding. Assume that the speed of the center of the nebula relative to the earth is negligible. (c) Assuming that the expansion speed of the Crab Nebula has been constant since the supernova that produced it, estimate the diameter of the Crab Nebula. Give your answer in meters and in light-years. (d) The angular diameter of the Crab Nebula as seen from the earth is about 5 arc-minutes ( 1 arc-minute = 1 60 degree ). Estimate the distance (in light-years) to the Crab Nebula, and estimate the year in which the supernova actually took place.
DATA Supernova! (a) Equation (16.30) can be written as
f
R
=
f
S
(
1
−
υ
c
)
1
/
2
(
1
+
υ
c
)
−
1
/
2
where c is the speed of light in vacuum, 3.00 × 108 m/s. Most objects move much slower than this (υ/c is very small), so calculations made with Eq. (16.30) must be done carefully to avoid rounding errors. Use the binomial theorem to show that if υ ≪ c, Eq. (16.30) approximately reduces to fR= fS [1 − (υ/c)]. (b) The gas cloud known as the Crab Nebula can be seen with even a small telescope. It is the remnant of a supernova, a cataclysmic explosion of a star. (The explosion was seen on the earth on July 4, 1054 C.E.) Its streamers glow with the characteristic red color of heated hydrogen gas. In a laboratory on the earth, heated hydrogen produces red light with frequency 4.568 × 1014 Hz; the red light received from streamers in the Crab Nebula that are pointed toward the earth has frequency 4.586 × 1014 Hz. Estimate the speed with which the outer edges of the Crab Nebula are expanding. Assume that the speed of the center of the nebula relative to the earth is negligible. (c) Assuming that the expansion speed of the Crab Nebula has been constant since the supernova that produced it, estimate the diameter of the Crab Nebula. Give your answer in meters and in light-years. (d) The angular diameter of the Crab Nebula as seen from the earth is about 5 arc-minutes ( 1 arc-minute =
1
60
degree ). Estimate the distance (in light-years) to the Crab Nebula, and estimate the year in which the supernova actually took place.
A new satellite launched to the space. It is
orbiting the earth so that its displacement f
north of
the equator is given f =
A sin(wt + a). Sketch 2 cycles of f as a
function of t if A = 500 km, w = 3.6 rad/hour
and a = 0. Use proper scale to sketch graph.
Show detailed steps including how to find
the x-intercepts.
A particle has γ=18,399.
a) Calculate c-v in m/s. (I would have asked for 1 - v/c, making the answer dimensionless, but the system doesn't seem to take numbers that small. Gamma is chosen to make the particle extremely close to the speed of light.)
If your calculator gives problems, you might want to solve the appropriate equation for c-v or c(1 - v/c) and use an approximation.
b) In a race to the moon, by 3/4ths the distance, light is one or ten meters ahead of the particle. We routinely approximate mass as zero, gamma as infinite, and speed as the speed of light. ("Massless particles" -- gamma and m have to be eliminated from the expressions. Light is a true massless particle.)
If a massless particle has momentum 1,739 MeV/c, calculate its energy in MeV.
Thank you so much!!
A particle has γ=18,399.
a)Calculate c-v in m/s. (I would have asked for 1 - v/c, making the answer dimensionless, but the system doesn't seem to take numbers that small. Gamma is chosen to make the particle extremely close to the speed of light.)
If your calculator gives problems, you might want to solve the appropriate equation for c-v or c(1 - v/c) and use an approximation.
b) In the previous problem, in a race to the moon, by 3/4ths the distance, light is one or ten meters ahead of the particle. We routinely approximate mass as zero, gamma as infinite, and speed as the speed of light. ("Massless particles" -- gamma and m have to be eliminated from the expressions. Light is a true massless particle.) If a massless particle has momentum 1,739 MeV/c, calculate its energy in MeV.
Chapter 16 Solutions
University Physics with Modern Physics Plus Mastering Physics with eText -- Access Card Package (14th Edition)
Need a deep-dive on the concept behind this application? Look no further. Learn more about this topic, physics and related others by exploring similar questions and additional content below.