
Sign up to save your podcasts
Or


Naar aanleiding van een aantal vragen van luisteraar Bas, kijken we in deze ietwat lange aflevering naar hoe planeten rond sterren cirkelen.
The mass-period distribution of close-in exoplanets:
https://www.aanda.org/articles/aa/full_html/2011/04/aa15774-10/aa15774-10.html
Halting Planet Migration In The Evacuated Centers Of Protoplanetary Disks:
https://iopscience.iop.org/article/10.1086/342370/pdf
Orbital migration of the planetary companion of 51 Pegasi to its present location:
https://pages.astro.umd.edu/~dcr/reprints/lin_nature380,606.pdf
Connecting the dots II: Phase changes in the climate dynamics of tidally locked terrestrial exoplanets:
https://arxiv.org/pdf/1508.00419
The climate and habitability of planets with eternal day and night sides:
https://serious-science.org/the-climate-and-habitability-of-planets-with-eternal-day-and-night-sides-5289
import numpy as np
import matplotlib.pyplot as plt
import matplotlib.ticker as ticker
a = 1.0 # semi-major axis (AU)
M2 = 1.0 # mass of the central body
# M1: mass of the orbiting body, from 0 to 1
M1 = np.linspace(0, 1, 500)
# Newton's law
T = np.sqrt(a**3 / (M1 + M2))
fig, ax = plt.subplots(figsize=(9, 5.5))
fig.patch.set_facecolor("#0d1117")
ax.set_facecolor("#0d1117")
# Gradient-ish line via a LineCollection
from matplotlib.collections import LineCollection
points = np.array([M1, T]).T.reshape(-1, 1, 2)
segments = np.concatenate([points[:-1], points[1:]], axis=1)
norm = plt.Normalize(T.min(), T.max())
lc = LineCollection(segments, cmap="cool", norm=norm, linewidth=2.5, zorder=3)
lc.set_array(T)
ax.add_collection(lc)
ax.scatter([0], [np.sqrt(a**3 / M2)], color="#ff6b9d", s=70, zorder=5,
label=f"Test-particle limit (M₁→0, T={np.sqrt(a**3/M2):.3f} yr)")
T_eq = np.sqrt(a**3 / (M2 + M2))
ax.scatter([M2], [T_eq], color="#ffd166", s=70, zorder=5,
label=f"Equal masses (M₁=M₂={M2}, T={T_eq:.3f} yr)")
for spine in ax.spines.values():
spine.set_edgecolor("#30363d")
ax.tick_params(colors="#8b949e", labelsize=10)
ax.xaxis.label.set_color("#c9d1d9")
ax.yaxis.label.set_color("#c9d1d9")
ax.set_xlabel("M₁ — Mass of orbiting body (M☉)", fontsize=12, labelpad=10)
ax.set_ylabel("Orbital Period T (years)", fontsize=12, labelpad=10)
ax.set_title("Orbital Period vs. Mass of Orbiting Body\n"
r"$T = \sqrt{\,a^3\,/\,(M_1+M_2)\,}$"
f" [a = {a} AU, M₂ = {M2} M☉]",
color="#e6edf3", fontsize=13, pad=14)
ax.set_xlim(-0.01, 1.01)
ax.set_ylim(T.min() * 0.97, T.max() * 1.03)
ax.grid(color="#21262d", linestyle="--", linewidth=0.7, zorder=0)
ax.legend(facecolor="#161b22", edgecolor="#30363d",
labelcolor="#c9d1d9", fontsize=10, loc="upper right")
plt.tight_layout()
plt.show()
De Zimmerman en Space podcast is gelicenseerd onder een Creative Commons CC0 1.0 licentie.
http://creativecommons.org/publicdomain/zero/1.0
By Hens Zimmerman5
33 ratings
Naar aanleiding van een aantal vragen van luisteraar Bas, kijken we in deze ietwat lange aflevering naar hoe planeten rond sterren cirkelen.
The mass-period distribution of close-in exoplanets:
https://www.aanda.org/articles/aa/full_html/2011/04/aa15774-10/aa15774-10.html
Halting Planet Migration In The Evacuated Centers Of Protoplanetary Disks:
https://iopscience.iop.org/article/10.1086/342370/pdf
Orbital migration of the planetary companion of 51 Pegasi to its present location:
https://pages.astro.umd.edu/~dcr/reprints/lin_nature380,606.pdf
Connecting the dots II: Phase changes in the climate dynamics of tidally locked terrestrial exoplanets:
https://arxiv.org/pdf/1508.00419
The climate and habitability of planets with eternal day and night sides:
https://serious-science.org/the-climate-and-habitability-of-planets-with-eternal-day-and-night-sides-5289
import numpy as np
import matplotlib.pyplot as plt
import matplotlib.ticker as ticker
a = 1.0 # semi-major axis (AU)
M2 = 1.0 # mass of the central body
# M1: mass of the orbiting body, from 0 to 1
M1 = np.linspace(0, 1, 500)
# Newton's law
T = np.sqrt(a**3 / (M1 + M2))
fig, ax = plt.subplots(figsize=(9, 5.5))
fig.patch.set_facecolor("#0d1117")
ax.set_facecolor("#0d1117")
# Gradient-ish line via a LineCollection
from matplotlib.collections import LineCollection
points = np.array([M1, T]).T.reshape(-1, 1, 2)
segments = np.concatenate([points[:-1], points[1:]], axis=1)
norm = plt.Normalize(T.min(), T.max())
lc = LineCollection(segments, cmap="cool", norm=norm, linewidth=2.5, zorder=3)
lc.set_array(T)
ax.add_collection(lc)
ax.scatter([0], [np.sqrt(a**3 / M2)], color="#ff6b9d", s=70, zorder=5,
label=f"Test-particle limit (M₁→0, T={np.sqrt(a**3/M2):.3f} yr)")
T_eq = np.sqrt(a**3 / (M2 + M2))
ax.scatter([M2], [T_eq], color="#ffd166", s=70, zorder=5,
label=f"Equal masses (M₁=M₂={M2}, T={T_eq:.3f} yr)")
for spine in ax.spines.values():
spine.set_edgecolor("#30363d")
ax.tick_params(colors="#8b949e", labelsize=10)
ax.xaxis.label.set_color("#c9d1d9")
ax.yaxis.label.set_color("#c9d1d9")
ax.set_xlabel("M₁ — Mass of orbiting body (M☉)", fontsize=12, labelpad=10)
ax.set_ylabel("Orbital Period T (years)", fontsize=12, labelpad=10)
ax.set_title("Orbital Period vs. Mass of Orbiting Body\n"
r"$T = \sqrt{\,a^3\,/\,(M_1+M_2)\,}$"
f" [a = {a} AU, M₂ = {M2} M☉]",
color="#e6edf3", fontsize=13, pad=14)
ax.set_xlim(-0.01, 1.01)
ax.set_ylim(T.min() * 0.97, T.max() * 1.03)
ax.grid(color="#21262d", linestyle="--", linewidth=0.7, zorder=0)
ax.legend(facecolor="#161b22", edgecolor="#30363d",
labelcolor="#c9d1d9", fontsize=10, loc="upper right")
plt.tight_layout()
plt.show()
De Zimmerman en Space podcast is gelicenseerd onder een Creative Commons CC0 1.0 licentie.
http://creativecommons.org/publicdomain/zero/1.0

213 Listeners

5 Listeners

9 Listeners

60 Listeners

41 Listeners

23 Listeners

137 Listeners

84 Listeners

15 Listeners

270 Listeners

92 Listeners

37 Listeners

31 Listeners

0 Listeners

0 Listeners

0 Listeners