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CME Propagation Instructor Solution Activities Activity 1 : Solar Wind & The Shape Of IMF Question 1: What are the ranges of particle number densities in solar winds and in a CME bubble? Solar Wind CME Bubble : : Nr ≃ 15 − 20 cm−3 Nr ≃ 35 − 55 cm−3 Question 2: Why is the solar wind spiral in shape? What will be the shape of the solar wind jet if the sun were not spinning? While the solar wind particles themselves move radially outward from the sun, because of sun’s rotation the locus of all such particles emerging from the same spot on the sun forms a spiral pattern. This situation is analogous to a garden water sprinkler where sun is the sprinkler and the solar wind is the water jet. If the sun were not spinning the shape of solar wind would be straight line directed radially outward. Activity 2 : CME Propagation Speed Question 3: What is the CME propagation speed in km/s, as calculated from the snapshots? Show your calculation and take the average of the values. vcme r t 1AU = 1.4959 × 108 km ∆r (1 AU − 0.5 AU) 0.5 AU = = = = 1037 km/s ∆t (20 hrs) 20 hrs ∆r ( km) 0.5 AU Mar 05, 8:03 1.0 AU Mar 06, 4:04 7.479 × 107 1.5 AU Mar 07, 4:04 7.479 × 107 ∆t ( s) vcme km/s 7.206 × 104 8.64 × 104 1037 865 1 Question 4: Look at the color code in the velocity plot and answer the following questions (i) What is the maximum radial speed of CME plasma particles in km/s? vrmax ≃ 850 − 1000 km/s (ii) What is the typical speed of solar wind plasma particles in km/s? vr ≃ 400 − 500 km/s Question 5: As the CME propagates through space it leaves a cavity behind itself. This can be seen as the dark blue region behind it representing very low particle number density. Why is the region behind the CME empty? Hint: Examine your answers to the previous question. It is clear from the answers to the previous questions that the CME plasma travel 2-2.5 times faster than the solar wind plasma. So it sweeps the solar wind plasma infront of it leaving behind a cavity. Question 6: Assuming that the CME bubble does not accelerate as it propagates through the heliosphere, calculate the CME propagation time to the orbits of various planets. We are assuming circular orbits with radii equal to the mean distances between the sun and the planets. The CME propagation time is : Tcme = r/vcme ; vcme ≃ 950 km/s = 3.42 × 106 km/hr. Table 1: CME Propagation Time Planet Orbital Radius ( AU) Propagation Time Planet Orbital Radius ( AU) Propagation Time Mercury 0.387 AU 16.9 hrs Jupiter 5.203 AU 9 days − 11 hrs Venus 0.723 AU 1 day − 7 hrs Saturn 9.523 AU 17 days − 8 hrs Earth 1.00 AU 1 day − 20 hrs Uranus 19.209 34 days − 23 hrs Mars 1.524 AU 2 days − 18 hrs Neptune 30.087 54 days − 18 hrs 2 Activity 3 : CME & The IMF Question 7: Why is the IMF spiral in shape, in the absence of CME? Hint: In a highly conducting fluid like the solar plasma, the magnetic field lines are frozen in the fluid and are dragged along by the moving fluid. Since the IMF is dragged along by the solar wind it takes the same shape as the trails of the solar wind, a spiral shape. Question 8: How does the shape of IMF change as the CME bubble propagates through it? The fast moving CME plasma sweeps all the solar wind plasma between itself and the sun. So the magnetic field line behind a CME bubble is straight because of the absence of spiral structure due to solar wind. The field remains pinned to the CME plasma and gets stretched sideways as the CME spreads out. 3