Lecture 10: In-Situ Heliophysics: Parker Solar Probe

ASTR 370 Solar Physics and Space Weather

Context and Why This Matters

Lecture 08 derived the Parker wind solution theoretically and Lecture 09 surveyed the remote-sensing techniques that measure the Sun from a distance; this lecture completes the observational picture with in-situ measurement, made real and current by the Parker Solar Probe mission, named for the same physicist whose 1958 theory this course derived in Lecture 08.

Learning Goals

  1. Distinguish in-situ measurement from the remote-sensing techniques of Lecture 09.
  2. Summarize Parker Solar Probe’s real mission design, perihelion distance, and record-setting heliocentric speed.
  3. Connect Parker Solar Probe’s in-situ measurements directly to Lecture 08’s Parker wind theory as an observational test.

Opening Phenomenon

Parker Solar Probe, launched 2018-08-12, uses repeated gravity assists from Venus to reach a perihelion of just 9.86 solar radii (6.9e+06 km from the Sun’s center) -- deep inside the corona, well within Lecture 08’s computed critical radius (4.62 R_sun) -- reaching a record heliocentric speed of 191 km/s (690,000 km/h) at its closest approach, making it the fastest human-made object ever built.

Terms Developed in Context

in-situ measurement

Direct sampling of local plasma, fields, particles, or dust by an instrument located within the environment being studied. In this lecture, the term is needed to interpret the following evidence or model claim: In-situ measurement directly samples the plasma, fields, and particles at the spacecraft’s own location, in contrast to remote sensing’s reliance on radiation received from a distance; the two techniques are complementary, not competing, and heliophysics missions are frequently coordinated (e.g., Parker Solar Probe and Solar Orbiter observing simultaneously from different vantage points, as both missions have done).

Its relationship to perihelion is part of the lecture's reasoning chain rather than a synonym: Because Parker Solar Probe’s perihelion ({PSP_PERIHELION_RSUN:.2f} R_sun) is close to, though still somewhat outside, Lecture 08’s computed critical radius ({PARKER_RC_RSUN:.2f} R_sun), its in-situ measurements provide a direct observational test of the Parker wind theory’s predictions in the very region where the wind is theoretically expected to become supersonic. The working relation \( \text{In-situ: measure plasma/field properties directly at the spacecraft.}\quad \text{Remote sensing: infer properties from received radiation (Lecture 09).} \) makes the relevant observable or model dependence explicit.

Limitation and usage: Confusing Parker Solar Probe’s own orbital (heliocentric) speed with the solar wind’s outflow speed that it measures. The spacecraft’s record-breaking 191 km/s speed at perihelion is a consequence of its own orbital mechanics (falling deep into the Sun’s gravitational well), not a measurement of how fast the solar wind itself is flowing at that location -- these are two entirely distinct velocities that a careless reading of headlines can easily conflate. This caution sets the boundary on what can be inferred when using in-situ measurement in an explanation.

perihelion

The point in a spacecraft or planet's orbit at which its distance from the Sun is smallest. In this lecture, the term is needed to interpret the following evidence or model claim: Parker Solar Probe, launched 2018-08-12, uses repeated gravity assists from Venus to reach a perihelion of just 9.86 solar radii (6.9e+06 km from the Sun’s center) -- deep inside the corona, well within Lecture 08’s computed critical radius (4.62 R_sun) -- reaching a record heliocentric speed of 191 km/s (690,000 km/h) at its closest approach, making it the fastest human-made object ever built.

Its relationship to gravity assist is part of the lecture's reasoning chain rather than a synonym: Parker Solar Probe’s extreme heliocentric speed near perihelion is a direct consequence of orbital mechanics (Kepler’s second law: a highly eccentric orbit moves fastest at its point of closest approach), engineered deliberately by the mission’s repeated Venus gravity assists to progressively lower its perihelion over its multi-year mission. The working relation \( \text{In-situ: measure plasma/field properties directly at the spacecraft.}\quad \text{Remote sensing: infer properties from received radiation (Lecture 09).} \) makes the relevant observable or model dependence explicit.

Limitation and usage: Confusing Parker Solar Probe’s own orbital (heliocentric) speed with the solar wind’s outflow speed that it measures. The spacecraft’s record-breaking 191 km/s speed at perihelion is a consequence of its own orbital mechanics (falling deep into the Sun’s gravitational well), not a measurement of how fast the solar wind itself is flowing at that location -- these are two entirely distinct velocities that a careless reading of headlines can easily conflate. This caution sets the boundary on what can be inferred when using perihelion in an explanation.

gravity assist

An exchange of energy and angular momentum with a moving planet that changes a spacecraft's heliocentric orbit without equivalent propellant use. In this lecture, the term is needed to interpret the following evidence or model claim: Parker Solar Probe, launched 2018-08-12, uses repeated gravity assists from Venus to reach a perihelion of just 9.86 solar radii (6.9e+06 km from the Sun’s center) -- deep inside the corona, well within Lecture 08’s computed critical radius (4.62 R_sun) -- reaching a record heliocentric speed of 191 km/s (690,000 km/h) at its closest approach, making it the fastest human-made object ever built.

Its relationship to Alfven surface is part of the lecture's reasoning chain rather than a synonym: Parker Solar Probe’s extreme heliocentric speed near perihelion is a direct consequence of orbital mechanics (Kepler’s second law: a highly eccentric orbit moves fastest at its point of closest approach), engineered deliberately by the mission’s repeated Venus gravity assists to progressively lower its perihelion over its multi-year mission. The working relation \( \text{In-situ: measure plasma/field properties directly at the spacecraft.}\quad \text{Remote sensing: infer properties from received radiation (Lecture 09).} \) makes the relevant observable or model dependence explicit.

Limitation and usage: Confusing Parker Solar Probe’s own orbital (heliocentric) speed with the solar wind’s outflow speed that it measures. The spacecraft’s record-breaking 191 km/s speed at perihelion is a consequence of its own orbital mechanics (falling deep into the Sun’s gravitational well), not a measurement of how fast the solar wind itself is flowing at that location -- these are two entirely distinct velocities that a careless reading of headlines can easily conflate. This caution sets the boundary on what can be inferred when using gravity assist in an explanation.

Alfven surface

The boundary where outward solar-wind speed first exceeds the inward communication speed of Alfven waves along the magnetic field. In this lecture, the term is needed to interpret the following evidence or model claim: In 2021, Parker Solar Probe crossed the Alfven surface (the boundary within which the solar wind’s outward speed is slower than the local Alfven wave speed, so that magnetic disturbances can in principle propagate back toward the Sun) for the first time, entering the solar atmosphere in a meaningful physical sense -- described by NASA as the mission "touching the Sun."

Its relationship to magnetic switchback is part of the lecture's reasoning chain rather than a synonym: Parker Solar Probe, launched 2018-08-12, uses repeated gravity assists from Venus to reach a perihelion of just 9.86 solar radii (6.9e+06 km from the Sun’s center) -- deep inside the corona, well within Lecture 08’s computed critical radius (4.62 R_sun) -- reaching a record heliocentric speed of 191 km/s (690,000 km/h) at its closest approach, making it the fastest human-made object ever built. The working relation \( \text{In-situ: measure plasma/field properties directly at the spacecraft.}\quad \text{Remote sensing: infer properties from received radiation (Lecture 09).} \) makes the relevant observable or model dependence explicit.

Limitation and usage: Confusing Parker Solar Probe’s own orbital (heliocentric) speed with the solar wind’s outflow speed that it measures. The spacecraft’s record-breaking 191 km/s speed at perihelion is a consequence of its own orbital mechanics (falling deep into the Sun’s gravitational well), not a measurement of how fast the solar wind itself is flowing at that location -- these are two entirely distinct velocities that a careless reading of headlines can easily conflate. This caution sets the boundary on what can be inferred when using Alfven surface in an explanation.

magnetic switchback

A localized, often sharp reversal or fold in the heliospheric magnetic-field direction observed in the young solar wind. In this lecture, the term is needed to interpret the following evidence or model claim: Parker Solar Probe has directly detected numerous "magnetic switchbacks" (sudden, localized reversals in the solar wind’s magnetic field direction) in the near-Sun solar wind, a real, still-being-investigated phenomenon relevant to the coronal-heating and wind-acceleration problems introduced in Lecture 02 and Lecture 08.

Its relationship to Faraday cup is part of the lecture's reasoning chain rather than a synonym: Parker Solar Probe carries direct-sampling ("in-situ") instruments -- a Faraday cup and electrostatic analyzers (SWEAP) to directly measure solar wind ion/electron velocity, density, and temperature; magnetometers (FIELDS) to directly measure the local magnetic field; and energetic-particle detectors (IS(sun)IS) -- rather than remotely imaging the Sun from a distance as SDO and SOHO do (Lecture 09). The working relation \( \text{In-situ: measure plasma/field properties directly at the spacecraft.}\quad \text{Remote sensing: infer properties from received radiation (Lecture 09).} \) makes the relevant observable or model dependence explicit.

Limitation and usage: Confusing Parker Solar Probe’s own orbital (heliocentric) speed with the solar wind’s outflow speed that it measures. The spacecraft’s record-breaking 191 km/s speed at perihelion is a consequence of its own orbital mechanics (falling deep into the Sun’s gravitational well), not a measurement of how fast the solar wind itself is flowing at that location -- these are two entirely distinct velocities that a careless reading of headlines can easily conflate. This caution sets the boundary on what can be inferred when using magnetic switchback in an explanation.

Faraday cup

A particle detector that collects charged particles and uses the resulting current-versus-voltage response to infer plasma density, speed, and temperature. In this lecture, the term is needed to interpret the following evidence or model claim: Parker Solar Probe carries direct-sampling ("in-situ") instruments -- a Faraday cup and electrostatic analyzers (SWEAP) to directly measure solar wind ion/electron velocity, density, and temperature; magnetometers (FIELDS) to directly measure the local magnetic field; and energetic-particle detectors (IS(sun)IS) -- rather than remotely imaging the Sun from a distance as SDO and SOHO do (Lecture 09).

Its relationship to in-situ measurement is part of the lecture's reasoning chain rather than a synonym: Parker Solar Probe, launched 2018-08-12, uses repeated gravity assists from Venus to reach a perihelion of just 9.86 solar radii (6.9e+06 km from the Sun’s center) -- deep inside the corona, well within Lecture 08’s computed critical radius (4.62 R_sun) -- reaching a record heliocentric speed of 191 km/s (690,000 km/h) at its closest approach, making it the fastest human-made object ever built. The working relation \( \text{In-situ: measure plasma/field properties directly at the spacecraft.}\quad \text{Remote sensing: infer properties from received radiation (Lecture 09).} \) makes the relevant observable or model dependence explicit.

Limitation and usage: Confusing Parker Solar Probe’s own orbital (heliocentric) speed with the solar wind’s outflow speed that it measures. The spacecraft’s record-breaking 191 km/s speed at perihelion is a consequence of its own orbital mechanics (falling deep into the Sun’s gravitational well), not a measurement of how fast the solar wind itself is flowing at that location -- these are two entirely distinct velocities that a careless reading of headlines can easily conflate. This caution sets the boundary on what can be inferred when using Faraday cup in an explanation.

Evidence

Derivation and Model

Working Equation

\[ \text{In-situ: measure plasma/field properties directly at the spacecraft.}\quad \text{Remote sensing: infer properties from received radiation (Lecture 09).} \]

Worked Example

  1. Parker Solar Probe’s record heliocentric speed of 191 km/s, achieved during its closest perihelion passage, is more than 1 times Lecture 08’s computed coronal isothermal sound speed (144 km/s) -- though this comparison is only illustrative, since the spacecraft’s orbital speed (driven by gravity and repeated Venus flybys) is a completely different physical quantity from the solar wind’s own outflow speed that it measures in situ, and the two should not be conflated.
  2. Parker Solar Probe’s perihelion distance (9.86 R_sun) is only about 2.1 times Lecture 08’s computed Parker-wind critical radius (4.62 R_sun) -- meaning the spacecraft samples plasma in a region where the simplified isothermal Parker wind model predicts the flow should already be at or somewhat above the sound speed, directly testable against the mission’s real in-situ SWEAP velocity measurements.

Common Misconception

Confusing Parker Solar Probe’s own orbital (heliocentric) speed with the solar wind’s outflow speed that it measures. The spacecraft’s record-breaking 191 km/s speed at perihelion is a consequence of its own orbital mechanics (falling deep into the Sun’s gravitational well), not a measurement of how fast the solar wind itself is flowing at that location -- these are two entirely distinct velocities that a careless reading of headlines can easily conflate.

Active-Learning Guidance

Using Kepler’s second law (equal areas in equal times), explain qualitatively why Parker Solar Probe’s speed is far higher at its {PSP_PERIHELION_RSUN:.2f} R_sun perihelion than at its much more distant aphelion, independent of any solar-wind physics.

Lab Connection

Lab 05’s second half uses Parker Solar Probe’s real perihelion distance and Lecture 08’s numerically solved wind-speed curve to predict the in-situ solar wind speed the spacecraft should sample near its closest approach.

Synthesis Questions

References