Magnetometer and radar study of the ionospheric convection response to sudden changes in the interplanetary magnetic field R. A. D. Fiori 1,2, D. Boteler.

Slides:



Advertisements
Similar presentations
Abstract Using observations at 1-Hz sampling rate from the Greenland west coast magnetometer chain we study ULF waves over a wide frequency band and a.
Advertisements

J. Goldstein (1), R. A. Wolf(1), B. R. Sandel(2), T. Forrester (2), D. L. Gallagher (3), P. H. Reiff (1), (1) Department of Physics & Astronomy, Rice University,
Anti-Parallel Merging and Component Reconnection: Role in Magnetospheric Dynamics M.M Kuznetsova, M. Hesse, L. Rastaetter NASA/GSFC T. I. Gombosi University.
Fate of sub-keV ring current ions observed by Viking Viking 20 years Yamauchi and Lundin * Superposed epoch analyses * Viking Ion data + AE (and Dst) 
E. Amata M. Candidi (1), M.F. Marcucci (1), S. Massetti (1), P. Francia (3), U. Villante (3) (1) Istituto di Fisica dello Spazio Interplanetario (IFSI),
The role of solar wind energy flux for transpolar arc luminosity A.Kullen 1, J. A. Cumnock 2,3, and T. Karlsson 2 1 Swedish Institute of Space Physics,
VT SuperDARN Group2011 SuperDARN WorkshopJoseph Baker Testing the Equipotential Magnetic Field Line Assumption Using Interhemispheric.
Spatial distribution of the auroral precipitation zones during storms connected with magnetic clouds O.I. Yagodkina 1, I.V. Despirak 1, V. Guineva 2 1.
Magnetopause flow vortices revealed during high speed solar wind streams Mona Kessel (NASA GSFC), Yaireska Collado-Vega (University of Puerto Rico), Xi.
PHYSICS AND ENGINEERING PHYSICS Mohsen Ghezelbash, H. Liu, A.V. Koustov and D. André F-region echo occurrence in the polar cap: A comparison of PolarDARN.
SuperDARN interhemispheric observations of reconnection signatures: a case study. Coco, I. (1), S. Massetti (1), E. Amata (1), M. F. Marcucci (1), and.
Anti-parallel versus Component Reconnection at the Magnetopause K.J. Trattner Lockheed Martin Advanced Technology Center Palo Alto, CA, USA and the Polar/TIMAS,
Identification and Analysis of Magnetic Substorms Patricia Gavin 1, Sandra Brogl 1, Ramon Lopez 2, Hamid Rassoul 1 1. Florida Institute of Technology,
Peter Boakes 1, Steve Milan 2, Adrian Grocott 2, Mervyn Freeman 3, Gareth Chisham 3, Gary Abel 3, Benoit Hubert 4, Victor Sergeev 5 Rumi Nakamura 1, Wolfgang.
SuperDARN Workshop May 30 – June Magnetopause reconnection rate and cold plasma density: a study using SuperDARN Mark Lester 1, Adrian Grocott 1,2,
On the relationship between polar cap flows and the IMF W.A. Bristow, R.T. Parris, J. Spaleta, T. Theurer Geophysical Institute, University of Alaska.
31 May 2011SuperDARN Workshop, 29 May - 3June 2011, Hanover, US 1 Short-period Doppler shift variations in the polar cap: ULF waves or something else?
Tracing Geomagnetic Conjugate Points by means of Extremely Similar Interhemispheric Auroras N. Sato (1), A. Kadokura (1), Y. Ebihara (1), H. Deguchi (1),
What DMSP Data Tell us About the Thermosphere Response to Solar Wind Forcing Delores Knipp CU Aerospace Engineering Sciences and NCAR HAO With Assistance.
On the importance of IMF |B Y | on polar cap patch formation Qinghe Zhang 1, Beichen Zhang 1, Ruiyuan Liu 1, M. W. Dunlop 2, M. Lockwood 2, 3, J. Moen.
Radio and Space Plasma Physics Group The formation of transpolar arcs R. C. Fear and S. E. Milan University of Leicester.
Solar wind-magnetosphere- atmosphere coupling: effects of magnetic storms and substorms in atmospheric electric field variations Kleimenova N., Kozyreva.
Magnetospheric ULF wave activity monitoring based on the ULF-index OLGA KOZYREVA and N. Kleimenova Institute of the Earth Physics, RAS.
5 th European Space Weather Week, November 2008, Brussels Operational implementation of the SWIF model in DIAS system Tsagouri Ioanna Koutroumbas.
EISCAT Svalbard Radar studies of meso-scale plasma flow channels in the polar cusp ionosphere Y. Dåbakk et al.
EISCAT-Cluster observations of quiet-time near-Earth magnetotail fast flows and their signatures in the ionosphere Nordic Cluster Meeting, Uppsala, Sweden,
Ground level enhancement of the solar cosmic rays on January 20, A.V. Belov (a), E.A. Eroshenko (a), H. Mavromichalaki (b), C. Plainaki(b), V.G.
PAPER I. ENA DATA ANALYSIS RESULTS. The Imager for Magnetopause-to- Aurora Global Exploration (IMAGE) missionis the first NASA Mid-size Explorer (MIDEX)
A T Y Lui, V Angelopoulos, S B Mende, O LeContel, H Frey, E Donovan, D G Sibeck, W Liu, H U Auster, X Li, M Nose, and M O Fillingim Outline  Conjunction.
Large electric fields near the nightside plasmapause observed by the Polar spacecraft K.-H. Kim 1, F. Mozer 2, and D.-H. Lee 1 1 Department of Astronomy.
Magnetic Flux Transport and Pressure Variations at Magnetotail Plasma Flow Bursts during Geomagnetically Quiet Times Motoharu Nowada ( 野和田 基晴 :
Oxygen Injection Events observed by Freja Satellite M. Yamauchi 1, L. Eliasson 1, H. Nilsson 1, R. Lundin 1, and O. Norberg 2 1.Swedish Institute of Space.
Response of the Magnetosphere and Ionosphere to Solar Wind Dynamic Pressure Pulse KYUNG SUN PARK 1, TATSUKI OGINO 2, and DAE-YOUNG LEE 3 1 School of Space.
Coupling of the Magnetosphere and Ionosphere by Alfvén Waves at High and Mid-Latitudes Bob Lysak, Yan Song, University of Minnesota, MN, USA Murray Sciffer,
Mapping high-latitude TEC fluctuations using GNSS I.I. SHAGIMURATOV (1), A. KRANKOWSKI (2), R. SIERADZKI (2), I.E. ZAKHARENKOVA (1,2), Yu.V. CHERNIAK (1),
University of Saskatchewan PHYSICS AND ENGINEERING PHYSICS Spectral widths of F-region PolarDARN echoes, a statistical assessment A.V. Koustov, S. Toderian.
Testing the Equipotential Magnetic Field Line Assumption Using SuperDARN Measurements and the Cluster Electron Drift Instrument (EDI) Joseph B. H. Baker.
GEOSYNCHRONOUS SIGNATURES OF AURORAL SUBSTORMS PRECEDED BY PSEUDOBREAKUPS A. Kullen (1), S. Ohtani (2), and H. Singer (3) A. Kullen (1), S. Ohtani (2),
ESS 7 Lecture 13 October 29, 2008 Substorms. Time Series of Images of the Auroral Substorm This set of images in the ultra-violet from the Polar satellite.
Ionospheric Convection during an extended period of Northward IMF
Yvonne Rinne, Departement of Physics, University of Oslo Mesoscale transient flow channels observed in the cusp ionosphere by the EISCAT Svalbard Radar.
Simultaneous in-situ observations of the feature of a typical FTE by Cluster and TC1 Zhang Qinghe Liu Ruiyuan Polar Research Institute of China
Cluster and SuperDARN observations during a positive B y period D. Ambrosino, E. Amata, M.F. Marcucci, I. Coco Istituto di Fisica dello Spazio Interplanetario,
Guan Le NASA Goddard Space Flight Center Challenges in Measuring External Current Systems Driven by Solar Wind-Magnetosphere Interaction.
Dawn-dusk asymmetry in the intensity of the polar cap flows as seen by the SuperDARN radars A.V. Koustov, R.A.D. Fiori, Z. Abooalizadeh PHYSICS AND ENGINEERING.
Substorm-origin sub-keV ring current ions: wedge-like structure ICS-9, Graz, ~7 Substorm : production of plasma Sub-keV ring current : fossil of.
Towards an information theory approach for monitoring the ionospheric convection dynamics Towards an information theory approach for monitoring the ionospheric.
MULTI-INSTRUMENT STUDY OF THE ENERGY STEP STRUCTURES OF O + AND H + IONS IN THE CUSP AND POLAR CAP REGIONS Yulia V. Bogdanova, Berndt Klecker and CIS TEAM.
Effects of January 2010 stratospheric sudden warming in the low-latitude ionosphere L. Goncharenko, A. Coster, W. Rideout, MIT Haystack Observatory, USA.
Combined Sounding Rocket and SuperDarn/EISCAT Radar Observations of Plasma Convection, Shear, Irregularities and other Phenomena in the Cusp and Boundary.
R. Maggiolo 1, M. Echim 1,2, D. Fontaine 3, A. Teste 4, C. Jacquey 5 1 Belgian Institute for Space Aeronomy (IASB-BIRA); 2 Institute.
Statistical Characterization of sub-auroral polarization stream using using large scale observations by mid- latitude SuperDARN radars B. S. R. Kunduri.
Postmidnight ionospheric trough in summer and link to solar wind: how, when and why? Mirela Voiculescu (1), T. Nygrén (2), A. Aikio(2), H. Vanhamäki (2)
VT SuperDARN Group Joseph Baker Ground-Based Observations of the Plasmapause Boundary Layer (PBL) Region with.
Auroral Arcs in the Late Growth Phase
Department of Electrical and Computer Engineering, Virginia Tech
Night-side effects on the plasma convection in the polar ionosphere due to a Sudden Impulse (SI) of solar wind dynamic pressure Coco, I.(1,2,3); Amata,
Disturbance Dynamo Effects in the Low Latitude Ionosphere
Evidence for Dayside Interhemispheric Field-Aligned Currents During Strong IMF By Conditions Seen by SuperDARN Radars Joseph B.H. Baker, Bharat Kunduri.
CEDAR 2013 Workshop International space weather and climate observations along the 120E/60W meridional circle and its surrounding areas Space weather observations.
The Physics of Space Plasmas
Yuki Takagi1*, Kazuo Shiokawa1, Yuichi Otsuka1, and Martin Connors2  
Subauroral heliosphere-geosphere coupling during November 2004 ionospheric storms: F2-region, North-East Asia Chelpanov M. A., Zolotukhina N.A. Institute.
P. Stauning: The Polar Cap (PC) Index for Space Weather Forecasts
Dynamic Coupling between the Magnetosphere and the Ionosphere
SuperDARN and SCANDI data
Determination of the Substorm Initiation Region From a Major Conjunction Interval of THEMIS Satellites A T Y Lui, V Angelopoulos, S B Mende, O LeContel,
Determination of the Substorm Initiation Region From a Major Conjunction Interval of THEMIS Satellites A T Y Lui, V Angelopoulos, S B Mende, O LeContel,
Determination of the Substorm Initiation Region From a Major Conjunction Interval of THEMIS Satellites A T Y Lui, V Angelopoulos, S B Mende, O LeContel,
M. Yamauchi1, T. Sergienko1, C. -F. Enell2, A. Schillings1, R
Presentation transcript:

Magnetometer and radar study of the ionospheric convection response to sudden changes in the interplanetary magnetic field R. A. D. Fiori 1,2, D. Boteler 1, A. V. Koustov 2 1 Natural Resources Canada, Geomagnetic Observatory, Ottawa, ON, Canada 2 University of Saskatchewan, Institute for Space and Atmospheric Studies, Saskatoon, SK, Canada

Effect to be Investigated Following a southward turning of the IMF the convection pattern must transition from a B z <0 multi-celled to a B z <0 two-celled convection pattern Following a southward turning of the IMF the convection pattern must transition from a B z <0 multi-celled to a B z <0 two-celled convection pattern ? Bz > 0Bz < 0

Two reconfiguration scenarios Scenario 1: Ionospheric convection response begins at the dayside cusp region and propagates toward the nightside. Scenario 1: Ionospheric convection response begins at the dayside cusp region and propagates toward the nightside. Scenario 2: The entire high-latitude ionosphere responds simultaneously in all MLT sectors. Scenario 2: The entire high-latitude ionosphere responds simultaneously in all MLT sectors.

Objective In this work, simultaneous observations and mapping of measurements from both the SuperDARN and ground-based magnetometer instruments are examined to attempt a more comprehensive picture of the phenomenon. In this work, simultaneous observations and mapping of measurements from both the SuperDARN and ground-based magnetometer instruments are examined to attempt a more comprehensive picture of the phenomenon. Resolve peculiarities! Resolve peculiarities!

Event Study Criteria Criteria ACE data available ACE data available Sudden (<5 min) transition from at least +5nT to -5nT preceded by at least 1 hour of relatively stable IMF B z Sudden (<5 min) transition from at least +5nT to -5nT preceded by at least 1 hour of relatively stable IMF B z SuperDARN data available on a large scale (>500 points) SuperDARN data available on a large scale (>500 points) SuperMAG data available (2000 or 2001) SuperMAG data available (2000 or 2001) Transition in the early to mid afternoon to ensure good radar location Transition in the early to mid afternoon to ensure good radar location Events selected Events selected January 20, 2001 January 20, 2001 November 02, 2001 November 02, 2001

IMF A sharp southward transition in the IMF B z at 10:25 UT is expected to arrive at the ionosphere at 11:58 UT A sharp southward transition in the IMF B z at 10:25 UT is expected to arrive at the ionosphere at 11:58 UT

Magnetometer-observed response Magnetometer response time was identified as the start of any noticeable change to the perturbation magnetic field Magnetometer response time was identified as the start of any noticeable change to the perturbation magnetic field In general, responses were delayed on the nightside compared to the dayside In general, responses were delayed on the nightside compared to the dayside 10.3 MLT (dayside) 1.5 MLT (nightside) delay=0 delay=12

Magnetometer-observed response The perturbation in the H component of the magnetic field was generated for all stations available from the SuperMAG data repository The perturbation in the H component of the magnetic field was generated for all stations available from the SuperMAG data repository Station locations are mapped in MLAT/MLT coordinates at 12:00 UT Station locations are mapped in MLAT/MLT coordinates at 12:00 UT 14 MLT 10 MLT 05 MLT 03 MLT

Magnetometer-observed response The perturbation magnetic field enhanced to more positive or more negative values in response to a sharp transition in the IMF Bz The perturbation magnetic field enhanced to more positive or more negative values in response to a sharp transition in the IMF Bz The shortest delays of 0-1 minutes were observed in the 10 MLT sectors, and the longest delays of 9-12 minutes were observed in the 14 MLT sector The shortest delays of 0-1 minutes were observed in the 10 MLT sectors, and the longest delays of 9-12 minutes were observed in the 14 MLT sector delay=6-8 mindelay=0-8 min delay=0-1 min delay=5-12 min

MLT/MLAT dependence observed by magnetometers For the January and November events, 142 and 157 magnetometer traces were examined and 38 and 26 events were identified as having clear transition onsets. For the January and November events, 142 and 157 magnetometer traces were examined and 38 and 26 events were identified as having clear transition onsets. Red and blue dots indicate enhancements and depressions in the magnetic field Red and blue dots indicate enhancements and depressions in the magnetic field Ionospheric response was first observed 1-2 MLT before noon, and then progressed toward midnight over minutes Ionospheric response was first observed 1-2 MLT before noon, and then progressed toward midnight over minutes MLAT dependence is suggested by the November event MLAT dependence is suggested by the November event January Event November Event 37 km/s 21 km/s 1.5 km/s

MLT/MLAT dependence observed by magnetometers For the January and November events, 142 and 157 magnetometer traces were examined and 38 and 26 events were identified as having clear transition onsets. For the January and November events, 142 and 157 magnetometer traces were examined and 38 and 26 events were identified as having clear transition onsets. Red and blue dots indicate positive and negative gradients in the magnetic field Red and blue dots indicate positive and negative gradients in the magnetic field Ionospheric response was first observed 1-2 MLT before noon, and then progressed toward midnight over minutes Ionospheric response was first observed 1-2 MLT before noon, and then progressed toward midnight over minutes MLAT dependence is suggested by the November event MLAT dependence is suggested by the November event January Event November Event 37 km/s 21 km/s 1.5 km/s #1

SuperDARN-observed response The gridded l-o-s velocity was plotted for all grid cells of the 8 SuperDARN radars available for this event. The gridded l-o-s velocity was plotted for all grid cells of the 8 SuperDARN radars available for this event. Radar fields-of- view and sample grid cells are mapped in MLAT/MLT coordinates at 12:00 UT. Radar fields-of- view and sample grid cells are mapped in MLAT/MLT coordinates at 12:00 UT.

SuperDARN-observed response The average response time was 11 minutes for the PGR, KOD, and KAP radars located in the early morning sector The average response time was 11 minutes for the PGR, KOD, and KAP radars located in the early morning sector The average response time was 5 and 9 minutes for the SAS and STO radars located in the late morning sector The average response time was 5 and 9 minutes for the SAS and STO radars located in the late morning sector delay=~10-15 min delay=~5 min delay=~10 min delay=~5 min delay=~10 min

SuperDARN-observed response The average response time was 2 minutes for the GBR radar located in the 9 MLT sector The average response time was 2 minutes for the GBR radar located in the 9 MLT sector The average response time was 3 and 7 minutes for the PYK and HAN radars located in the ~16 MLT sector The average response time was 3 and 7 minutes for the PYK and HAN radars located in the ~16 MLT sector delay=~2-4 min delay=~5 min

SuperDARN-observed response The average response time was 2 minutes for the GBR radar located in the 9 MLT sector The average response time was 2 minutes for the GBR radar located in the 9 MLT sector The average response time was 3 and 7 minutes for the PYK and HAN radars located in the ~16 MLT sector The average response time was 3 and 7 minutes for the PYK and HAN radars located in the ~16 MLT sector #2 delay=~2-4 min delay=~5 min

MLT/MLAT dependence observed by SuperDARN For the January and November events, 171 and 116 grip points were identified as having clear transition onsets For the January and November events, 171 and 116 grip points were identified as having clear transition onsets Ionospheric response was first observed in the pre-noon sector and then progressed toward midnight in 5-20 minutes Ionospheric response was first observed in the pre-noon sector and then progressed toward midnight in 5-20 minutes Ionospheric response was observed first at higher latitudes and then increasingly lower latitudes for the November event (opposite to magnetic data) Ionospheric response was observed first at higher latitudes and then increasingly lower latitudes for the November event (opposite to magnetic data) January Event November Event 23 km/s 17 km/s 1.5 km/s

MLT/MLAT dependence observed by SuperDARN For the January and November events, 171 and 116 grip points were identified as having clear transition onsets For the January and November events, 171 and 116 grip points were identified as having clear transition onsets Ionospheric response was first observed in the pre-noon sector and then progressed toward midnight in 5-20 minutes Ionospheric response was first observed in the pre-noon sector and then progressed toward midnight in 5-20 minutes Ionospheric response was observed first at higher latitudes and then increasingly lower latitudes for the November event (opposite to magnetic data) Ionospheric response was observed first at higher latitudes and then increasingly lower latitudes for the November event (opposite to magnetic data) January Event November Event 23 km/s 17 km/s 1.5 km/s #1 #3

CPCP Dawnside vortex begins close to midnight and then shifts eastward at onset, reaching a steady position near 4 MLT after 16 minutes Dawnside vortex begins close to midnight and then shifts eastward at onset, reaching a steady position near 4 MLT after 16 minutes Location of the duskside vortex was highly variable until after the transition onset where it settled at 16 MLT Location of the duskside vortex was highly variable until after the transition onset where it settled at 16 MLT During periods of B z >0 the CPCP was small, compared to periods of B z 0 the CPCP was small, compared to periods of B z <0 Transition was marked by an immediate increase in the CPCP, reaching a maximum value ~40 minutes later. Transition was marked by an immediate increase in the CPCP, reaching a maximum value ~40 minutes later.

Residual convection-1 At 12:04 a positive cell starts to form near midnight and then shifts eastward over the next four intervals. At 12:04 a positive cell starts to form near midnight and then shifts eastward over the next four intervals.

Residual convection-2 At 12:14 UT the vortex of the dawnside convection cell settles at 07 MLT At 12:14 UT the vortex of the dawnside convection cell settles at 07 MLT After 12:14 UT convection evolves becoming stronger, but the vortices are stationary After 12:14 UT convection evolves becoming stronger, but the vortices are stationary

Summary of convection response based on the residual convection pattern Convection vortices do not simply ‘snap’ to their final location, but develop over a period of time Convection vortices do not simply ‘snap’ to their final location, but develop over a period of time Dawnside convection vortex takes 4-6 minutes to form and 8-10 minutes to move to a final location and then continues to enhance until a steady state is reached ~40 minutes after the initial onset Dawnside convection vortex takes 4-6 minutes to form and 8-10 minutes to move to a final location and then continues to enhance until a steady state is reached ~40 minutes after the initial onset

Summary of convection response based on the residual convection pattern Convection vortices do not simply ‘snap’ to their final location, but develop over a period of time Convection vortices do not simply ‘snap’ to their final location, but develop over a period of time Dawnside convection vortex takes 4-6 minutes to form and 8-10 minutes to move to a final location and then continues to enhance until a steady state is reached ~40 minutes after the initial onset Dawnside convection vortex takes 4-6 minutes to form and 8-10 minutes to move to a final location and then continues to enhance until a steady state is reached ~40 minutes after the initial onset #4

Summary and Conclusions – 1 Line-plots of the perturbation magnetic field were generated in the 03, 05, 10, and 14 MLT sectors. The delay between the expected arrival time of the ionospheric onset and the magnetometer-observed response was shorter for stations in the 10 and 14 MLT sectors, and longer in the 03 and 05 MLT sectors. Line-plots of the perturbation magnetic field were generated in the 03, 05, 10, and 14 MLT sectors. The delay between the expected arrival time of the ionospheric onset and the magnetometer-observed response was shorter for stations in the 10 and 14 MLT sectors, and longer in the 03 and 05 MLT sectors. Line plots of the gridded l-o-s velocity were generated throughout the MLT sector. The delay between the expected arrival time of the ionospheric onset and the SuperDARN-observed response varied from 0-20 minutes, with shorter delays observed in the MLT region and longer delays closer to 02 MLT. Line plots of the gridded l-o-s velocity were generated throughout the MLT sector. The delay between the expected arrival time of the ionospheric onset and the SuperDARN-observed response varied from 0-20 minutes, with shorter delays observed in the MLT region and longer delays closer to 02 MLT. Ionospheric onset times were determined for all available magnetometer stations and all available SuperDARN grid- cells. For both data sets, the initial onset was observed near noon and propagated toward the nightside. Ionospheric onset times were determined for all available magnetometer stations and all available SuperDARN grid- cells. For both data sets, the initial onset was observed near noon and propagated toward the nightside.

Summary and Conclusions - 2 Prior to the southward transition, the vortex of the dawnside convection cell was located close to midnight. After the southward transition, the vortex of the dawnside cell propagated eastward and settled at ~05 MLT within minutes. Prior to the southward transition, the vortex of the dawnside convection cell was located close to midnight. After the southward transition, the vortex of the dawnside cell propagated eastward and settled at ~05 MLT within minutes. The location of the duskside convection cell was erratic during periods of northward IMF, but settled at 16 MLT within ~16 minutes of the southward transition. The location of the duskside convection cell was erratic during periods of northward IMF, but settled at 16 MLT within ~16 minutes of the southward transition. The southward transition of the IMF was immediately marked by an increase in the CPCP determined by SuperDARN. The southward transition of the IMF was immediately marked by an increase in the CPCP determined by SuperDARN.

Two-stage process Stage 1 (~15 min): Stage 1 (~15 min): Noon-to-midnight progression of the ionospheric onset of the observed magnetic and electric field response (5-6 min) Noon-to-midnight progression of the ionospheric onset of the observed magnetic and electric field response (5-6 min) Foci of the Dungey convection cells moves from the nightside to the dayside (8-10 min) Foci of the Dungey convection cells moves from the nightside to the dayside (8-10 min) Stage 2 (~25 min): Stage 2 (~25 min): Overall convection pattern intensifies Overall convection pattern intensifies

Curiosities (1) Noon to midnight progression not really seen on the dusk side (1) Noon to midnight progression not really seen on the dusk side (2) Conflicting results for the PYK/HAN radars and magnetometer data (2) Conflicting results for the PYK/HAN radars and magnetometer data (3) MLAT dependency for magnetometers and SuperDARN data (3) MLAT dependency for magnetometers and SuperDARN data (4) CPCP shows immediate response but residual convection shows a delay of 5-6 minutes (4) CPCP shows immediate response but residual convection shows a delay of 5-6 minutes

The End