determination of a realistic precision measure for ... · a significant difference between the s...

1
The meteorologicly well-accepted modell of takes the state of aggregation into account and is given by Murray The differences between this two modells increase for high temperatures. In the area of the Antarctic Peninsula this effect could be neglected. Within the associated literature (e.g. or ) different values for the empirical constants could be found. compared and analysed various experiments and methods in order to find a best set of constants . The upper and the middle graph show the wet refractivity differences of the above mentioned models with respect to temperature and water vapour pressure. To be able to evaluate the significance of the effect of these differences the third graph shows the standard deviation of the temperature depending on temperature and water vapour pressure. These values were determined under the demand: = 1. An of these differences . k k N i i D Thayer Bevis et al. Rueger effect on ( ) values is not detectable I P WV Determination of a realistic Precision Measure for Integrated Precipitable Water Vapour Values in the Area of the Antarctic Peninsula Michael Mayer 1 1 1 2 , Carolin Schmitt Francisco Gonzalez , Bernhard Heck and Christoph Kottmeier 12 , Geodetic Institute University of Karlsruhe (TH) Introduction 1 2 Geodetic Institute, University of Karlsruhe (TH), Germany Institute for Meteorology and Climate Research, University of Karlsruhe (TH), Forschungszentrum Karlsruhe GmbH, Germany Within the data evaluation process of global satellite navigation systems (e.g. GPS) one has to handle all with care in order to guarantee point positions. The factors, which are affecting the GPS, are classified in satellite-related, atmospheric, and site-specific factors. Analyzing the limiting atmospheric effects, the most important and most critical areas of the he of the neutrosphere. Thus, water vapour is a limiting factor for GPS applications. For precise point positioning applications using GPS data, one has to model and estimate the neutrospheric effects in order to guarantee results of highest quality. Based on the standard evaluation of GPS data the neutrospheric noise could be used to determine values of the ( ). In the framework of a case study carried out for the area of the efforts are made to evaluate a realistic measure for the precision and the accuracy of estimates. As external reference the meteorological data of the is used. highly precise and accurate earth's atmosphere are the ionosphere (approx. 50 - 1000 km) and the subjacent electrical neutral atmosphere ( ). The poster will focus on the neutrosphere consisting of troposphere, stratosphere, and mesosphere, and especially on t IWV limiting factors water vapour integrated water vapour Antarctic Peninsula GPS-based integrated water vapour NCEP Reanalysis neutrosphere Results Institute for Meteorology and Climate Research University of Karlsruhe (TH) SV SV Ionosphere Neutrosphere direct, euklidian distance Curved, true signal apparent true n<1 n>1 Space Thermosphere Mesosphere Stratosphere Troposphere Temperature Composition Ionisiation Protonosphere Ionosphere Neutrosphere Homosphere Heterosphere Height [km] 100000 _ 10000 _ 1000 _ 100 _ 10 _ 0_ ( ) ò ò - = - = D SV E 6 SV E d 10 d 1 s N s n Zenit NEU r D NEU Zenith Based on the estimates of the of the zenithal neutrospheric effect values for the integrated water vapour and the ( ) could be determined using IPWV wet part integrated precipitable water vapour whereas the parameter depends on the empirical constants , on the specific gas constants of dry and wet air as well as on the and the density of water . k R r mean atmospheric temperature T If it is not assumed, that the atmosphere behaves like a mixture of two es, could be calculated depending e.g. on the T . ideal gas compressibility factor Z In addition to the GPS-based determination of values these values could be calculated using independent data sources like weather models (e.g. NCEP reanalysis) e.g. with respect to specific humdity and under the ideal gas asumption by means of IPWV q gravity g Basic Formulas ò ò = H Z T e H TZ e T w w m d d 2 IWV=PD NEU w , Zenith ² 3 2 1 T e k T e k T p k N d + + = Within the determination of values of the based on GPS observations the functional conection between the refractivity index resp. the refractivity and the neutrospheric effect along the curved way path in the direction of the local topocentric direction is given by IWV n N s D NEU Zenith Hereby could be calculated with respect to meteorological parameters , and and experimentaly determined constants using N k pressure of the dry air water vapour pressure temperature , i w w i . . and , P m w m P ÷ ÷ l ö ç ç L æ + = ÷ ÷ l ö ç ç L æ - + = ÷ ÷ l ö ç ç L æ - + = 2 3 6 1 2 3 6 1 2 3 6 10 10 10 k T k R R R k k T k R M M k k T k R m w w d m w d w m w IPWV IWV = / r d/w d = ò ¥ p p p g q P IPWV 0 0 d 1 = ò ¥ H H w H T e R H IPWV and . Assumptions NCEP pressure [hPa] relative humidity Are only limited (height, resolution) model data sets existing one has to to the surface resp. height of GPS site (lower limit). If the value of the highest layer (scetch: 300 hPa) is not equal to zero, an extrapolation to the upper limit (presented investigations: 200 hPa) is also needed. Both extrapolations can only be carried out under certain (linear extrapolation downward; =0) , so that the following formulas result. (e.g. relative humidity of NCEP reanalysis), f extrapolate constraints 200hPa 1 , 1 , 1 , 200 + + + D » å i i p p i i i i p g q P IPWV surf 1 , 1 , 1 , 200 1 + + + D » å i i H H i i i i w H T e R H IPWV surf In order to evaluate an area of precision which guarantees reliable NCEP-based values investigations with respect to different affecting parameters were carried out, especially the , the , the , the , the , and the were taken into account. The analysed NCEP data covers the months January and February of the years 1995, 1998, and 2002. The NCEP data has a temporal resolution of 6 h. The standard vertical resolution of the pressure layers up to 300 hPa is 8. The horizontal resolution is 2.5° (latitude, longitude). NCEP provides e.g. information for geopotential height, humidity, and temperature at different pressure layers. IPWV mean atmospheric temperature formulas used to calculate water vapour pressure effect of compressibility factors resolution (vertical, horizontal) of the NCEP data values of the empirical constants integration approach gravity formulas height definitions k including and i -70.0 -67.5 -65.0 -62.5 -60.0 -57.5 -55.0 -52.5 -50.0 -47.5 -45.0 -72.5 -70.0 -67.5 -65.0 -62.5 -60.0 longitude [°] latitude [°] ozean ozean continent mixed zone Within the redundant parameter estimation of standard GPS applications the effect of the neutrosphere is handled in two ways. On the one hand the neutrospheric effect is (e.g. Saastamoinen, Askne and Nordius, Niell), developed for and under (i.E. standard atmosphere conditions), on the other hand site-specific and time- dependend are estimated based on real GPS observations. Both modelling elements depend e.g. on the value of the so-called . This value varies between 273.00 and 273.16. The effect of an error due to the difference of the absolute zero-point on the water vapour pressure [hPa] with respect to the temperature [°C] is shown for two calculation approaches of the water vapour pressure, called BS and Murray. The model used within the (BS) is given by predicted based on modells specific regions various assumptions improvements for this predictions absolute zero-point of the temperature scale Bernese GPS Software The most important affecting parameter is due to the vertical resolution of the layered NCEP reanalysis data. The increment of the NCEP pressure levels varies between 75 hPa and 100 hPa. If this standard vertical resolution is used to carry out the piecewise summation in order to gain ( ) values a systematic and significant difference between the two summation approaches (summation with respect to the pressure difference of two consecutive pressure layers) and (summation with respect to the geopotential height difference corresponding to two consecutive pressure layers) results. Within the associated graphs the mean values are shown as well as the corresponding RMS-values for the 66 grid points each based on 708 NCEP-realizations of the earth’s atmosphere. The graphs also contain three different characteristics of both summation approaches. Hereby the expression “layer8!=0” stands for “value of the highest layer of relative humidity is not equal to 0 hPa”, whereas “layer8=0” stands for “value of the highest layer of relative humidity is equal to 0 hPa”, and “layer87=0” stands for “values of the minimum two highest layers of relative humidity are equal to 0 hPa”. I P WV p H D D If the vertical resolution is virtualy increased by means of the hydrostatic governing equation (e.g. 5 hPa) the difference between both summation approaches is highly reduced. So that only by means of virtual increasing of the vertical resolution the - and the -approach provide the same ( ) values. The other above mentioned effects (e.g. effect of compressibility factors) are not or weakly significant, normally. D D p H I P WV [] [] ² K 8T 0.00025690 - K 0.2131665T 37.2465 - e 100 + ÷ l ö ç L æ = f e f e 100 = [] ( ) [] b T T a - - K 16 . 273 K e 1078 . 6 aice = 21.8745584 bice = 7.66 K awater = 17.2693882 bwater = 35.86 K -0,05 0,00 0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,40 26,9 23,9 20,9 17,9 14,9 11,9 8,9 5,9 2,9 -0,1 -3,1 -6,1 -9,1 -12,2 -15,2 -18,2 -21,2 Temperature [° C] BS_Standard (f=90) BS_Standard (f=80) BS_Standard (f=70) BS_Standard (f=60) BS_Standard (f=50) BS_Standard (f=40) BS_Standard (f=30) BS_Standard (f=20) BS_Standard (f=10) Difference [hPa] { In order to calculate values of integrated (precipitable) water vapour the mean atmospheric temperature has to be determined. Therefore different formulas are existing, e.g. developed by Bevis et al. or Braun et al., enabling the calculation based on values of the surface temperature (T ). Using NCEP values of the continental part of the Antarctic Penisula these suface- temperature-based approaches were compared to Peninsula-adapted approaches. Detectable are: a significant difference between the standard and the Peninsula-adapted approache no dependence on the latitude no significant difference between linear and 2 order polynomial approach. Therefore, in order to guarantee results of highest quality the determination of a functional model to calculate the mean atmospheric temperature based on the surface temperature is recommended. s ! ! ! nd regional-adapted linear polynomial 2nd order continent linear continent - - - - - - - - - - comparison of the wet part (Rueger-Bevis) comparison of the wet part (Rueger-Thayer) demand: =1 sMean [mm] Grid Points Grid Points Mean [mm] Grid Points Grid Points

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Page 1: Determination of a realistic Precision Measure for ... · a significant difference between the s tan dr h eP i ul - p approache nodependenceonthelatitude no significant difference

The meteorologicly well-accepted modell of takes the state of

aggregation into account and is given by

Murray

The differences between this two modells increase for high temperatures. In the

area of theAntarctic Peninsula this effect could be neglected.

Within the associated literature

(e.g. or )

different values for the

empirical constants could be

found. compared and

analysed various experiments

and methods in order to find a

best set of constants .

The upper and the middle graph

show the wet refractivity

differences of the above

mentioned models with respect

to temperature and water

vapour pressure. To be able to

evaluate the significance of the

effect of these differences the

third graph shows the standard

deviation of the temperature

depending on temperature and

water vapour pressure. These

values were determined under

the demand: = 1.

An of these differences

.

k

k

N

i

i

D

Thayer Bevis et al.

Rueger

effect

on ( ) values is not

detectable

I P WV

Determination of a realistic Precision Measure for Integrated PrecipitableWater Vapour Values in the Area of the Antarctic Peninsula

Michael Mayer1 1 1 2, Carolin Schmitt Francisco Gonzalez , Bernhard Heck and Christoph Kottmeier

12,

Geodetic InstituteUniversity of Karlsruhe (TH)

Introduction

1

2

Geodetic Institute, University of Karlsruhe (TH), Germany

Institute for Meteorology and Climate Research, University of Karlsruhe (TH), Forschungszentrum Karlsruhe GmbH, Germany

Within the data evaluation process of global satellite navigation systems

(e.g. GPS) one has to handle all with care in order to

guarantee point positions. The factors, which

are affecting the GPS, are classified in satellite-related, atmospheric, and

site-specific factors.

Analyzing the limiting atmospheric effects, the most important and most

critical areas of the

he of the

neutrosphere. Thus, water vapour is a limiting factor for GPS

applications. For precise point positioning applications using GPS data,

one has to model and estimate the neutrospheric effects in order to

guarantee results of highest quality. Based on the standard evaluation of

GPS data the neutrospheric noise could be used to determine values of

the ( ).

In the framework of a case study carried out for the area of the

efforts are made to evaluate a realistic measure for the

precision and the accuracy of

estimates. As external reference the meteorological data of the

is used.

highly precise and accurate

earth's atmosphere are the ionosphere (approx. 50 -

1000 km) and the subjacent electrical neutral atmosphere ( ).

The poster will focus on the neutrosphere consisting of troposphere,

stratosphere, and mesosphere, and especially on t

IWV

limiting factors

water vapour

integrated water vapour

Antarctic

Peninsula

GPS-based integrated water vapour

NCEP

Reanalysis

neutrosphere

Results

Institute for Meteorologyand Climate Research

University of Karlsruhe (TH)

SVSV

Ionosphere

Neutrosphere

direct, euklidiandistance

Curved,true signal

apparenttrue

n<1

n>1

Space

Thermosphere

Mesosphere

Stratosphere

Troposphere

Temperature Composition Ionisiation

Protonosphere

Ionosphere

NeutrosphereHomosphere

Heterosphere

Heig

ht [k

m]

100000 _

10000 _

1000 _

100 _

10 _

0 _

( ) òò -=-=DSV

E

6

SV

E

d10d1 sNsnZenit

NEUrDNEU

Zenith

Based on the estimates of the of the zenithal neutrospheric effect values for the integrated water vapour and

the ( ) could be determined usingIPWV

wet part

integrated precipitable water vapour

whereas the parameter depends on the empirical constants , on the specific gas constants of dry and wet air

as well as on the and the density of water .

k

R rmean atmospheric temperature T

If it is not assumed, that the atmosphere behaves like a mixture of two es, could be calculated depending

e.g. on the

T

.

ideal gas

compressibility factor Z

In addition to the GPS-based determination of values these values could be calculated using independent data

sources like weather models (e.g. NCEP reanalysis) e.g. with respect to specific humdity and under the

ideal gas asumption by means of

IPWV

q gravity g

Basic Formulas

òò

=H

ZT

e

HTZ

e

T

w

wm

d

d

2

IWV=PD NEU w,

Zenith

²321

T

ek

T

ek

T

pkN d ++=

Within the determination of values of the based on GPS observations the functional conection between the

refractivity index resp. the refractivity and the neutrospheric effect along the curved way path in the

direction of the local topocentric direction is given by

IWV

n N sDNEU

Zenith

Hereby could be calculated with respect to meteorological parameters ,

and and experimentaly determined constants using

N

k

pressure of the dry air water vapour

pressure temperature, i

w

w

i

.

.

and ,

Pm

w

m

P

÷÷ø

öççè

æ+

=

÷÷ø

öççè

æ-+

=

÷÷ø

öççè

æ-+

=

23

6

123

6

123

6 101010

kT

kR

R

Rkk

T

kR

M

Mkk

T

kR

m

w

w

d

m

w

d

w

m

w

IPWV IWV= / r

d/w

d= ò¥p

p

pg

qPIPWV

0 0

d1

= ò¥H

Hw

HT

e

RHIPWVand .

Assumptions

NCEP

pre

ssu

re [

hP

a]

relative humidity

Are only limited (height, resolution) model data sets existing one has to

to the surface resp. height of GPS site (lower limit). If the value of the highest layer (scetch: 300 hPa) is

not equal to zero, an extrapolation to the upper limit (presented investigations: 200 hPa) is also needed. Both

extrapolations can only be carried out under certain (linear extrapolation downward; =0) , so that

the following formulas result.

(e.g. relative humidity of NCEP reanalysis),

f

extrapolate

constraints 200hPa

1,

1,

1,200

+

+

+ D» å ii

p

p ii

iip

g

qPIPWV

surf

1,

1,

1,

200

1+

+

+ D» å ii

H

H ii

ii

w

HT

e

RH

IPWV

surf

In order to evaluate an area of precision which guarantees reliable

NCEP-based values investigations with respect to different

affecting parameters were carried out, especially the

, the , the

, the

, the , and the

were taken into account.

The analysed NCEP data covers the months January and February of

the years 1995, 1998, and 2002. The NCEP data has a temporal

resolution of 6 h. The standard vertical resolution of the pressure layers

up to 300 hPa is 8. The horizontal resolution is 2.5° (latitude,

longitude). NCEP provides e.g. information for geopotential height,

humidity, and temperature at different pressure layers.

IPWV

mean atmospheric

temperature formulas used to calculate water vapour pressure

effect of compressibility factors resolution (vertical, horizontal) of

the NCEP data values of the empirical constants

integration approach gravity formulas height definitions

k

including and

i

-70.0 -67.5 -65.0 -62.5 -60.0 -57.5 -55.0 -52.5 -50.0 -47.5 -45.0

-72.5

-70.0

-67.5

-65.0

-62.5

-60.0

longitude [°]la

titu

de

[°]

ozean ozean continent mixed zoneWithin the redundant parameter estimation of standard GPS applications the

effect of the neutrosphere is handled in two ways. On the one hand the

neutrospheric effect is (e.g. Saastamoinen,Askne and

Nordius, Niell), developed for and under

(i.E. standard atmosphere conditions), on the other hand site-specific and time-

dependend are estimated based on real GPS

observations. Both modelling elements depend e.g. on the value of the so-called

. This value varies between 273.00

and 273.16. The effect of an error due to the difference of the absolute zero-point

on the water vapour pressure [hPa] with respect to the temperature [°C] is shown

for two calculation approaches of the water vapour pressure, called BS and

Murray.

The model used within the (BS) is given by

predicted based on modells

specific regions various assumptions

improvements for this predictions

absolute zero-point of the temperature scale

Bernese GPS Software

The most important affecting parameter is due to the vertical resolution

of the layered NCEP reanalysis data. The increment of the NCEP pressure levels varies between 75 hPa and 100 hPa. If this standard vertical

resolution is used to carry out the piecewise summation in order to gain ( ) values a systematic and significant difference between the two

summation approaches (summation with respect to the pressure difference of two consecutive pressure layers) and (summation with

respect to the geopotential height difference corresponding to two consecutive pressure layers) results. Within the associated graphs the mean

values are shown as well as the corresponding RMS-values for the 66 grid points each based on 708 NCEP-realizations of the earth’s atmosphere.

The graphs also contain three different characteristics of both summation approaches. Hereby the expression “layer8!=0” stands for “value of the

highest layer of relative humidity is not equal to 0 hPa”, whereas “layer8=0” stands for “value of the highest layer of relative humidity is equal to

0 hPa”, and “layer87=0” stands for “values of the minimum two highest layers of relative humidity are equal

to 0 hPa”.

I P WV

p HD D

If the vertical resolution is virtualy increased by means of the hydrostatic governing equation (e.g. 5 hPa) the

difference between both summation approaches is highly reduced. So that only by means of virtual

increasing of the vertical resolution the - and the -approach provide the same ( ) values.

The other above mentioned effects (e.g. effect of compressibility factors) are not or weakly significant,

normally.

D Dp H I P WV

[ ] [ ]²K8T0.00025690-K0.2131665T37.2465-e100

+÷ø

öçè

æ=

fe

fe

100=

[ ]( )[ ] bT

Ta

-

-

K

16.273K

e1078.6

aice = 21.8745584

bice = 7.66 K

awater = 17.2693882

bwater = 35.86 K

-0,05

0,00

0,05

0,10

0,15

0,20

0,25

0,30

0,35

0,40

26,923,920,917,914,911,98,95,92,9-0,1-3,1-6,1-9,1-12,2-15,2-18,2-21,2

Temperature [° C]

BS_Standard (f=90) BS_Standard (f=80) BS_Standard (f=70)

BS_Standard (f=60) BS_Standard (f=50) BS_Standard (f=40)

BS_Standard (f=30) BS_Standard (f=20) BS_Standard (f=10)

Dif

fere

nce [

hP

a]

{

In order to calculate values of integrated

(precipitable) water vapour the mean

atmospheric temperature has to be

determined. Therefore different formulas are

existing, e.g. developed by Bevis et al. or

Braun et al., enabling the calculation based on

values of the surface temperature (T ).

Using NCEP values of the continental part of

the Antarctic Penisula these suface-

temperature-based approaches were

compared to Peninsula-adapted approaches.

Detectable are:

a significant difference between the

standard and the Peninsula-adapted

approache

no dependence on the latitude

no significant difference between linear

and 2 order polynomial approach.

Therefore, in order to guarantee results of

highest quality the determination of a

functional model to

calculate the mean atmospheric temperature

based on the surface temperature is

recommended.

s

!

!

!

nd

regional-adapted

linearpolynomial 2nd order

continent

linear continent

-

----

-----

comparison of the wet part (Rueger-Bevis)

comparison of the wet part (Rueger-Thayer)

demand: =1sN

N-D

iffe

rence

N-D

iffe

rence

sT

Temperature [K]

Temperature [K]

Temperature [K]

Mean

[m

m]

Grid Points

S SS

W W W W W W W W W W W W W W W W W W W W W W

S S S S S S S S S S S S S S S S S SS

Grid Points

S S S S S S S S S S S S S S S S S S S S S S

W W W W W W W W W W W W W W W W W W W W W W

Mean

[m

m]

Grid Points

W W W W W W W W W W W W W W W W W W W W W W

S S S S S S S S S S S S S S S S S S S S S S

Grid Points

S S S S S S S S S S S S S S S S S S S S S S

W W W W W W W W W W W W W W W W W W W W W W