SAR Calibration Certificate

FCC ID: QDMPPR11

RF Exposure Info

Download: PDF
FCCID_3829411

KCTL Inc. Report No.: 65, Sinwon-ro, Yeongtong-gu, Suwon-si, Gyeonggi-do, 16677, Korea KR18-SPF0002-A Tel : 82-31-285-0894 Fax : 82-505-299-8311 Page (28) of (53) www.kctl.co.kr Appendix A. Calibration certificate A.1 Probe Calibration certificate This test report shall not be reproduced, except in full, without the written approval. KCTL-TIA002-004/1

. KCTL Calibration Laboratory of Schweizerischer Kallbrirdionst w o w Schmid & Partner Service suisse détalonnage Engineering AG Servizio svizzero dtaratura Zeughausstrasse 43, 8004 Zurich, Switzerland Swiss Calibration Service Accredited by the Swiss Accreditation Service (SAS) Accreditation No.: SCS 0108 The Swiss Accreditation Service is one of the signatories to the EA Multiateral Agroement for the recognition of calibration cortficates Glossary: TSL tissue simulating liquid NORMxcy,z sensitivityin free space ConvF sensitivity in TSL / NORMy,z DCP diode compression point CF crest factor (1/duty_cycle) of the RF signal A, B,C, D modulation dependentlinearization parameters Polarization rotation around probe axis Polarization 8 8 rotation around an axis that is in the plane normal to probe axis (at measurement center), Le. 0 is normal to probe axis Connector Angle information used in DASY system to align probe sensor X to the robot coordinate system Calibration is Performed According to the Following Standards: a) IEEE Std 1528—2013, "IEEE Recommended Practice for Determining the Peak Spatial—Averaged Specific Absorption Rate (SAR) in the Human Head from Wireless Communications Devices: Measurement Techniques®, June 2013 b) 12C 622001 , ‘Measurement procedure for the assessmentof Specific Absorption Rate (SAR) from hand— held and body—mounted devices used next to the ear (frequency range of 300 MHz to 6 GHz)®, July 2016 0 IEC 62209—2, "Procedure to determine the Specific Absorption Rate (SAR) for wireless communication devices used in close proximity to the human body (frequency rangeof 30 MHz to 6 GHz)*, March 2010 d KDB 865664, "SAR Measurement Requirements for 100 MHz to 6 GHz" Methods Applied and Interpretation of Parameters: NORMxy,z: Assessed for E—field polarization 8 = 0 (f = 900 MHz in TEM—cell; {> 1800 MHz: R22 wevegulde} NORMxy,z are only intermediate values, ie., the uncertainties of NORMx,y,z does not affect the E*—field uncertainty inside TSL (see below ConvF). NORM()xy,z = NORMx,y,z * frequency_response (see Frequency Response Chart). This linarization is implemented in DASY4 software versions later than 4.2. The uncertainty of the frequency responseis included in the stated uncertainty of ConvF. DCPxy,z: DCP are numerical inearization parameters assessed based on the data of power sweep with CW signal (no uncertainty required). DCP does not depend on frequency nor media. PAR: PAR is the Peak to Average Ratio that is not calibrated but determined based on the signal characteristics Axy.z; Buy,z: Coy.z; Dxy,z; VRxy,z: A, B, C, D are numerical inearization parameters assessed based on the data of power sweep for specific modulation signal. The parameters do not depend on frequency nor media. VR is the maximum calibration range expressed in RMS voltageacross the diode. Convand Boundary Effect Parameters: Assessed in flat phantom using E—field (or Temperature Transfer Standard for f s 800 MHz) and inside waveguide using analytical field distributions based on power measurements for 1 > 800 MHz. The same setups are used for assessment of the parameters applied for boundary compensation (alpha, depth) of which typical uncertainty values are given. These parameters are used in DASY4 software to improve probe accuracy close to the boundary. The sensitivity in TSL corresponds to NORMxy,z * ConvF whereby the uncertainty corresponds to that given for ConvF. A frequency dependent ConvF is used in DASY version 4.4 and higher which allows extending the validity from + 50 MHz to + 100 MHz. Spherical isotropy (3D deviation from isotropy); in a field of low gradients realized using a flat phantom exposed by a patch antenna. Sensor Offset: The sensor offset corresponds to the offset of virtual measurement center from the probe tip (on probe axis). No tolerance required. Connector Angle: The angle is assessed using the information gained by determining the NORMx (no uncertainty required). Certficate No: EX3—3028_Jan18 Page 2 of 11

<—> 0 (KCTL EXGDVé — SN:3028 January 23, 2018 Probe EX3DV4 SN:3928 Manufactured: March 8, 2013 Calibrated: January 23, 2018 Calibrated for DASY/EASY Systems (Note: non—compatible with DASY2 system!) Certficate No: EX3—3028_Jant8 Page 3 of 11

KCTL EXGDV4— SN:3028 January 23, 2018 DASY/EASY — Parameters of Probe: EX3DV4 — SN:3928 Basic Calibration Parameters Sensor K Sensor Y SensorZ Une (ke2) Norm (Vi(Vim)) 0.49 021 055 £10.1% DCP (mV)" se EFG 100.6 Modulation Calibration Parameters up Communication System Name A s 6 b vr Une® aB aByjv as my (ke2) o ow x oo o0 10 on fses #25% y o0 o0 10 Tse8 2 o0 o0 10 1478 The reported uncertainty of measurement is stated as the standard uncertainty of measurement multiplied by the coverage factor k=2, which for a normal distribution corresponds to a coverage probability of approximately 95%. ‘ The uncertainties of Norm XY.Z do not affect the E*feld uncertainty insde TSL (see Pages 5 and 6) * Numericalinearization parameter: uncertainty not required. Uncertainty is determined using the max. deviation from linear response applying rectangular distrbution and is expressed forthe square of the field value. Certficate No: EX3—3028_.Jant8 Page 4 of 11

Lo o KCTL EXGDV4~ SN:3028 January 23, 2018 DASY/EASY — Parameters of Probe: EX3DV4 — SN:3928 Calibration Parameter Determined in Head Tissue Simulating Media Relative Conductivity Depth® Une £(MHz)®_|_ Pormittivity" (Sim)" ConvFX ConvEY ConvEZ Aipha®| (mm) (ke2) 750 410 0.89 9.79 a.79 9.70 0.44 0.80 £120% 850 41.5 0.92 9.47 9.47 9.47 0.41 0.88 £12.0% 900 41.5 0.97 9.28 9.28 9.28 0.37 0.97 £12.0% 1750 40.1 1.37 8.34 8.34 8.34 0.29 0.80 £12.0% 1900 40.0 140 8.09 8.09 8.00 0.34 0.80 £120% 2300 39.5 1.67 7.68 7.68 7.68 0.37 0.80 £12.0% 2450 39.2 1.80 7.28 7.28 7.28 0.34 0.94 £12.0% 2600 39.0 196 717 77 717 0.35 084| £120% 5200 36.0 4.66 5.40 5.40 5.40 0.35 180 £181% 5300 35.9 4.76 5.15 5.15 5.15 0.35 180 £131% 5500 35.6 4.96 4.98 4.98 4.98 0.40 180 £13.1% 5600 35.5 5.07 484 4.84 4.84 0.40 180 £13.1% 5800 35.3 527 4.79 4.79 4.70 0.40 180 £181% © Frequency valdty above 300 Mz of : 100 MHz only apples for DASY v4.4 and higher (see Page 2), es i is restricted to + 50 MHz. The uncertainty is the RSS of the ConvE: uncertainty at calloration frequency and the uncertaintyfor the indlcated frequency band. Frequency valdty below 300 Mtiz is + 10, 25, 40, 50 and 70 MHz for Convassessments at 20, 64, 128, 150 and 220 MHz respectvely. Above 5 GHz frequency yalidty can be extended to + 110 MHz. " Atfrequencies below 3 GH, the validty ofssue parameters (e and a) can be relaxed to + 10% ifiquid compensation formula is applied to measured SAR values. At requencies above 3 GHiz,the validty oftissue parameters (s and a)is restrcted to + 5%. The uncertaiy is the RSS of the Convuncertainty foindicated target tssue parameters. * AhaDapth are determined during calbration. SPEAG warrants thatthe remaining deviation due to the boundary effect ater compensation is always less than : 19% for requencies below 3 GHiz and below * 2% for fequencies between 3—6 GHz at any distance larger than halfthe probe tip ciameter from the boundary. Certficate No: EX3—3928_Jan18 Page 5 of 11

KCTL EXGDV4— SN:3028 January 23, 2018 DASY/EASY — Parameters of Probe: EX3DV4 — SN:3928 Calibration Parameter Determined in Body Tissue Simulating Media Relative Conductivity Depth Une £(MHz)_|_ Pormittivity" (Sim)" ConvFX ConvEY ConvFZ Aipha® |__(mm) (ke2) 750 588 0.%6 9.70 9.70 9.70 0.42 0.89 £120% 850 55.2 0.99 9.36 9.36 9.36 0.48 0.84 £120% 00 55.0 1.05 9.26 9.26 9.26 0.44 089 £120% 1750 53.4 149 7.85 785 7.85 o43 084 £120% 1900 53.3 152 7.50 7.59 7.59 0.43 0.80 £120% 2300 52.9 1.81 744 744 744 0.38 0.85 £12.0 % 2450 52.7 1.95 7.38 7.38 7.38 0.37 0.85 £12.0 % 2600 525 2.16 6.87 6.87 6.87 0.25 1.02 £12.0 % 5200 49.0 5.30 4.85 4.85 4.85 0.35 190 £131% 5300 48.9 542 4.65 4.65 4.65 0.35 1.90 £13.1% 5500 48.6 5.65 4.30 4.30 4.30 0.40 1.90 £13.1% se00 48.5 577 4.10 4.10 4.10 0.40 100 a18.1% 5800 48.2 £.00 4.37 4.37 4.37 0.40 190 £131% © Frequency valdty above 300 Mz of : 100 MHz only apples for DASY v4.4 and higher (see Page 2else ts resticted to + 50 MHz. The uncertainty is the RSS o the Conv: uncertainty at calloration frequency and the uncertainty for the indicated frequency band. Frequency valdity below 300 Mz is x 10, 25,40, 50 and 70 MHz for ConvE assessments at 30, 64, 128, 150 and 220 VHz respectively. Above 5 GHz frequency validty can be extended to + 110 iz * Atfrequencies below 3 GHz,the validty ofissue parameters (e and a) can be relaxed to : 10% ifiquid compensation formula is applied to measured SAR values. At requencies above 3 GHz,the validty oftissue parameters (e and 0)is restrcted to + 5%. The uncertaints the RSS of the Corv‘® uncertainty foindicated target issue parameters. * AphaDepth are determined during caltration. SPEAG warrants thatthe remaining deviation due to the boundary effect aftr compensation is always less than + 1% for frequencies below 3 GHiz and below + 2% for fequencies between .6 GHz at any ditance larger than halfthe probe tip diameter rom the boundary: Certficate No: EX3—3028_Jan18 Page 6 of 11

<—<<—~ lc KCTL EXGDV4~ SN:3028 January 23, 2018 Frequency Response of E—Field (TEM—Cell:ifi110 EXX, Waveguide: R22) Frequency response (normalized) Uncertainty of Frequency Response of E—field: 2 6.3% (k=2) Certficate No: EX3—3928_Jan18 Page 7 of 11

EXGDV4— SN:3028 January 23, 2018 Receiving Pattern (¢), 8 = 0° £=600 MHz,TEM £21800 MHz,R22 w we o i r as > is as "—@s * * * * # xo n To x ® 2 To £cicc ioi ‘ 4‘%0 I ® I -g.fl 6 RotP] & 10%%!11 sc%’—u 1e Wz sWz Uncertainty of Axial Isotropy Assessment: £ 0.5% (k=2) Certiicate No: EX3—3928_Jan18 Page 8 of 11

KCTL EXGDV4— SN:3928 January 23, 2018 Dynamic Range f(SARneaq) (TEM cell , fou= 1900 MHz) € 10° F3 5 & & & 103 102 10 10 10‘ 10 SAR {mWiem9] C+] Ce] not compensated compensated 2 1 @ . & wClkan 07 s w I I 103 102 101 108 101 1of 108 SAR {mWiomd] C+] not compensated compensated Uncertainty of Linearity Assessment: £ 0.6% (k=2) Certiicate No: EX3—3028_Jan18 Page 9 of 11

P j | KCTL EXGDV4— SN:3028 January 23, 2018 Conversion Factor Assessment 1= 850 MHz.WGLS RO (H_convr) 1= 1900 MHz.WGLS R22 (H_comr) s i . s[ w5 B s % ¢s 2 a is io se > sfim a a sf «3B wille wiBle Deviation from Isotropy in Liquid Error (6, 3), f= 900 MHz jation «10 —o8 ~o6 ~os 02 o0 o2 o4 o% o8 10 Uncertainty of Spherical Isotropy Assessment: £ 2.6%(k=2) Certiicate No: EX3—3928_Jan18 Page 10 of 11

KCTL Inc. Report No.: 65, Sinwon-ro, Yeongtong-gu, Suwon-si, Gyeonggi-do, 16677, Korea KR18-SPF0002-A Tel : 82-31-285-0894 Fax : 82-505-299-8311 Page (38) of (53) www.kctl.co.kr This test report shall not be reproduced, except in full, without the written approval. KCTL-TIA002-004/1

KCTL Inc. Report No.: 65, Sinwon-ro, Yeongtong-gu, Suwon-si, Gyeonggi-do, 16677, Korea KR18-SPF0002-A Tel : 82-31-285-0894 Fax : 82-505-299-8311 Page (39) of (53) www.kctl.co.kr A.2 Dipole Calibration certification D2450V2 This test report shall not be reproduced, except in full, without the written approval. KCTL-TIA002-004/1

Calibration : Laboratory of s Schweizerischer Kalibrierdienst Schml_d & Partner g Service suisse d‘étalonnage Engineering AG Servizio svizzero di taratura Zeughausstrasse 43, 8004 Zurich, Switzerland s Swiss Calibration Service Aceredited by the Swiss Accreditation Service (SAS) Accreditation No.: SCS 0108 The Swiss Accreditation Service is one of the signatories to the EA Multilateral Agreement for the recognition of callbration certificates Glossary: TSL tissue simulating liquid ConvF sensitivity in TSL / NORM xy,z N/A not applicable or not measured Calibration is Performed According to the Following Standards: a) IEEE Std 1528—2013, "IEEE Recommended Practice for Determining the Peak Spatial— Averaged Specific Absorption Rate (SAR) in the Human Head from Wireless Communications Devices: Measurement Techniques", June 2013 b) EC 62209—1, "Procedure to measure the Specific Absorption Rate (SAR) for hand—held devices used in close proximity to the ear (frequency range of 300 MHz to 3 GHz)®, February 2005 c) IEC 62209—2, "Procedure to determine the Specific Absorption Rate (SAR) for wireless communication devices used in close proximity to the human body (frequency range of 30 MHz to 6 GHz)®, March 2010 d) KDB 865664, "SAR Measurement Requirements for 100 MHz to 6 GHz" Additional Documentation: e) DASY4/5 System Handbook Methods Applied and Interpretation of Parameters: * Measurement Conditions: Further details are available from the Validation Report at the end of the certificate. All figures stated in the certificate are valid at the frequency indicated. * Antenna Parameters with TSL: The dipole is mounted with the spacerto position its feed point exactly below the center marking of the flat phantom section, with the arms oriented parallel to the body axis. * Feed Point Impedance and Returm Loss: These parameters are measured with the dipole positioned under the liquid filled phantom. The impedance stated is transformed from the measurement at the SMA connector to the feed point. The Return Loss ensures low reflected power. No uncertainty required. * Electrical Delay: One—way delay between the SMA connector and the antenna feed point. No uncertainty required. * SAR measured: SAR measured at the stated antenna input power. * SAR normalized: SAR as measured, normalized to an input power of 1 W at the antenna connector. * SAR for nominal TSL parameters: The measured TSL parameters are used to calculate the nominal SAR result. The reported uncertainty of measurementis stated as the standard uncertainty of measurement multiplied by the coverage factor k=2, which for a normal distribution corresponds to a coverage probability of approximately 95%. Certificate No: D2450V2—805_Jul16 Page 2 of 8

. bonmm ree reenerene ec Do _C Nevermvern wg ng nnvripage mm d n en g n nc Mess nc e en en > I r—m mm mss mss mss mss mm Measurement Conditions DASY system configuration, as far as not given on page 1. DASY Version DASYS V52.8.8 Extrapolation Advanced Extrapolation Phantom Modular Flat Phantom Distance Dipole Center — TSL 10 mm with Spacer Zoom Scan Resolution dx, dy, dz =5 mm Frequency 2450 MHz + 1 MHz Head TSL parameters The following parameters and calculations were applied. Temperature Permittivity Conductivity Nominal Head TSL parameters 22.0 °C 30.2 1.80 mho/m Measured Head TSL parameters (22.0 £0.2) °C 38.0 6 % 1.86 mhoim 2 6 % Head TSL temperature change during test <0.5°C ud ~— SAR result with Head TSL SAR averaged over 1 em(1 g) of Head TSL Condition SAR measured 250 mW input power 13.3 Whg SAR for nominal Head TSL parameters normalized to 1W 52.0 Wikg 17.0 % (k=2) SAR averaged over 10 em* (10 g) of Head TSL condition SAR measured 250 mW input power 6.15 Wig SAR for nominal Head TSL parameters normalized to 1W 24.3 Wikg x 16.5 % (k=2) Body TSL parameters The following parameters and calculations were applied. Temperature Permittivity Conductivity Nominal Body TSL parameters 22.0 °C 52.7 1.95 mho/m Measured Body TSL parameters (22.0 £0.2) °C 51.8 26 % 2.03 mho/m + 6 % Body TSL temperature change during test <0.5°C m n SAR result with Body TSL SAR averaged over 1 m‘ (1 g) of Body TSL Condition SAR measured 250 mW input power 13.0 Wikg SAR for nominal Body TSL parameters normalized to 1W 50.8 Wikg 17.0 % (k=2) SAR averaged over 10 cm* (10 g) of Body TSL condition SAR measured 250 mW input power 6.05 Wig SAR for nominal Body TSL parameters normalized to 1W 23.0 Wikg 2 16.5 % (k=2) Certiicate No: D2450V2—895_Jul6 Page 3 of 8

Appendix (Additional assessments outside the scope of SCS 0108) Antenna Parameters with Head TSL Impedance, transformed to feed point 54.1 0+22j0 Retun Loss —27.0 dB Antenna Parameters with Body TSL Impedance, transformed to feed point 49.8 2 + 4.0 jQ Retun Loss —28.0 dB General Antenna Parameters and Design Electrical Delay (one direction) | 1.158 ns _] After long term use with 100W radiated power, only a slight warming of the dipole near the feedpoint can be measured. The dipole is made of standard semirigid coaxial cable. The center conductor of the feeding line is directly connected to the second arm of the dipole. The antenna is therefore short—circuited for DC—signals. On some of the dipoles, small end caps are added to the dipole arms in order to improve matching when loaded according to the position as explained in the ‘MeasurementConditions" paragraph. The SAR data are not affected by this change. The overall dipole length is still according to the Standard. No excessive force must be applied to the dipole arms, because they might bend or the soldered connections near the feedpoint may be damaged. Additional EUT Data Manufactured by SPEAG Manufactured on June19, 2012 Certificate No: D2450V2—895_Jult6 Page 4 of 8

DASY5 Validation Report for Head TSL Date: 25.07.2016 Test Laboratory: SPEAG, Zurich, Switzerland DUT: Dipole 2450 MHz D2450V2; Type: D2450V2; Serial: D2450V2 — SN:895 Communication System: UID 0 — CW; Frequency: 2450 MHz Medium parameters used: f= 2450 MHz; 0 = 1.86 S/m; & = 38; p = 1000 kg/m‘ Phantom section: Flat Section Measurement Standard: DASYS (IEEE/AEC/ANSI C63.19—2011) DASY32 Configuration: * Probe: EX3DV4 — SN7349; ConvF(7.72, 7.72, 7.72); Calibrated: 15.06.2016; * Sensor—Surface: 1.4mm (Mechanical Surface Detection) * Electronics: DAE4 Sn601; Calibrated: 30.12.2015 * Phantom: Flat Phantom 5.0 (front); Type: QDOOOP50AA; Serial: 1001 «_ DASY52 52.8.8(1258); SEMCAD X 14.6.10(7372) Dipole Calibration for Head Tissue/Pin=250 mW, d=10mm/Zoom Scan (7x7x7)/Cube 0: Measurement grid: dx=mm, dy=5mm, dz=5mm Reference Value = 114.6 V/m; Power Drift=—0.01 dB Peak SAR (extrapolated) = 27.2 W/kg SAR(L g) = 13.3 W/kg; SAR(1O g) = 6.15 W/kg Maximum value of SAR (measured) = 22.0 W/kg ~4.62 —9.24 —13.85 18.47 —23.09 0 dB =22.0 W/kg = 13.42 dBW/kg Certificate No: D2450V2—805_Jul16 Page 5 of 8

KCTL Impedance Measurement Plot for Head TSL 25 gul zere es:ssres CHD sar i ucrs 1840590 220120 14299 pH 2 450.000 ooo miz by 18° ma cn2 si1__loe s de/rer ~20 o 11=27.008 8 _2 «50.000 000 kz Stakt 2 250.000 00 Miz Stor 2 e50.000 000 Miz Certificate No: D2450V2—805_Jul6 Page 6 of 8

KCTL DASY5 Validation Report for Body TSL Date: 25.07.2016 Test Laboratory: SPEAG, Zurich, Switzerland DUT: Dipole 2450 MHz D2450V2; Type: D2450V2; Serial: D2450V2 — SN:895 Communication System: UID 0 — CW; Frequency: 2450 MHz Medium parameters used: £= 2450 MHz; 0 = 2.03 S/m; &, = 51.8; p = 1000 kg/m‘ Phantom section: Flat Section Measurement Standard: DASY5 (IEEE/AEC/ANSI C63.19—2011) DASY52 Configuration: Probe: EX3DV4 — SN7349; ConvF(7.79, 7.79, 7.79); Calibrated: 15.06.2016; Sensor—Surface: 1.4mm (Mechanical Surface Detection) Electronics: DAE4 Sn601; Calibrated: 30.12.2015 Phantom: Flat Phantom5.0 (front); Type: QDOOOP5OAA; Serial: 1001 DASY52 52.8.8(1258); SEMCAD X 14.6.10(7372) Dipole Calibration for Body Tissue/Pin=250 mW, d=10mm/Zoom Scan (7x7x7)/Cube 0: Measurement grid: dx=3mm, dy=Smm, dz=5mm Reference Value = 106.8 V/m; Power Drift =—0.03 dB Peak SAR (extrapolated) = 26.0 W/kz SAR (1 g) = 13 W/kg; SAR(1O g) = 6.05 W/kg Maximum value of SAR (measured) = 21.2 W/kg ~4.40 —8.79 41319 —17.58 —21.98 0 dB =21.2 W/kg = 13.26 dBW/kg Certificate No: D2450V2—895_Jult6 Page 7 of 8

KCTL Inc. Report No.: 65, Sinwon-ro, Yeongtong-gu, Suwon-si, Gyeonggi-do, 16677, Korea KR18-SPF0002-A Tel : 82-31-285-0894 Fax : 82-505-299-8311 Page (46) of (53) www.kctl.co.kr This test report shall not be reproduced, except in full, without the written approval. KCTL-TIA002-004/1


Document Created: 2018-04-20 16:59:33
Document Modified: 2018-04-20 16:59:33
© 2024 FCC.report
This site is not affiliated with or endorsed by the FCC