Return-Path: Received: from post.thorcom.com (post.thorcom.com [195.171.43.25]) by klubnl.pl (8.14.4/8.14.4/Debian-8+deb8u2) with ESMTP id x2CGe4WT018925 for ; Tue, 12 Mar 2019 17:40:11 +0100 Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1h3kLT-00065w-Pq for rs_out_1@blacksheep.org; Tue, 12 Mar 2019 16:33:39 +0000 Received: from [195.171.43.32] (helo=relay1.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1h3kLQ-00065n-Ga for rsgb_lf_group@blacksheep.org; Tue, 12 Mar 2019 16:33:36 +0000 Received: from sonic316-11.consmr.mail.bf2.yahoo.com ([74.6.130.121]) by relay1.thorcom.net with esmtp (Exim 4.91) (envelope-from ) id 1h3kLO-0002bc-74 for rsgb_lf_group@blacksheep.org; Tue, 12 Mar 2019 16:33:35 +0000 DKIM-Signature: v=1; a=rsa-sha256; c=relaxed/relaxed; d=aol.com; s=a2048; t=1552408409; bh=0nN39rfdcGcpo1dbjBa311gBnfy2iT0Fag0scGNc8fM=; h=Date:From:To:Subject:References:From:Subject; b=JCTO0cBe4aRg/O+gueIx93ItONDsYckWqpaOs/b563gQDRblN9vuF1KL92crbFcgWHdDfAkBZu5OOP9bXzpJws/lQYhhj+rg6N0R+K7QmZjUAHRk2xBBE30CqY0rmrTNDjJxr48be2fLFcgApYwiFv4aJAcD1XzpJ0niXLd16F3NO5y1NKwvoCIcVPPJu6/SRz0MWJfyx04Wov8sxupBK/tBKoNuiYs8LBMcjO8FelkRptn9pkes7bI6Et48pnmxCHYjEI8tihJ8so1WHppnXvyA+G+9ZvNhmSaVWr85NSEUqRTIBjHCymk0ijex56qs2TJj36+oIqpsr68Sh0QHtQ== X-YMail-OSG: so1diFQVM1l_wnwZOWY.ODlEgbafIKG.fFB6Qf2tuKVoIJSUtksoUbXjTwHd6wU tiPCE3S0vn6YY88RLrXjcVh8Ux.r1de8s8_i73gLWMxPIriDSQYHALyvWFa2ly6sug5Fc2rs027p 556Qb.3f2ihXgX3HmdQ6SY3rNzI2lAIV47431NvPI9aFvKIC1SRxryogIVjDdXyEwxYAShOWLgjC iKhpnuVKYZc_snlPgMh2hKlmes3sgabzTHPc1aySlEacDcUs84FT1dWU9X6o1EcIrDCS7jV7K7vj DjT1j5z5zYo3NIBRIjSq8XjezgN7ju1TrCXEr7PMwoLocM2LaK90ZOQbc4LJ2kuqqD2R0JxYFBOH ZzcpuV9Ek8iMeUGDQrLf12K_n5BzFTC7GGb08Xf0ZZYMQCFsGVs01chc.aP7x_kJRUkh_ahR4M5o grhA8FJZgQIPkK1RQLyCrUXkLvCcbe7JYUVsSpcdOug71S1cnNy6BgXTg.yy3quGr9Dt1EVA2naD OdcnXTvbsD.UnGifCd_tCoaFRY8AHAUJt0ZzxEbppngdW1dj_5OEb0i2HK1nIwX8AQNvD54uNKDJ 5Q4._z6.VvEVKBnlcfmwdGngved4MZWR7oTZUskpP1ImgHNK.Fg1fXIdbeGPTAuKS0mM2M8efKIx 9pcTpiYlUUAoQPhjzMRltiMdDBU1vLjw.QjbYz1wB8_i0dyz7yXwfEDeRLTVbMnXSJ3QI1tyFvWs fKKnNj9.tSqwFZb_.Qdo_eqXTncLftbeiPPnv13C5BTHwzpD2OR7LqiQ415pasMzwwcvEL_XtlYk ZcMfYKxBZmLud3O2Fclz01BKg4q_Q7cT8AQMddma50hGAXIsjhxBjV.xjCYRVy0C5Tez0cYoS7ad qYLICNrY9Whx5gyTpfKHmSguwKIQpUkJ1c2h8hqWQMv89aD74UsHExx.woojkYRNKs.yH49dZkTY Vfj4uiKPAqvlETAw2PZpOqDrH4W_Pd8ic5U6z1IsVF9Pyc9gJTQ51Vqzpxx4TpzY6EiWSgeFdjlH 3n.8IZqSpOG15qQ-- Received: from sonic.gate.mail.ne1.yahoo.com by sonic316.consmr.mail.bf2.yahoo.com with HTTP; Tue, 12 Mar 2019 16:33:29 +0000 Date: Tue, 12 Mar 2019 16:33:26 +0000 (UTC) From: Markus Vester To: rsgb_lf_group@blacksheep.org Message-ID: <1811819281.3633936.1552408406386@mail.yahoo.com> MIME-Version: 1.0 References: <1811819281.3633936.1552408406386.ref@mail.yahoo.com> X-Mailer: WebService/1.1.13212 aolwebmail Mozilla/5.0 (Windows NT 6.1; WOW64; Trident/7.0; rv:11.0) like Gecko X-Spam-Score: 0.0 (/) X-Spam-Report: Spam detection software, running on the system "relay1.thorcom.net", has NOT identified this incoming email as spam. The original message has been attached to this so you can view it or label similar future email. If you have any questions, see the administrator of that system for details. Content preview: Hi Stefan, why not drive the antenna in parallel resonance? This would provide a better impedance match to the low current high voltage DC source. You'd preferably want a high voltage transistor, which could a [...] Content analysis details: (0.0 points, 5.0 required) pts rule name description ---- ---------------------- -------------------------------------------------- -0.0 RCVD_IN_DNSWL_NONE RBL: Sender listed at http://www.dnswl.org/, no trust [74.6.130.121 listed in list.dnswl.org] -0.0 SPF_PASS SPF: sender matches SPF record 0.0 FREEMAIL_FROM Sender email is commonly abused enduser mail provider (markusvester[at]aol.com) 0.0 HTML_MESSAGE BODY: HTML included in message X-Scan-Signature: c172b771707a94a5bc2f57171c0c1a85 Subject: Re: LF: Re: Re Loomis? & ... 12.47 Hz Content-Type: multipart/mixed; boundary="----=_Part_3633935_947996224.1552408406386" X-Spam-Checker-Version: SpamAssassin 2.63 (2004-01-11) on post.thorcom.com X-Spam-Level: *** X-Spam-Status: No, hits=3.2 required=5.0 tests=FORGED_MUA_MOZILLA,HTML_20_30, HTML_MESSAGE autolearn=no version=2.63 X-SA-Exim-Scanned: Yes Sender: owner-rsgb_lf_group@blacksheep.org Precedence: bulk Reply-To: rsgb_lf_group@blacksheep.org X-Listname: rsgb_lf_group X-SA-Exim-Rcpt-To: rs_out_1@blacksheep.org X-SA-Exim-Scanned: No; SAEximRunCond expanded to false ------=_Part_3633935_947996224.1552408406386 Content-Type: multipart/alternative; boundary="----=_Part_3633934_1991748924.1552408406383" ------=_Part_3633934_1991748924.1552408406383 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: quoted-printable Hi Stefan, why not drive the antenna in parallel resonance? This would provide a bette= r impedance match to the low current high voltage=C2=A0DC source. You'd=C2= =A0preferably want a high voltage transistor, which could also operate=C2= =A0in class-C with low duty cycle. >From my experience, 100 uA DC seems=C2=A0overly optimistic. Best I=C2=A0got= from my ant (40 m of wire) was 1 to 2 uA, which was actually during a prec= ipitation static event (aka Grabber whiteout). In fair weather, the current= is normally not measurable with a 10 Mohm millivoltmeter, i.e. less than ~= 0.1 nA. Best 73, Markus -----Urspr=C3=BCngliche Mitteilung----- Von: DK7FC An: rsgb_lf_group Verschickt: Di, 12. Mrz 2019 16:09 Betreff: Re: LF: Re: Re Loomis? & ... 12.47 Hz Well, today: The circuit in operation on the INV-L since last night,=20 100% WSPR @MF. The reports on the local RX in 20m distance were between=20 0...+7 dB at night and -11...-9 dB in daylight. On the tree grabber in 3.5 km distance the signal was only detectable at=20 night, levels reaching about -24 dB in average. Nothing in daylight. Where does the energy come from? It must be the voltages coming from=20 other transmitters (DC to HF) which leave voltages up to the range of 1=20 V at this antenna. This RX voltage spectrum is modulated by the circuit=20 and radiates a very weak signal. That's why the signal is about 13 dB=20 weaker in daylight. In this experiment this is an unwanted effect. It=20 causes some kind of offset, i.e. it lowers the SNR difference to a=20 signal generated by cloud charges. So the 'sky-current' must be higher=20 to become clearly observable. And it is easier to detect it in daylight. The effect should be less expressed at LF because the external voltages=20 from other transmitters are the same but the expected voltage from a 100=20 uA 'sky-current' will be 475/137 higher, i.e. the system is 10 dB more=20 sensitive for the observation of the expected effect. Unfortunately there is no LF monitor on the tree... Anyway i need to be more patient. There has been no static rain yet=20 anyway... Meanwhile i read a bit about Miller capacity and=20 https://en.wikipedia.org/wiki/Cascode. I built one out of two BS170 FETs=20 somehow it does not work yet. 73, Stefan Am 11.03.2019 17:24, schrieb DK7FC: > ...the circuit is completed (attached). > First i used a simple rectangular input signal coming from the source,=20 > over an ferrite core. The gate voltage was +-10V. But then, obviously=20 > due to the FETs internal reverse transfer capacitance i got a 200 mVpp=20 > output across 470 pF (tested in the lab, later to be replaced by the=20 > antenna). I built a test source for the assumed 100 uA 'sky-current'=20 > by using a 1 kV voltage source and 10 MOhm in series. As assumed, a=20 > linear rising voltage was observed during the off-times of the FET.=20 > However, together with the voltage coming over the Crss, the residual=20 > rms value even dropped! Thus i had to reduce the gate peak-peak=20 > voltage and ended up with the circuit shown in the attachment. There=20 > is a DC offset and the AC component is as low as possible. The reduced=20 > the unwanted voltage 8 mV. > Then, 50 mV rms at 475 kHz at 100 uA DC 'sky-current'. > > How far will a 50 mV rms WSPR signal be detectable? And will the=20 > 'sky-current' reach 100 uA at all? At least the signal strength will=20 > rise with the square of that current, so the report are nearly as good=20 > as a current measurement. > > 73, Stefan > > > > Am 11.03.2019 13:29, schrieb DK7FC: >> Hello Jim, >> >> Yes, indeed. >> I'm now preparing the circuit and want to set it up in the evening.=20 >> Found an IRF820 in the 'junk box', a good choice. Or, maybe even a=20 >> BS170 will work. It handles 60V only but i had the following thought: >> >> The ERP at a constant voltage across the antenna (say 50 V rms at the=20 >> fundamental frequency) will rise with the sqare of the frequency (for=20 >> electrically short antennas). But that voltage will not be constant=20 >> in practice. It will drop linearly with the frequency ( ~ 1/f)=20 >> because the sky-current is assumed to be constant and the charge up=20 >> time is T/2. And, doubling the voltage at the antenna will also rise=20 >> the ERP by a factor of 4. All in all it means the the ERP is=20 >> constant, or independend of the frequency!? >> That means, it would be wise to select a band where many RX stations=20 >> are watching and propagation is promising. The number of RX stations=20 >> is higher at MF but (groundwave) propagation is better at LF. >> Since the peak voltage will be lower at MF (shorter charge-up time),=20 >> MF is less critical. >> >> And which mode?! I think the best choice is a 100% duty cycle WSPR=20 >> beacon. It also has the advantage that one can check the results in=20 >> the database. And there are many RX stations, even in the groundwave=20 >> distance and even in less than 100 km here. And i have my tree which=20 >> can detect small differences at very low levels. >> At MF, the BS170 is a good choice i think. And it can be driven by a=20 >> Raspi directly, maybe with a ferrite transformer in the gate-source=20 >> path, to decouple the shack from the antenna... >> >> If that works, one could try LF. >> >> 73, Stefan >> >> >> >> Am 10.03.2019 20:18, schrieb hvanesce@comcast.net: >>> All great ideas in the preceding messages. >>> >>> A steady signal from the 136 kHz sky-current transmitter could=20 >>> indicate that a data bit might be available later from the 10 Hz=20 >>> sky-current transmitter. >>> >>> Agreed, the triggered gap sounds better than an HV vacuum relay (for=20 >>> jitter and reliability). >>> >>> Sounds like the voltage divider doesn't need to be more than a=20 >>> gigohm, but perhaps for future reference: a reliable 50kV 1 terohm=20 >>> divider can be made very easily: encapsulate ten 100 gigohm=20 >>> resistors in hard epoxy, being sure not to touch them during=20 >>> assembly. A single linearity calibration after curing will be remain=20 >>> valid +/- 10% for years in varying humidity and temperature. >>> >>> 73, >>> >>> Jim AA5BW >>> >>> >>> -----Original Message----- >>> From: owner-rsgb_lf_group@blacksheep.org=20 >>> [mailto:owner-rsgb_lf_group@blacksheep.org] On Behalf Of DK7FC >>> Sent: Sunday, March 10, 2019 5:52 AM >>> To: rsgb_lf_group@blacksheep.org >>> Subject: Re: LF: Re: Re Loomis?&=C2=A0 ... 12.47 Hz >>> >>> Hi Jacek, DC, >>> >>> Yes yes, i already see a new project for summer :-) >>> >>> A floating antenna will charge up to a voltage where the E field=20 >>> strength is high enough to start partial discharges, something like=20 >>> 20 kV maybe, depending on the wire diameters and homogenity of the=20 >>> arrangement, also on pressure and humidity. So there will be a=20 >>> voltage limit given by the arrangement. But a higher field strength=20 >>> in summer will help to charge up the antenna faster, so higher=20 >>> switching frequencies are possible. >>> >>> One could build/use a triggered spark gap,=20 >>> https://en.wikipedia.org/wiki/Trigatron, this will hold higher=20 >>> voltages and you can connect the trigger directly to a ublox GPS=20 >>> module running e.g. at 3 Hz :-) I think this will give a lower=20 >>> jitter than when using a vacuum relay. >>> Could this work over my 3.5 km path if i use my inv-L? I don't think=20 >>> so. >>> The time to integrate will be to short and there will be much QRN=20 >>> during such an experiment, so the SNR will be very low. Currently=20 >>> (at 12.47 Hz) i already have 15 kV DC available... >>> >>> Anyway, interesting questions, there is something interesting to learn. >>> Maybe i will do a few experiments in summer. Building a HV divider=20 >>> and measurement should be no problem... >>> >>> 73, Stefan >>> >>> PS: Assuming 100 uA constant current 'coming from the sky', my 470=20 >>> pF antenna would charge up with 213 kV/s, so it would be possible to=20 >>> switch at 10 Hz and get a 21 kV 'square wave'. Maybe the harmonics=20 >>> could be detected easier than the fundamental frequency. >>> At 137 kHz it would be 1.5 V only (0.53 V rms). This can be switched=20 >>> with a normal FET! Imagine we would switch the antenna permanently=20 >>> at, say 136.172 kHz, using a FET and a ublox GPS module. Then, as=20 >>> soon as the field strength is high enough, we would see a carrier on=20 >>> the grabbers? We need to try that out! Amazing! What a great hobby=20 >>> we have!?! >>> PPS: For this experiment, the antenna can be series resonated, which=20 >>> would help to concentrate the energy to the wanted spectrum... >> ------=_Part_3633934_1991748924.1552408406383 Content-Type: text/html; charset=UTF-8 Content-Transfer-Encoding: quoted-printable
Hi Stefan,

why not drive the antenna in parallel = resonance? This would provide a better impedance match to the low current h= igh voltage DC source. You'd preferably want a high voltage trans= istor, which could also operate in class-C with low duty cycle.
From my experience, 100 uA DC seems overly optimistic. Best I go= t from my ant (40 m of wire) was 1 to 2 uA, which was actually during a pre= cipitation static event (aka Grabber whiteout). In fair weather, the curren= t is normally not measurable with a 10 Mohm millivoltmeter, i.e. less than = ~ 0.1 nA.

Best 73,
Markus

-----Urspr=C3=BCngliche Mitteilu= ng-----
Von: DK7FC <selberdenken@posteo.de>
An: rsgb_lf_group &= lt;rsgb_lf_group@blacksheep.org>
Verschickt: Di, 12. Mrz 2019 16:09Betreff: Re: LF: Re: Re Loomis? & ... 12.47 Hz

Well, today: The circuit in operation on the INV-L since last nigh= t,
100% WSPR @MF. The reports on the local RX in 20m dis= tance were between
0...+7 dB at night and -11...-9 dB in= daylight.
On the tree grabber in 3.5 km distance the sig= nal was only detectable at
night, levels reaching about = -24 dB in average. Nothing in daylight.

Where does the energy come from? It must be the voltages coming from
other transmitters (DC to HF) which leave voltages up to the= range of 1
V at this antenna. This RX voltage spectrum = is modulated by the circuit
and radiates a very weak sig= nal. That's why the signal is about 13 dB
weaker in dayl= ight. In this experiment this is an unwanted effect. It
= causes some kind of offset, i.e. it lowers the SNR difference to a
signal generated by cloud charges. So the 'sky-current' must be = higher
to become clearly observable. And it is easier to= detect it in daylight.
The effect should be less express= ed at LF because the external voltages
from other transm= itters are the same but the expected voltage from a 100
= uA 'sky-current' will be 475/137 higher, i.e. the system is 10 dB more
sensitive for the observation of the expected effect.
Unfortunately there is no LF monitor on the tree...

Anyway i need to be more patient. There has been = no static rain yet
anyway...
Meanwhile= i read a bit about Miller capacity and
https://en.wikipedia.org/wiki/Cascode. I built one= out of two BS170 FETs
somehow it does not work yet.

73, Stefan


Am= 11.03.2019 17:24, schrieb DK7FC:
> ...the circuit is = completed (attached).
> First i used a simple rectangu= lar input signal coming from the source,
> over an fe= rrite core. The gate voltage was +-10V. But then, obviously
> due to the FETs internal reverse transfer capacitance i got a 200 = mVpp
> output across 470 pF (tested in the lab, later= to be replaced by the
> antenna). I built a test sou= rce for the assumed 100 uA 'sky-current'
> by using a= 1 kV voltage source and 10 MOhm in series. As assumed, a
> linear rising voltage was observed during the off-times of the FET. =
> However, together with the voltage coming over the = Crss, the residual
> rms value even dropped! Thus i h= ad to reduce the gate peak-peak
> voltage and ended u= p with the circuit shown in the attachment. There
> i= s a DC offset and the AC component is as low as possible. The reduced
> the unwanted voltage 8 mV.
> Then, = 50 mV rms at 475 kHz at 100 uA DC 'sky-current'.
>
> How far will a 50 mV rms WSPR signal be detectable? And= will the
> 'sky-current' reach 100 uA at all? At lea= st the signal strength will
> rise with the square of= that current, so the report are nearly as good
> as = a current measurement.
>
> 73, St= efan
>
>
>> Am 11.03.2019 13:29, schrieb DK7FC:
>> Hello Jim,
>>
>> = Yes, indeed.
>> I'm now preparing the circuit and w= ant to set it up in the evening.
>> Found an IRF82= 0 in the 'junk box', a good choice. Or, maybe even a
>= ;> BS170 will work. It handles 60V only but i had the following thought:=
>>
>> The ERP at a constan= t voltage across the antenna (say 50 V rms at the
>&g= t; fundamental frequency) will rise with the sqare of the frequency (for >> electrically short antennas). But that voltage wi= ll not be constant
>> in practice. It will drop li= nearly with the frequency ( ~ 1/f)
>> because the = sky-current is assumed to be constant and the charge up
= >> time is T/2. And, doubling the voltage at the antenna will also ri= se
>> the ERP by a factor of 4. All in all it mean= s the the ERP is
>> constant, or independend of th= e frequency!?
>> That means, it would be wise to se= lect a band where many RX stations
>> are watching= and propagation is promising. The number of RX stations
>> is higher at MF but (groundwave) propagation is better at LF.
>> Since the peak voltage will be lower at MF (shorter= charge-up time),
>> MF is less critical.
>>
>> And which mode?! I think the = best choice is a 100% duty cycle WSPR
>> beacon. I= t also has the advantage that one can check the results in
>> the database. And there are many RX stations, even in the groun= dwave
>> distance and even in less than 100 km her= e. And i have my tree which
>> can detect small di= fferences at very low levels.
>> At MF, the BS170 i= s a good choice i think. And it can be driven by a
>&= gt; Raspi directly, maybe with a ferrite transformer in the gate-source >> path, to decouple the shack from the antenna...>>
>> If that works, one coul= d try LF.
>>
>> 73, Stefan<= br clear=3D"none">>>
>>
>= ;>
>> Am 10.03.2019 20:18, schrieb hvanesce@comcast.net:
>>> All great ideas in the preceding messages.
>>>
>>> A steady signal from the 136= kHz sky-current transmitter could
>>> indicate= that a data bit might be available later from the 10 Hz
>>> sky-current transmitter.
>>>
>>> Agreed, the triggered gap sounds better than an H= V vacuum relay (for
>>> jitter and reliability)= .
>>>
>>> Sounds like= the voltage divider doesn't need to be more than a
>= >> gigohm, but perhaps for future reference: a reliable 50kV 1 terohm=
>>> divider can be made very easily: encapsula= te ten 100 gigohm
>>> resistors in hard epoxy, = being sure not to touch them during
>>> assembl= y. A single linearity calibration after curing will be remain
>>> valid +/- 10% for years in varying humidity and temperat= ure.
>>>
>>> 73,
>>>
>>> Jim AA5BW
>>>
>>>
&g= t;>> -----Original Message-----
>>> From: = owner-rsgb_lf_group@blacksheep.org
>>> [ma= ilto:owner-rsgb_lf_group@blacksheep.org] On Behalf Of DK7FC
>>> Sent: Sunday, March 10, 2019 5:52 AM
>>> To: rsgb_lf_group@blacksheep.org
>>> Su= bject: Re: LF: Re: Re Loomis?&  ... 12.47 Hz
>= ;>>
>>> Hi Jacek, DC,
&g= t;>>
>>> Yes yes, i already see a new proj= ect for summer :-)
>>>
>>= ;> A floating antenna will charge up to a voltage where the E field
>>> strength is high enough to start partial discha= rges, something like
>>> 20 kV maybe, depending= on the wire diameters and homogenity of the
>>>= ; arrangement, also on pressure and humidity. So there will be a
>>> voltage limit given by the arrangement. But a higher= field strength
>>> in summer will help to char= ge up the antenna faster, so higher
>>> switchi= ng frequencies are possible.
>>>
>>> One could build/use a triggered spark gap,
>>> https://en.wikipedia= .org/wiki/Trigatron, this will hold higher
>>&= gt; voltages and you can connect the trigger directly to a ublox GPS
>>> module running e.g. at 3 Hz :-) I think this will= give a lower
>>> jitter than when using a vacu= um relay.
>>> Could this work over my 3.5 km pat= h if i use my inv-L? I don't think
>>> so.
>>> The time to integrate will be to short and there= will be much QRN
>>> during such an experiment= , so the SNR will be very low. Currently
>>> (a= t 12.47 Hz) i already have 15 kV DC available...
>>= >
>>> Anyway, interesting questions, there is= something interesting to learn.
>>> Maybe i wil= l do a few experiments in summer. Building a HV divider
= >>> and measurement should be no problem...
>= >>
>>> 73, Stefan
>&g= t;>
>>> PS: Assuming 100 uA constant current = 'coming from the sky', my 470
>>> pF antenna wo= uld charge up with 213 kV/s, so it would be possible to
= >>> switch at 10 Hz and get a 21 kV 'square wave'. Maybe the harmo= nics
>>> could be detected easier than the fund= amental frequency.
>>> At 137 kHz it would be 1.= 5 V only (0.53 V rms). This can be switched
>>>= with a normal FET! Imagine we would switch the antenna permanently
>>> at, say 136.172 kHz, using a FET and a ublox GPS m= odule. Then, as
>>> soon as the field strength = is high enough, we would see a carrier on
>>> t= he grabbers? We need to try that out! Amazing! What a great hobby
>>> we have!?!
>>> PPS: For t= his experiment, the antenna can be series resonated, which
>>> would help to concentrate the energy to the wanted spectrum= ...
>>

<= /div>
------=_Part_3633934_1991748924.1552408406383-- ------=_Part_3633935_947996224.1552408406386 Content-Type: image/jpeg Content-Transfer-Encoding: base64 Content-Transfer-Encoding: base64 Content-Disposition: attachment; filename="Loomis_parallel_resonance.jpg" Content-ID: <6wfAzpSboXIXAWKCXf4n> /9j/4AAQSkZJRgABAQAAAQABAAD/2wBDAAYEBQYFBAYGBQYHBwYIChAKCgkJChQODwwQFxQYGBcU FhYaHSUfGhsjHBYWICwgIyYnKSopGR8tMC0oMCUoKSj/2wBDAQcHBwoIChMKChMoGhYaKCgoKCgo KCgoKCgoKCgoKCgoKCgoKCgoKCgoKCgoKCgoKCgoKCgoKCgoKCgoKCgoKCj/wAARCAE1AW4DAREA AhEBAxEB/8QAHAAAAgIDAQEAAAAAAAAAAAAAAAIBAwUGBwQI/8QATBAAAQMDAwIEBAMFAwcICwAA AQACAwQFEQYSIQcxE0FRYSIycYEUkaEVI1KxwQgWQhckM3KC0eFDU2KSorLC8CUmNDVERXOTo7Px /8QAFAEBAAAAAAAAAAAAAAAAAAAAAP/EABQRAQAAAAAAAAAAAAAAAAAAAAD/2gAMAwEAAhEDEQA/ APp4jBQTsPsgcdgglAIBBLmlvdBCAQS1pI4QTsPsgVBBIAyUEOILMhBS5pcfmIHogSCLwgRuJz5e iBXsLeTjugljS3Dz2QTje4OHb3QWoLkAgEBhp75ygEAgEAOSgtYMDlBW5pb3QQghwyMIKnDsPQ5Q T9yPogV7S4cEhBUYnZ7hBawbWgFBKAQUmJ2TyEDsj2kE90FgGThBPh4+VA0TCCRxyUDgYeB7oHe0 k8IPO45KCQS35soGHZBKAQCAJJ7lAIBAAkdignJ9SghBBAPcZQQSBxhAjiCeEEIK3SDBwMn3QIXn ZtIAQQ0luDk7coLhI0nAygva4OGQglADuEEDzQSgEAgEDtfgc5KCHuDsYQKgEEOAweEFSBWvDjwg iUkM4OEExnLBlAyAQLJngDvlA6CEDsOcoHGcZCCxgy0E90EucAeUHnYARygYgHuglAIBAIBAIBAI BAIBBBaCgqGecoGdjyQUHa3ksPPugV5aRw0gnzQI1wdgZ+HKC9jWZy1BYDtGAgsHYIJQK4nPCBkA gloyRkcIBww7AQQRjugZgBzlAqAQQexQVEgZz5IKoWkE5GEFjgCMFBIAAwOyAQJJu42oHHygfdBY 0AjJ7oDaPRBIAHZBPljyQSHEDAKAOXc90FIdjjhA7jjCCR2CCUAgEAgEAgEAgEAgjI9UCSd/sgoE 2HAPGAUCtG5x3E4QE2AAMnA9ECENGNnZBZE8NBygaOUE/HgfRBe12ceiB0AgEAgZjuw4wgCfjQM4 NJ5P6oIJDflOcoEQCAQaHeLzWwdTbTaxUOZRVVFLI6IMby9p4dkjPbI9OSg3KOTJO79EFn0QCAQC AQWM+UIGbyXA+QQCAQA7hBa0ADg5QeQcOygsccIJHIQSgEAgEAggnAyUEkYQCAQS0ZOEFR+f7oB/ dBXIzfjnGEFZcHjaeMeaCs8Hg5QST8IHogHHIA9EExs3k84QX/KAPsgvaPhPsgEAgEAgEAgEAgEC l2DjCDn+ro4mdTNJVDtviPZURcjJxsyg3mNmwnnKAa/Ly3CB0AgEAS0Y+IILW8BBKAQS0ZOEA4YO EEtdtGMIPOOH5PbCCwPGeR5IJHYIJQCAQCAQCAQCAQCCt3zIAtOPJBXI0uYQ04JQUvILuECoBAIL 42FpOcILAMnCCxowEAexQQ0YygZBAOSRg8DOUEjkoG2H2QTGAc5CBEEE4CDT9b6zpdPeBTQ08tdd 6s7KajiOHOceBk87W+6DnWuJ9ctvWnL1V261QMhqX0/hQyvqXs3tI3OaNocMtHynIz2POA3qql1d aWOqK6K23eka3c5lGX08+BycNcS15wOBlqDabNX010tVJXUUgkp6iJskbx/iaR3Qe1AIJAygA3J7 BBY0YGEAeyCSMYQCAHcIJcQTwMIK2AEcoBzfQICMOA+JA6AQCAQCAQCAQCAQIQd2UDHsUFSCqZoD cgeaCsY2nPdBHb3QWNGR8LQf6ILyc+WEEs5PHkgsQI8nPdA6AQS084J4QBxnjsgMn1KCuLxAXGRp ZzgDdnI9UFhBAz5IEk+Q+eOUHPJrXHHrCxzVDWurKiWoqJXHk4DQGN+wQby+CCp2ukjbJsIxuHYg gj9QEGD11eorJYpKh/iPmdiOCKP5pHn5Wj74/JBboi2S2fStroKgETQwNEnxZ+M8u/UlBnw0nHog baPRBBbj5UClrsfD3QWDsEEoGbj/ABIIGN3PZAOxnjsghAjCMd0DoBAIBAIBAIBAIBAIBAIIceCg qQVz/J90FJBHdBLOXN+qD04wgkhA7GgDjzQMgUtBKBkAgEAOSEFmwe6CJfJApJIx5IFd8pyg4Nqp 9dNru9VU1ZXthtuyKmZBO5gjEkXDhgjHx7R90Hprr7r/AETbIrpdZ7PeLe4h0tO1xiqWAk/IScSk AjjOeOAcoM5omsHUKvj1DVt222ke5tFSn5g8d3yDPDgeMIOoNA4HkgsAwMIJQCAQCBmty0nzQKRj ugMH0KBtvw55yglrMjnIQeZBcgEAgEBx5HKAQCAQCAQCAQQ44GUFZOSghBBGceoQeF4k/EuHw+Ft Pmc7s/ywgvjbtDDnzQehAc+ZygtHYIJQCAQCAQMxuec+aCxB52zCUux/hODwe6BkEHsg0HVdDDZ9 TU18e0Ooqtgt9waW5AYfkefUA4B9kGRp9G6ep6llxprfTCZvLJCN230LckoNR6OzsrdYa7uFE4m3 VFZEYzj4XPawtcR69gfPug6w35kFiAQCAQCCyP5fugHN3HOUA47WjCCWnIyglB40Dx+aB0AgEAgE AgEAgEAgEFbvmQQRgoIQQ920ZIQQH5LRjugY9igknIHsglndBYgEEtaSOEE7D7IIaMnhBLOHoGLS XZQD2knhBWgEAgpqaeOphkimY2SN42uY8Za4e4QcI6q6aqaXVWlLZb71dqCyXOqdTz0lPUFkQBAJ Hrg+nYc4CDs+n7JQ2K2xUFrp2QU0Y4a0dz5k+6DJFpAQMz5QgZBLmlvdBCC1nyhBKAQCCH/KUER/ L90HkB+LODjCCyPzQOgEAgEB5A+RQCAQCAQCAQIQd2UA8EnhBEpDccfkgUgHuMoAAA9ggB2CAQO0 Fp5BQOgB3CCwPaOwQDwTjCAYR2A5wgARuxjlAyAQK7a3uECuII4GECoMTqesqLZYq64UtLLWS00T pW08UgY6TAyWgkYzjOEHzHqPqTqXU1VpzUNJp3/1eguwFKBODVyPaCHNIzjPB4xjgfVB3zpzr+za 6paiSyzS+NSuDKmmmjMctO45w1zT9DyCRwfRBuuOBlBKBS4A4KC13x9h2QMGjAyAglAIBAIBAjgc /D2QUP7oJj80DoBAIIJA7oDcMAZ4CAJAGUEbh6oDcPVAyAQCBXOwPdB54ayGdm6GZj25LctOeQcE fUEEILtx9UCk/F7YQCAQMwA5ygsBI7IBAIIPA5QJDVRzMD4pGvaexbyEFgOOQgMnOfNBO93qgkOc e38kA8g4wgUDPZAIFmyaaQDzBH6IPjjq5X1Whbxf7VRjw6Oativdta5vET3NLXgf7RzgeiDsX9mP SzdPdO4K2Tcbhd8Vkz3Ag4I+Ac+g5z7lB2dAIMbe6WrrKGeCirZ6KSRga2eAMMkfxZJbva5uSOOQ QgykIcM7vbCCxAIBAIBApLt3sgZB5o48j5vzQMG7fMH6IJQCCC4AgEgE9vdBDgCeSgrQSTkYQQgD 2QWsy5oOQPqglAgLt57bfL1QYu+3ektLA+tmbG152sGCXOOM8Yzyg570vvlLT6RiErKqWSSsrJ8x U5LTvqZXjkDnhyDb5NX0THhroK0euad3CCp+t7Wx+HMq2jPcwOwg9UesLI8fFXMjPpIC3+iC5up7 I4Ai60eD/wBPCD1R3y1Yy25UbgeRiUIPRT3SgqQTT1tNIB32yA4QesPaezmnPoUDINf1lqam0xap KypHiuxiKBnzyv8A4Qg41pLWeom9YLtDc7FLSPuNFGympH1XwtkjBczPGG7gXDPtz7BvcPU6Shpo BqnS97s9U4APayD8XEHejZIyQRjzICB39XtOj5Iru/nsLbNz9OEEx9WbZM8tp7HqebGMmO0ykefm gu/ypUrJdh05qhrOcvfa3tAOM+Z9kHm/yw6ea57aikvtMWnnxrVMP6IMzb+pekqudkMd/t8VS/5Y amTwHn/ZftKDZaO50NbGJKSspp2u7GKVrwfuCg9YcD8OR3QcA/tc2amqNG0VxmoGSilq42zVTHES wxuODtGMEH0PAPKDYf7Oeq63WGmrjVVUTGUVJVmkoi1ga7wWMbtDsdyA5B15ADkhBLxg8ILUAgEA gEAgEAg87OyBkAghxwMoOZUl7vVZ1ouNHHM2SxUlFTsliyB4Uzy5zXdsnIGMZ44KDpJJPdANOCgh xxkoMDpjU1JqE1/7PZIYaSoNOZXABr3AAnH54QbA12B2QM05QRv9kCHJOQcIMffHCC01tS5xzDA9 4J8sNJQa90eyemmn3uBHiUwlAJycOJI/mg3FwB8h9+UEBo8+yBHwRv8AnjY4f9JoKCh1sonnJo6X ce5MLSgoqNNWeoBEttozkAcQNH9EHnfo+wPcHm1UgeBjLWbePsg8smgdPueXNojGT/zcr24+mHcI Ik0HZHAZZVjHpUyf1KDQtWWLTenNT0LrubgKQUzn04ifK8mYPHA5POPog8ugaOe4dXayturZ43RW tstHFO7fIxrnEAuJ89pQdwLQ9oDhkeiADGhuAM+5QMgEA6Aubgu/IIPHUWukrRtrKeCdo7CSIOx+ aDXq7pzpOsqfFqLDbS5oLWllO1hAPlluOEHkPTa0wyeJa6y8W6X1pq+UD/quJb+iDD3bTWsKGknj pNQUt3odrnvpbvRteZR5s3NAznsM598hBnulDrRNoy31en7bTW2jq4xOYIIwxrXnh2cDGQQQfog3 JBY04ZlBLTuGUEoBBWZQJGsI7nAKCxArnbTjCCS7DQcIFD8kDCB0FCCUAgh3blBzzQzDJq3W1dtY fEuDKZh75EcTP6ucgeo1LcJeqLLBRxwm201tNVXTOaS5sjnbYmtIOOcOOMcDlBlbXLbqa+V1HTXJ 0tfJ/nM1K+oLzHuxyGk8N7duPZBkL1UOprNW1AdgxwPeOeeGkhBqXSChbbOn1LJKdj53PqZXyHGX Ocef0H5IN6oJ45oQ+OVkjHcte124Eex80HpQCAQYvVQ3aZuoxnNNIMf7JQYPpAMdMdM98G3wYJGM jw28oNwPDtvmgkDJQS0fFgoHwPQIJQCAQCCuWCGUDxo2vLeRkA4KDRpAyn6yQv8AhzVWhw7Y5bK3 +hQb435R9EEoBAILkAAB2CCtzTyUCoEljEkL2u+UtIP3Qc66AOb/AJNqGNgaBBNURfD7TP8AYIOk AZOEDngbfNAzRtBygAQf9yCUCPia5wdj4h2QS1pDSEC7D7IGc0loCBAMPA90FqClAIBBXPnwnY7+ SDmVpu0FjotWzzfDLFdZXBhOCXOY3YAO/Psg1rR1wOmq3VNfey6W8VMsTWxPOHvcYztYB6DOPRBj 9P6Rud21RrCK5tr6KruNOGftCJpZs3bHfC7HOCMYHoUFdLa9VaduVBpypuofRXKKelLJHGUyuEZx IP4DnbwPdBs9h09f79baGi1RTG2WuhDYvw8T8uqcADc7Hlx/NBnNBWaXTN5vVtpw79lybaqlYTkR A5Dmj6Y9fJBvG538R/NA8biOXE4QDZMSE5yEHj1C9rrDcQfOnf8A90oMD0oBPTbTAjPwtt0DOPZg Hn9EG4DOST3ygYkYGO6Bh2BQBB3eyBkAgEAgg9ig0K9gM6r6Yka0ZfR1THceQwUG+t+UfRBKAQCC x4JxhAPyGj1QR/yaBECSkhhwfqg5j/Z3a9uhKjec7rnWO47ZMzshB1FBIPxAlBL3Z+U+SBIw8lzj kOPHB4QXjsMoBAIBAEgd0COLSOO6Bcn1KCEEu28bUEIEkw5pafPhBrNXpS0S6hN4kpi6sOCcvOze Oz9vbdjjKC2axWqS7tustDA64NYIxUFuXBvog9MM8U7HmGRr2tc6Nxac4cO4KDmd/q/xHXGw0QLD 4FG+pwXc8hwyBj1H6IOqs5aCBj0QDQckuAz249P/ACSgZAzCHOy/0QK7GTjsg8GoXeHYbg8OAIpp Dz5fCUGL6SAs6a6VjecltrpgcHPPhNQbb/iHp5oA54x6oLRjHHZBKAQCAQCCDyDnsg0jVuI9faOk IA3PqYi4/wAJjzj80G7M+UfRAyAHcZ7ILA1p7IGQLJ8v3QJk4x5IIQUVb/Dp5XYyQ0kD/wA/ZBzv +z01v+TOgkYDmaaeVw93SuKDpaCCQMZ80EoJBI7ILM4aCUEg5GQgjcM480EoIdjHxdkFbsZ47IIQ CAQVzyeFEX4yByfogwWktR0+p7Qy40sU0Eb3vYGTN2u+F2CfpkFBlJcGRBVMW5AbnHug5N0bd4db r6UufJjUFQGxE5a3AaQPTlBHSGzQ3Wkh1beXSVV9NTVRxTPkP7uJ0jmhgb2wA3j3z6oOrNkO0AYO Bj7IG8VoJDu/kgsjdG5uXHBQM7bj4Sc+6BGEZdv4A7YQYnWD2s0reH5AY2jlcS70DCgr6bwsi0Jp 5kbdrWW+na1voPCbhBsqBw0YHdABgDs5KB0AgEAgEGB1dqWl01b21FQ2SaSR2yGCFu58jvQBByfU Mmuf7xaYvN0bQR0X41zW28M/eNa5vZ0mcB23OM+fdB3Gme6SGN0kZjcWglju7T6HCC1ADkhBa0YH CCUCyfL90FaAQY3UEv4ezV9QT/oqeR35NJ/og0n+z3Tfhuk2nmlvEtP43/WcXevug6P27IAjJB9E EoJaAc5OEAXEgBAzHHIHkgYtBOUEoIcARycIK3AA8dkEIBAIElGWEEZB4IQaD0lLWaNEDf8A4Wpq IHgeREznf+L9EGD1t1G/upqWoEtPVVlDDDHG6GnaDiV252S44Aw0HuUGW0j1Bs+rJxBRmelq9u8Q VUTo3ObjO5uR8Q9cZwg1fpn+MZZ9bVFJDHPWG+VroopHYEjxgNB9M+qDWOnWv/2L03qWSWyrF0gl qHMpnRu8MuMpwzeBg8nug6XpXVk1bWTWi8CkivUELal8FK8uaI3YAzkcOBzkIMJQdQK+7Vms6Gmt LYjYwRBVmQyMnkAPBaACO3kT39kGP6I68vupau6U1+npayGniimZWRR+EGucAXRnHHw5KDrlLXQV cYkppGTRnOHscHDj3CBpJTkA8goMJ1GqDF091DI1pz+AmGAe+WEIMro7jStob/DSQj/8bUGYQWNO eEDIAckBA/yHHfKBXN245QQgh3ynCDnVmY3Vutay6S/FQWc/hqRhOQZP8UnoeAPz9kGf1taqi6Wy D8EM1dNURzxfUHn9CUGxNc4ck5QWA5GUEjggoH8T2QHieyCHO3DGECoDB9OEGqdVK8W3p3qOrIJE VDMeO/yOH9f1QerQdK2i0lZqeMAMjoYQABjA2DH6INhQCAQCBo/m+yCxAIFc7acYQK524YwgVAIB AIEkGW857oOP3S5XrQl8u8MNmqLpQXKfx6J1MARHI/gh48hnzH/FBl9N6Pkdpu6RanDZq28udJVs HIYCMBo+g/XKDHW/RV1hq7PBVVtE602mXxqcQxFkzyGlrQ7yHfJx3QeXpxHX2zVuprPNQTsg/aMl ZHVPGGPZIdwAPmcn9CgtfoaugsNyt1NXQNhdX/jqRr4z8GX7i1/PPPmEC2e1WrR2rYjVVznV95h8 AF/zSyNduJHoOeyDV9T3g9LL5fJpYDVtv84moGtAwJzgOjd5Y+LOUGLtvTOzWyqtdPf9V1dHU3SU yOtjKgRw1E7u4a0H1IGDx+aDu9noIbVQw0dFGY6eJu1rfIIPcfInCDWOqcvh9NNSkAkiikxj/VKD ZbE3w7NQN5AEDOOP4R6IMgAXuJacBB6GHb39EFgORlBKAQCAQU1f/ssv+qUGldH2xM0Sx7BzLPK9 313Y/ogzF/1bY9PtzdrhDTuxu2E5dj6Dt90Hq0zqC2aktcVxstVHV0UudsjDxkdxjuD9UFwvdEb8 6zh7vxohE23HG0k+f2QZMjBwgEAgdwGwcIEQQeyDnvXt+7pRqCJp+KaFsAHu97Wj+aDfKNgjp4mN ADWsaAAOwwEF47fdBW+UNODkn2Qc31t1esOm7uy1QRVt3u7m80duYJXs57Hng+wyfog2HQGrYtV0 tY/9l3O1VVLII5qW4xeHIMjIcOSCDzyPRBtaCWfMEFqBXEA8jKCs9ygEAgEEEgd0FeT6oKpWtDXO AG48ZQc7l6j292o6u1R0VzqI6SQQVFZBTF0ETz5Egn+SDcydoHPkgR7QGngY80Gvaj0+bvXW2thr amjq6GbxWPicdrhjlrm9nA+6DTepbGs6haGldk/5w5hBJ9Wny+vmg3S82eyX+OGmu1NSVbaaTxms lAdseM4I9DgoOD3qI6t/tH0tIx4EdoLfhAyGhoaePTkn9EH0kzDWtIdy44QWBr/E9soNV6ucdOdQ eJt8E0jg8EZ47H9EG22toio4Y42YjZG1rRntwg9zN3O1B6OwGUFrRgIJQCAQCBJRlhHqg5JfZr9o SV1t0zRx3Jl0nL6SF0oY+ncfnJzwWZ5Bzx6IMZYum19uM7X6ikp6ZkmHVT2v8WeU+bQ7s1vbsg63 Y7RR2S3xUVugbDTx8Na3zz5n1KDQ7Yw1fXC8VW93h0VCyDDTkbnYIB+weg6iDkAlBKAQGT6oBBBI 7FBznrc1s+nrPRB+01d6oYiM/M0ShxH5NQdDjIDee6BnuDW5JAHqUHD9a6hu3UDVk+i9EzS0lLTO abtdmPwGNB5ij9XHB/XyBQdH0Fomy6Otz4LTb2QTSOLpp3u8SaY5zl7zku7/AE9AOyDZ2RRxvc5j Gtc7AcQOTjsgsQCCQ45GSUD/AAu90FbiAfugUPaTgHn0QMgg9igrOTz3wghBXPzE5rXAOIwPZBzL pZNHboLnZ7m5kN7ZWSyysecGVriC14z3GAO3mEGU1pqWotdbb6Khp2zVtWSGeMSGADH08jnv6IPD 1N1XcNKaLmvFBbm3CoidG2SIE7WhxwXcAnAyg1W46l1n/df9rVkdvoaUxtePwoMr3l2Nobkn1HJC DT5JNZsvelH6mjjqaiaUzU5e5rC1xwdjgAPPCDa6uzQaZ1pWagq7ZPcvx0YeH0sbnmOcNHAH+EHG c480GmdOblb9Lap1jqTWLzR3iaQvgpJBiUh7shrGDOSfhHHl9EG46b1drM6ytLtR26Gis113CKAM y+mcOA1789ycHt6+nIdma4AAkhBqfV3L+mOpNp7UMp7ZxgZQbPZJjNaqKXP+kgY7PrloQZaAY3IL SMoGDueTwgsQCBWk55QMgWQhrCXHAHc+iDRdEZvV2ud/qgXEyupqXdyGRjuRn1KDeHFp+Ug/RBXI cAdu/mg5z0wmZU6j1dVfFl9aIcv7kNBOPtuH5oN8rr1bba+Blxr6SldO8RxCeZsfiO9G5PJ9ggyI IPYoJQCCMgHkoEeQXfDnCDmXVzw5dSdPqWbOyS9tkAHmWMc5B0xoBPKDRetOoq3TehaiotP/ALwn ljpadwGdr3u258ufuOUHv6ZaYi0tpG3UO7xKvb4tXP5zTu+d5Pnk/oAg2/I9QggPaTgOBPsUDIIL gBkkYQAIPYoLIyBnJQeO6Timoamc4/dxufz54BP9EGhdD5bhWaGpq+61tZW1FVUzTh87y4tYXuDW An/CAAR9kHRkEHsUCx+aBDwCfRB47nSS1NFURU9S6mmkaQyZrclh9cIOV3jpfe7xdIau4avnJp3h 0ToKRrJG4Odofk8e3ug3u+6eoL7Sx09zgbM2N25pI+Jp47EduyDWqvplZZoRAJ7h+FLtzoPxB2n2 55wg2uko4qeGOnhaGRRMDGt9ABgIMXfdN269z26auY4yUE4qIXMcR8Xv6oMq6PDRtHA5OMjP5IOW dcLNbbjYKWoqaNgq/wAbTxiojbiQNMgyA7uEHQvwNNUR08M0ZeyB7ZI9ziSHNxgoMuW4xygw2t6T 8Zoy+Uuf9LQzMz9WFB6NIzePpazyAYD6SFw+hYCg2CJxjz55QekdggBhx255QWjgIJQCAQYjVVVH S6euUkszYGtgeN7jgAlpwg5d0+1Pdquwx0em7bSCKBzmS1dbNtBd3JDfmQemv6kXew1dHHdaG13C KeQRyfsuqdJLFyQXeGQdwHBPI4z37IOrgCdgI4BGRkc8j/ig5JqDROsKO83R+jdTUVtoK+TxnMqK XxJY5MEEtcBwMD3QY2y9CKKsuDLrrm912oq4P8RofmKJpznG0EkjgcZA9uUHcYGhkTWNGA3gfRBY gECOb3OUCIOY9XqcnVXTurJPhw3prCPd0bgD+eEHT2jJQaH1ksVbd9HudamGe42+qiuFNB/zr4nb tnPrghBOk+pFhu9vjFVWQ2y5sZ/nNBXOEM0Dh3y12OM9iOEHj1T1i0hYWPjbdqaurhgMpaN3jSPc ezRt8+R+fmgjRN91Vqq6murbYyx2Rh+CmqmmSoqMjue2wefbz7IOmNGGgZzwg5X/AGiLpPRaAqaO 3TPjudc9sdOY3EPBadxII5GMD9UG+6XrhcNOWysa8SCopo5S8eZLQSfzygzJGMfRBjtQN3WK4Ad/ w8mP+qUGodDHPPS6x7gB+7I4GP8AEQg39AIEk8kCc+QygQMPibj+SCJWEkuz5IPO47RlBXMeAgof tAA80FZO3k+SDH6gucdtslbcJDhlNG6Q59hx+qDkOpqS4UvSWCruVXU1ldXV9PXGOpl3NgMj2kRs 8g0dgPUn2ADdqjqHo+nlmjm1La2SRPMb2mcZa4HGP0KB4uqWiWMIOpbaQBztlzjCDwVfVzQb6WSK TUdE9j2lpbh5BHoePNBqPTPrLpG06GtlJebvtq6VjoHNEMjjtY4hhHHYtDUG7WrrPoWvqIY4742J 8pxH+IhkiDj9XNwg6jT85cO2EDtjPi5yEF7RgIGQCAQc6qR/fPV8sJfmyWp7WvZn4Z5u+CPb+nug 2C46L0/dZhPX2qllnAA37cHt7YQei06ctFqz+zbdS03GMxxgHH17/qgy7TtABHmguPJJQI5gJz5o FIwUDSeSAD8DsgVxGRzyUFbpC07RjlBpHV6z1t10jm000lVcqKqp66njjc1pe+KQPwC7gcBBusM4 fTxuLXML2h214w4ZGcEeRCCyN7XZ5xhBhL5pWy34u/bNrt9cDjBnp2yEAe5BQTadLWSzySyWu02+ jklOXvgp2xucfctAygzUceHZHkg819uX7JtslYaSpq2x43RUzQ6QjzIbkZx6DlB883DW1LrLq9S1 NNb7xW221Uz4YqJtDIHPqJGkHcCMMIafPn0Qbp0yutwounl+tjYNt4sT5oGU8js4GwPjBPuCEFf+ VS41Fkhu9o0+6soaaMPuG2UxlmGbniMH5yMPGPXHqg3G/XqpGmW3aht8lfQVNMZJGxPxKxjmZBDT w7juMoNe/s/ajttx0FaqCGoH46niIfA8Fj2t3HnBxkcdxwg6qDkA4Iz6oJQJJ5IFbny4QCBXDLSP ZB5ZWOAAQavfNdaYs1ykt12usFLWMaHGORrhweRzjH6oMXUdS9FRxtlk1La2tJ2/6cE59MDlBgq/ rHptxMFlguV7nwcNoaV5Dj/rnDUGjdT9Ra9uGkri79iU1js79sZ/FSCWeUO8g1o4PbPdBuHUKkq4 +lVBTXZ0E1XBJR+M+EFsZLZmctB5Hb/+IMy/pboieR8ztM0LnvO5xLBkn+X6ILIemuh2vLRpW1F3 bmBpH6hB7KbQGkqN2Y9M2VrHEbsUcfI9M4QebQ+iaHTrLrTyU1FPBUXCWppwKYfuo34Ph9vI7voC Ag2Sr01Z62llp57ZRGKRpaf3Le35fX6INhpGiONrW8Ma0ADKD0HO3IP6oLA4cDlAOcG4z5oGHKCm ryIHbc7scYKDSOkzmfsatic3ZWMrpRUxu+Zrs4APn2GR90G+IKppGMxkgc8oNItPUGguetptNw0d x/FRNc4zljXQtx5Eh2QcZ4IQb40ggEHI9UEoIwPRAYygWRpLDtAyg5pfrr1AqbzVUmn9OUVNSxPx FcK6uD2yD18NnxD6E8e/ZBjYtIdRK+sEmoNdCmp8AugtNK2PJ/1ngnCDMUfTx7o3Gs1bqiplJyXf jvDbjOQNrQBwgdvT+QNcKTVuqInd9zq0SZP+00oPJ/dbX1sqmyWfWUFfCXZdBdqNp447SR7SO3mC gydv1fX0VfDR6uss9sc9zYm1kUjZqSR5OAN45YT5B4HfGe2Q3sYPbHognGECTNLoyAMny+qDXNI6 Ug04+7GKR05uNdJWSPeBn4sbWn12gYHZBi6jSlfR9Q4b5Z6inhttVGI7nTPYSZnMBEb247EA7Tn/ AAj6INtFvphTmBlPCyAggxiMBpB78IFbb6eltsdJFG1tNHGImxjsGgYxz5ING6a6cZb7a+3XO2Nb NQ1Lvw05aBujcS5uxw5wPNB0eMENw45PqgbzPpnhBBAPdBU9vx8jjCAAwgEEOaHdwg1+8aas933u uNtpaiR4wXyRgkj690Gvjpjo+JwcNP0J29stJH5ZQZygtlFboWQ2+lip4WfK2Ju0D8kHO/7QlTHT aCZ4hAidXU7HnOA1pfyfyz+SDH9QdQNvfRI322wS+BK6CRkeAXbWzt8uOTj9UGXd1Xs9JaKatrLd faUTcCGa3yCQHHngEY785QeKXrBbTKRa7DfbjKT2p6N5H5kABAM1V1Gvc5htOi2WuA8tqbpUjIH+ o0INRa/Xd06lP03Uajq3iGFktbNaqeGGOk3ty1uX5c/PGceqDsWkbNdrJWSQVl8qbvRSRbmuq2t8 SJ4cOAQBkEE8HthBucLmGP4iMe6C8YA+HkfVBIOecYQSTnugCXcZygPmwHHIQa5dtLOdd57rZrhU W24yMbG5zQJIpAO25hHJ8s5CDwvdr+Nhaz9gTHHDyyRufqN39UGi9S7HrKbRVe+/6khZC5zAYLbB 4JOXjjecnj+iDonT7S1s07YaeO3QYdNGySaV7i58jyAcuJ5PdBtbWhrQ1o4AwEE45QBGO6AQLJy3 HkUFJY0u3Ec+qCJdgGT8/kgGvaAMuGcIPJ+Lp6bc6pqYo2jze4NH5oFF7tR7XOi/++3/AHoHbLb6 0AiSnnYDu4cHDIQZCPbtyzseUDoBAIDsUAeUEOaHNIcMg90CNiYwYY0Ajsguc3tgHsgVAIIIyEFb +HADzQR5oEkcWkYGUAYwQOTwgjwm+6ClzGscWgcD1QaX1T0dDrbSdTY5al1L4rmyNmA3bXNORxxk INQ6o2eDTPQqW3U7w+G2Q0rRJtAc8RvZl3sTjOPVB02kcJKWN+GlpaPIen/BBcHBoPDefQBAQguk b225Hc480HP7BTMp+tWogSGuqLdTzNB4DtpLDj8kHSoPmJwMhBbsYXZcOPQILmP5DQAAgudhuPpl AMLXA8/qgc4PmgUD4kFhOTlBIA2kk8oNL6vwibp7dckgsax4xx2e1BmdHzfiNN2uQHIdTRnP+y1B nWAcHPKCD/pPugJPm+yBUFVQ4tYNrS8k8ADOf933QaRHcNfzAhtk0/SuacbnV8krSPUfu28fVAkt t15Wgme/WegDuHClo3SEfQvdg/kgx1f08lucpN81jfZy9uPDglbTNdjngNA/mg9Nu6UaSiDhUUD6 52cl1ZM6V36lBl29PNJNZt/u/biDjvCCg89T0z0rKd8FtFFODls1G8wvafUEINvt9P8AhaSODxZZ tgA3ynLncdyfVB6UBkD5s4QAPOQgCcnJQVuMgedoBYR8OBk590FxbhoPmgljRgFA6ClAIBAkjckO z2QKOSgHDBQQgEFEoJkOO6DzSNLhuIx5YQah1Us8l96d6gt9LGH1ElHIY2/xPDcgfmEGC6A3qbUP SuyzSvMk0EbqSVxOTujO1uTjk7A09/8AEg6DG0gbSPPOUFobxgd0Gm6jiFv17pq54IM5mt8rwe4c zczP+03+aDdo37cgDJPkgvHIBQWMaQ9hAyD3Pogvd8WPYYQQ1ob2QSex4JQU0tTHO79y+ORrXFhc x2QCMgj6jHZB7EEHgINb6jwip0ReYCM76Z5xj0GUFPSx7Z9D2ZzD8H4YADzGCR3Qbd4fugAzBByg lzdxzlBWgEFTs7jxx6oIQat1Fonz6dqaqn+GromGpgf2LZGfEMHvzjHpgkIMvp6tiudopK6DmOeJ r858yO32QZJA7W9jlBLnYPZANOUEuGQgljewQDhtJ9kFjBgZ9UDIBAIKywgeSCGtLuyCdh9kCkeR QRgegQGAe6CHNyOMIIc34fJBWSMbsIPP4W/Ls9kFPhHAzjsgpbSx04xTsjY0knAaByeSePdA212P icMeiBQR3yg1TqaCzTn45nEltqIaxrsfwvG7/sk/mg2unkY+OKVpBZI0PB89pAx/VB6WODhwDgeq Bsn1QX7xsB59EDteHj4QRhBo/VPWbNK6dlkpiH3SZjvwsWM5IGS7A8m4yg4r0km1xRV7LLY6ugiM tILpVSV8DpfGmlLnEEtcCO4HHrnlBvrNZXi4R2CapY62XGlvTrdcqOGQuieckDBI5aQMjPZBsPUG 5XCi1Xo2OjrJKeGeeQVEbHfDIMM4d3BGTlBr+ntQXLU/UfqBHJUvdp+3UwoIIR8gka0l7iM4Ltxc Nw8gAg2rouah+kYnyVHiUwc+KKLww3w9rznBHcHg+3ZB0VnyhBW/5igljgBygswPQIKnNIHKCECc FpICDz1UIqKWaJ4Ba9haQexyCOUGj9FJ3y6Hp4pDl1NLJTn1+F3/ABQb+zk/RBYgjA9EBjCCUAge MAjkIJc0k8YQeJzKs1rAx0P4b/FnO/7eSD3MBDQCcnHKCUCgHaQe6AYCM5QMgrc05J8kEBpPZAbH eiCEAMefZBV4e0bR8Q9SgAzA4GECPZvxz2QeYjPdAkjN5PpjhBSyFzcjGfRB4NS0H7R01cqN2f39 PKwY75LCB+qDF9Mat100JZ6iZzTL4Phv/wBZpLT/ACQbeGDaAwkn0QDcNf8AEgZ4LuW/KgUO2xOO SOfJBwGgtV31vZdR6svNFV09W6Oamt9BLGWvjja7BBZxh20fmSUHuhrYdFVdpvlU176SqsbIAdpw Z2AFsf8ArHH6IPBcxcLD03o79V0sr7nV3J1zdE7yftcWtd6IPO653X+6lhu8L6nUdbbJ3PqBE0Pe 0vblo4PIyPU4GEG8dFdM1Ni0jLHdGkXC4bpqoEc735LhnvnLj9sIM10WkDNM1lK8Br6a4VERb5jD 0HRQHY4zj6oDa70QMxuByEDIFk+X7oK0CkgAhBWg550fYaVmpKEgg090l4JzgOOR/NB0QcdkFjfl CCUAgEEtxnnsgsbgjhBKAwM9kAgECsJI5QMSB3QCAIyMFAAAdkAgR7cYwECIBAjyQcIEQJI0FvkE FGOTjlAIFe0FhaeyDSel+aalvlvzgUl2qIwz+EOcH4+nxlBvTTtBI+ZBByeT5oLWA+ERjlBEeGgh /H1QVmNjB+6GMgjv9T/UlBq3T7UbdWWeeeromQPjqHwSR53MJaTgjP8AVBtkkUT4HMeAYz3DuQgx lBaLbQxyMo6Slga524tjiDQT64A7oPdSxhrsYDR6AIOY6OuZs3V7UumZGkCucbpB6bS1pd+pQdcF VG0EOcMgkDnuggVsAkw+VjM9g44QLWVEkW18W0xBwEhccbRg5I9T244+qD1PJGMIKvFDsjcDgoAn 4chBWc9ygqlkDRwcFBz3QIkg1zrSnJcHGoilAI7gtP8AuQdGbnAz3QOHYb7oI3H1QG5xQOOwQSgs j+X7oGQCAQCCvdtAwgV7+24gILWkYHPkglApcQ7CBkAgqk4eMeaCECloJQK8bW5HdBRvc5rgR5IK 2tcGuL8DPA+iBXHAygOecd0GiaQaKTX2t6Rg275qasDc8fHCGn/9aDfQ0lAOJOB6ccIL4zubygSc ZIQICcbSOMHn7IOadDXg2W8tA+JtxlaR5jDj3/JBv93uP7NtVTUmmqKrwW7vBp498j/oEGkO6ive P3OlNRDnGH0RaR9iQg8/98NX1xc206NrIzgEPrJmRgfUZzn2QeQ23qXcqoVMkun7W/BaHeGZ5GA9 wDtGc+xQZWg6dXKua9uqNV3mrMnLmUkn4aP8hk/qgyUHSjS8TXeNDX1UhGN9RXzOP5bgP0QbLpLT sFgsxt8U9TUQ+K+QfiJTJt3HO0ZyQ0eQQZuU4wg4/qbqLXUHVCSwWtsE9HTWuSqqzI0ksmydgDh9 gR/JBsHTfXrdVeNRVMdPHdKZjXyinlEsUjT2exw8sgjHkgx/WnVr9K01gqcVfgPr2iU00Zedoa4l pA9eECaR6gVurLhEKLTNyp7d2fU1bPD49QD9vVB6NPbGdYdTQ4GXUVNL9fm5QdCaPh57jhAwAI5P KBtg90EgYQSgdrARnlAzRgcIJQCAQCClBVJEXTMkEjmhrXN24GDnHPrxj6c854QXxDBwOwCCxAIB AIBArmZOcoEcNpwghBW5uB3QVTfIgqaAWnjkIEPYoNBpy2l623NvibRX2iF/h+8cjxkfZyDoLnfA G47eaCGZ3DBwUHpDdowgEFc5LXgAZOD/ACQcw6E4MGpXDjNzl499xyg6PWuLCXBvAGT7oMZS3Ogr zJ+Eq6apMTtj/AeHBh9D7oMlC+PJB2j7oK6y9W2gb/nldTQY/wCckAQatceq2n6MPjojNcZc4DaZ hcCfTOEGLPUPVFdJ/wCidB3F0J+V9Q7wwRjvyOMoNj0XrKsulzls97sk9qusUAqXNc8Piewnblrh 558kGV1xqGn03pivu1UQG00L3tZnG9w7NHuTgfdB8z2NlfGNVXm7fDday2fiHguz4Ye7j8tzj98+ SD1aBrG2CgvGodNUsDqO2UTKONzs+HVyue0vJI8u+CgjVnVS66ov1rtFq0+2Srpbix8EzpP3Mp8P sfcEn6gBB33QUGpGWknVstE6pc7LW0se0RjHY84zlBhbbui63XgPGTJaYHA9s/G4IOhA5APqgdre xygdAIJaNxwgtaMDCAQCAQCAQeUtOPJA4OUDMODygcPBOOUDIBArGkHlAyAQQ4DB48kFSBX9kFMj S5uAgqMbgCchAmM8IOVapm/A9c9GS7g1tZQVVOQfPGHDCDquMENyCUEkbTj0QWA4btPcoHjaWg5O UGva31FHpqloKiaB0zKirZTOIdjYHA/ET7Y/VByvpbqq36f1Jc9Oz7pLnWXiZjYmYO1u553Efkg7 jUNL4s57+aDmU3Se1U9wmrLDV11llncXyiikwx7v4i055/3oHPTV0zv8+1Nd6huewkazj8igW6dP tP6e0/cbt+FfVT00D5GuqZDJkgEjIPflBmejM89foi2V9dS0sFXOxzniniDBjc7HA+gQdBawGNwA HOUGNprNDBeKm5AbqmdjI3Fx4Ab5Dj6IMFrvRlv1PLbHXR07mUkrpGRNkIY8kAEPHmOyDxXfRdBW X2Svk3fHSClkhH+jkbz3H0OEHspNHWiPSzrJHRQst0kfhuhaMDHYfyQa7SdLLbT6qhuLZCKam8GS mpmjHgyMG3OfMEEoOkMbtGO4Qc/uoFv6zWadxw24WySlzngujcCB/wBtB0NsZDQOOBhA+PhwgGjA QMgZvw8nsUFgORlAIBAIBAIPO35TlANx5IIYTnugsacOBKCzcPVAFwHdBKAQCAPYoKiCO6BCWnug Q+fogU4IwgpmAa8YHdByHquQ3qf0wkLcEV8se72LMYQdae0EhzeDj80DF+W/E3B9UFkbm4G7l3kg tQYTWOn6TU9intdfHvgl5yDhzHDlrmkeYcAftjzQc56cdK7raNdVOqNXXOluVwMApoHwReHgAYLn D1IH80HX5QPDwMYHkEGMlpi+ohmHD2ZBJORtPt68IPTsb6INW6y1poumF8ezLSYBGDn+Igf1QZHp hRtotCWSHw/Dc2ladvpnn+qDbYyAMeeUDoPPUtD3sB/w90FbmgDJHBQEeOzPJBDwN2SPiQWMaCzJ 8u6DnfWVv4O12y/RACW01sc24nsx3wu/8P5IOg0sjZqaKRjtzXtDg71BCC5AIBAzOTg9kFgGBgIB AIBAIBB5MkcDsgBnyQSzh3PCB8j1QS3uEDSHJ4QWZHqEAgTcTIWjs3ugdAkvkgpc3DTjOUCeXKCc 4aBx9UCuLRy4gYQce6uuA6g9Mnk//M5T7H4EHWGu2enogkAvdgYyUFwZkgnuEFmMoDGEBg+hQTt+ H3QLt/6P6IIcwHGRhBzzr62V3S+5iEZO6PPGeNwQbnpQMGnrc2I7mfh2Bh/iAaMH8kGaY3zOcoHQ VYdknHP0QK7y+qA2hriQgxV/u8dnpxPURTugL9r5I4XSCMerg0E498Y9SEHjoNZadrXeFS362SSO /wCT/EsD/T5c5BQXakt1JfLNW26q2yQVEbonAYOAR3+qDVtDasorbpejpdUXKjttfRbqWZlXMyIn YcBwJPxAgZyPVB7p+qeh4pmxf3stEj3fKIahsv8A3SUGXt+sdOVzXGmv1slIOC0VLA5pPYEZyEGf BDgCCCD6ILWAdwecIGQCAQCAQCDygZBKCY/NAFmXZygkNwc5QMgEEtG44QWjgAII2gEkdz3QSghz d2OUFSCtwxygSQ/B3xj0CDjPUnUd8pNYQ2q61n7C0tUsHhXamjJLpMcxvf2YSSeTxwg1HqvTUVh0 GblZLvRXFtPPHU09TUVm+pbUBww+J3IPHduB3PJ8g2vSXXjTF0tMlff7lRWoOl2RUh3PlYAO7gG5 5z5DH1QdP0pfLfqO2x3KzVUdXQSEiOaM8HHBB8wQfI4QZwclA7RhAOGUEjgIJQCBXDKDWuoVpffN GXa3RML5JoHBrR3LgMgfmAg8nSuslm0jbYqpj46qmjEEsT2FpY5o2459ufuEG67zkDhA6AQVubtG coI2/DnKBCM+eEGEu+k7HeC83S10VUX53GSFrs59coNQPRLQMkpe7T9Lz2aBgD8kGStfSbRFrkMl Dp2gZIf8bmbz+uUG1U9mt1NEI4aGlY0ekLR/IIGktVFIcupKbP8A9Jv+5BkGxBowDgegGEDNbtOc oGQCAQCAQCDzs7IGQK1pBQMgEAgsY0g8oGQCCuSIvka7JG3yz/5ygsQCCt7SOfdAjuyDmvV246nh hp6DS2koL8axpbJLUyM8GnPl4jDyR55yO3dByLT39miovFRUXLWt0hop55N/4S0Qsaxg9ASNo+zf uSg6pZehGg7VBsjssVU8/wDKVh8Zw+x4/RBvunbBb9PUEdDaKOno6Rhc5sUEYY3J5JwPNBl0AgEE l2WgYQG07c+SCEGK1RaJrxaZqOnuFRbp3t/d1dM7bJE7III8j25B4KDm40Z1SpGBtP1Co65gwAKu 0hn3y1x5Qeilpuq1vbKZJtL3X+EFs9MfcZG4H8kGd0hW63kuXh6ntNlp6f8Ajp690kgOf4fDAxj3 CDfkAgEAgR7TklAiAQCBmtPBQWIBAIBAIBAIBAIPJk+qBmHOUDoEBO/ugdAIHjJJ5KCZDgcIJZ8o QSgEAgWT5fugrQI5jSMloJHbhBEYHPAQE5LYnEcEA/yQLTvdLSxvdw5zQThBY0bQRknBxkoGQCAQ GTjGeEAgCSe5QGcjB7IKqiJksMjHjhzSDjg/mgup2NbE3A8h358kFqAQCCpxOTyUEZPqUAgEAgMn 1KCcn1KC1AIBAIBAIBAIP//Z ------=_Part_3633935_947996224.1552408406386--