throbber
  
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`1
`
`
`UNITED STATES PATENT AND TRADEMARK OFFICE
`  
`
`    
`
`BEFORE THE PATENT TRIAL AND APPEAL BOARD
`         
`
` !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
`
`  
 

`IICRO MOTION,
`INC.,
`
` "#$#$%&"'

`Petitioner,
`
`IPR2014-00167
`!()!*)" %)  !
`
`IPR2014-0017O
` !
`
`
`
` 
`
`at 4:25 p.m.
`
`IPR2014-00178
`  !
`
` +
`,
`
`,
`
`
 
 !-
`INVENSYS SYSTEMS,
`INC.,
`IPR2014-00179
`
`-
`
`Patent Owner.
`Volume II
`  *#"&#.&"' +%/01"
`
` !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
`
`
`
` +$2"%3*1$&*#$%&%4   
` 

`Video Examination of MICHAEL D. SIDMAN,
`
`  
#*5"&*##"$&)#*&6"%4#" *#"&#.&"'
0&2"'
`Ph.D.,
`taken at the instance of the Patent Owner, under
`
` *&270')0*&##%
`8*98989*&2  
`and pursuant
`to 35 USC 316(a)(5)(A) and 37 C.F.R.
`
`  829
:"4%'";  
`  
*"<$)#"'"2
`42.53(d), before JENNIFER L. SCHMALING,
`a Registered
`
` "'$#"7%'#"'
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"'#$4$"2
`Ierit Reporter, Certified Realtime Reporter, Certified
`
` '%*26*)#*7#$%&"'*&2 %#*'= 0:/$6$&*&24%'#"
`Broadcast Captioner and Notary Public in and for the
`
`-
`#*#"%4>$)6%&)$&
*#%/"=?*'2&"'
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`State of Wisconsin, at Foley & Lardner, 777 East
`
` >$)6%&)$&("&0"
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>$)6%&)$&
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`isconsin Avenue, Milwaukee, Wisconsin, on
`
` 0<0)#

6%11"&6$&<*#-@* 1 *&26%&6/02$&<
`August 7, 2014, commencing at 9:07 a.m. and concluding
`
` *#@7 1
`
`
`
`
`
`
`
`U.S. LEGAL SUPPORT
`
` 
` 
`  
`Invensys Ex. 2022
`713-653-7100
`Micro Motion v Invensys |PR2014-00393
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`2
`
`
`A P P E A R A N C E S
`    
`
`
`
`,? 
:=
`FOLEY & LARDNER, by
`  ;, 
`
`

`IR.
`JEFFREY N. COSTAKOS,
`IS. KADIE M.
`JELENCHICK,
`
`   ;  

` *)#>$)6%&)$&("&0"

`777 East Wisconsin Avenue,
`$/.*05""
>$)6%&)$&

`Iilwaukee, Wisconsin 53202,
` *77"*'"2%&:"*/4%4#" "#$#$%&"'
`appeared on behalf of the Petitioner.
`  
:=
`DLA PIPER LLP, by
` ;
`   ]

`IR.
`JAMES M. HEINTZ,
` -'""2%1'$("

`0$#"

`11911 Freedom Drive, Suite 300,
`")#%&
+$'<$&$*-!

`Reston, Virginia 20190-5602,
` *77"*'"2%&:"*/4%4#" *#"&#.&"'
`appeared on behalf of the Patent Owner.
`-  
:=
`DLA PIPER LLP, by
` ;, ;
`

`IR.
`JEFFREY L.
`JOHNSON,
` %0$)$*&*

`0$#"

`1000 Louisiana, Suite 2800,
` %0)#%&
"3*)

`Houston, Texas 77002,
` *77"*'"2%&:"*/4%4#" *#"&#.&"'
`appeared on behalf of the Patent Owner.
`  
:=
`DLA PIPER LLP, by
` > 
` 
`

`IR. EDWARD H. SIKORSKI,
`  
`#'""#

`0$#"

`401 B Street, Suite 1700 ,
`
`*&$"<%
*/$4%'&$*-!-

`San Diego, California 92101-4297,
` *77"*'"2%&:"*/4%4#" *#"&#.&"'
`appeared on behalf of the Patent Owner.
`
`
`A L S O
`P R E S E N T
`
` 
` 
`
`
`
`' ;%&
`7%&%/#^
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` _____
`-   `
`
`
`John Sponholtz, CLVS, Videographer.
`
`3*1$&*#$%&@ *<"
`
` ='  "$&#^ 
`
`
`
`
`
`
`
`
`
`
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`MICHAEL D. SIDMAN, Ph. D.
`   
` 
  
`
`
`8/7/2014
`
`
`
` _____
`
`   `
`
`
`
`
`
`3$:$# 2"&#$4$"2@ *<"
`
`Declaration Of Dr. Michael Sidman In
` % -!"6/*'*#$%&4' $6*"/
`$21*& &
`
`Connection With IPR2014-00170 Which
` %&&"6#$%&>$# !>$6
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`Concerns U.S. Patent 6,311,136 ..........
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`o. 2030 - U.S. Patent No. 6,311,136 ...............
`*
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`*
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` _____
`
`goooqow
`
`3
`
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`Disposition Of Original Exhibits:
`
`- "#0'&"2% $7"'
`Returned To DLA Piper LLP
`
`_____
`
`10
`
`
`11
`
`
`12
`
`
`13
`
`
`14
`
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`20
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`24
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`25
`
`
`U. S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`4
`
`
`-@@
`
`
`
`TRANSCRIPT OF PROCEEDINGS
`
`   
`
`
`-@@
`
`
`
` +  @>"*'"%44$6$*//=%&
`THE VIDEOGRAPHER:
`We are officially on
`
`-@@
`
`
`
`#"'"6%'2*#-@* 1 %2*=a)2*#"$)
`the record at 9:07 a.m. Today's date is
`
`-@@
`
`
`
`0<0)##
 $)$)$)5 % 
+%/01" $&
`August 7th, 2014.
`This is Disk No. 1, Volume II in
`
`-@@
`
`
`
`#"2"7%)$#$%&%4' $6*"/
`$21*&
`the deposition of Dr. Michael Sidman.
`
`-@@
`
`
`
`$)2"7%)$#$%&$):"$&<#*5"&$&#"
`This deposition is being taken in the
`
`-@@
`
`
`
`1*##"'$6'%%#$%&
 &6%'7%'*#"2
 "#$#$%&"'

`matter Micro Motion,
`Incorporated, Petitioner,
`
`-@@
`
`
`
`("')0) *#"&#.&"' &("&)=)
`=)#"1)
 &6%'7%'*#"2
`versus Patent Owner Invensys Systems,
`Incorporated.
`
`-@@
`
`-
`
`$)1*##"'$)7"&2$&<:"4%'"#" *#"&#'$*/*&2
`This matter is pending before the Patent Trial and
`
`-@@
`
`
`
`77"*/ %*'2
&$#"2
`#*#") *#"&#*&2'*2"1*'5
`Appeal Board, United States Patent and Trademark
`
`-@@
`
`
`
`44$6"
*)") %  !-
!
!
`Office, Cases No.
`IPR2014-l69, 2014-170, 2014-178
`
`-@@
`
`
`
`*&2!- $)2"7%)$#$%&$):"$&<#*5"&*#
`and 2014-179.
`This deposition is being taken at
`
`-@@
`
`
`
`#"%44$6")%4%/"=?*'2&"'/%6*#"2*#*)#
`the offices of Foley & Lardner located at 777 East
`
`-@@
`
`
`
`>$)6%&)$&("&0"
$/.*05""
>$)6%&)$&
`Wisconsin Avenue, Milwaukee, Wisconsin.
`
`-@@
`
`
`
`=&*1"$);%&
`7%&%/#^
($2"%<'*7"'
`My name is John Spohnholtz, videographer
`
`-@@
`
`
`
`4%'
` "<*/
*&2#"6%0'#'"7%'#"'$);"&&$4"'
`for U.S. Legal, and the court reporter is Jennifer
`
`-@@
`
`
`
`
`61*/$&< >$//6%0&)"/7/"*)")#*#"#"$'
`Schmaling. Will counsel please state their
`
`-@@
`
`
`
`*77"*'*&6")*&2.%1#"='"7'")"&#
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`appearances and whom they represent, beginning with
`
`-@@
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`-
`
`7"#$#$%&"'a)6%0&)"/ "&#"'"7%'#"'.$//)."*'
`petitioner‘s counsel.
`Then the reporter will swear
`
`-@@
`
`
`
`in the witness.
`$&#".$#&"))
`
`-@@
`
`
`
` 
`
`@;"44%)#*5%)
%/"=?
`MR. COSTAKOS:
`Jeff Costakos, Foley &
`
`-@@-
`
`
`
`*'2&"'
4%' "#$#$%&"'
$6'%%#$%&
*&24%'#"
`Lardner,
`for Petitioner, Micro Motion, and for the
`
`-@@
`
`
`
`witness.
`.$#&"))
`
`Invensys Systems.
`
`-@@
`
`
`
`   ]@;*1") "$&^4'%1 $7"'
`MR. HEINTZ:
`James Heinz from DLA Piper
`
`-@@
`
`
`
`4%' *#"&#.&"'
 &("&)=)
`=)#"1)
`for Patent Owner,
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`5
`
`
`-@@
`
`
`
`MR. SIKORSKI:
`Edward Sikorski of DLA
` 
` 
` @2.*'2
`$5%')5$%4
`
`-@@
`
`
`
` $7"'
*/)%4%' &("&)=)
`Piper, also for Invensys.
`
`-@@
`
`
`
` ;
` @&2;"44'"=;%&)%&

`MR.
`JOHNSON:
`And Jeffrey Johnson, DLA
`
`-@@
`
`
`
` $7"'
*/)%4%' &("&)=)
`=)#"1)
`Piper, also for Invensys Systems.
`
`    
` 
  
6*//"2*)*
`MICHAEL D. SIDMAN, Ph.D., called as a
`
` .$#&"))"'"$&
*($&<:""&4$')#20/=).%'&%&
`witness herein, having been first duly sworn on
`
` %*#
.*)"3*1$&"2*&2#")#$4$"2*)4%//%.)@
`oath, was examined and testified as follows:
`
`-@@
`
`
`
`EXAMINATION
``  
`
`-@@
`
`-
`
`BY MR. HEINTZ:
` ,   ]@
`
`-@@
`
`
`
`b%%21%'&$&<*<*$&
' 
`$21*&
`Good morning again, Dr. Sidman.
`
`-@@
`
`
`
`%%21%'&$&<
`Good morning.
`
`BY MR. HEINTZ:
`
`-@@
`
`
`
`b
`$'
*("=%0*2*&=)0:)#*&#$("6%&("')*#$%&)
`Sir, have you had any substantive conversations
`
`-@@-
`
`
`
`)$&6"."/"4##"'%%1=")#"'2*=*:%0##"
`since we left the room yesterday about
`the
`
`-@@
`
`
`
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`substance of this deposition?
`
`-@@
`
`
`
`No.
` %
`
`-@@
`
`
`
`b *("=%0%("'"*'2*&=6%&("')*#$%&)*:%0##"
`Have you overheard any conversations about
`the
`
`-@@
`
`
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`substance of this deposition?
`
`-@@
`
`
`
`No.
` %
`
`-@@
`
`-
`
`b5*= 
`$'
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`Okay. Sir,
`I'm going to ask you to turn to your
`
`-@-@
`
`
`
`"37"'#'"7%'#.$6*):""&1*'5"2*)3$:$#
`expert report which has been marked as Exhibit 2023
`
`-@-@
`
`
`
`7'"($%0)/=*&2$&7*'#$60/*'#%#0'&#%7*'*<'*7)
`previously and in particular to turn to paragraphs
`
`-@-@
`
`
`
`122 and 123.
`*&2
`
`-@-@
`
`
`
` 
`
`@$2=%0)*=ddc
`MR. COSTAKOS: Did you say "122"?
`
`-@-@
`
`
`
`   ]@ 2$2
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`MR. HEINTZ:
`I did, yes.
`
`-@-@
`
`
`
` ,   ]@
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`6
`
`
`
`
`b5*= 
`$'
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`Okay. Sir, would you agree that what you describe
`
`$&7*'*<'*7)*&2$)*)=&#")$)1%2"4%'
`in paragraphs 122 and 123 is a synthesis mode for
`
`<"&"'*#$&<#"2'$(")$<&*/)c
`generating the drive signals?
`
` 
`
`@:e"6#$%& %'1
`MR. COSTAKOS: Objection.
`Form.
`
` >  
`
`@
`%=%0*("&a#<$("&1"*
`THE WITNESS:
`So you haven't given me a
`
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`
`BY MR. HEINTZ:
` ,   ]@
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`b,%0)%0/2*("$#4'%1=")#"'2*=
`You should have it from yesterday.
`
`MR. COSTAKOS:
`I
`think it's in there.
` 
`
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`THE WITNESS:
`It's some place.
`
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` ,   ]@
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`b
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`2028, and they're in order,
`so it should be --
`
` 7'%:*:/=#%%5$#%0#%4%'2"' 5*= %#$# 
`I probably took it out of order. Okay. Got it.
`
`think that‘s a fair characterization.
`#$&5#*#a)*4*$'6*'*6#"'$^*#$%&
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`b5*=  )&a#$##'0"#*##"%&/=2$44"'"&6"
`Okay.
`Isn‘t it true that the only difference
`
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`between the wide band frequency sweep and the
`
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`the narrow frequency band
`
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`sweep referred to in paragraph 122 is the band of
`
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`$'

`frequencies used when driving the flowtube? Sir,
`
`1*= *)5=%0#%'"*2$&#%#"'"6%'2#"2%601"&#
`may I ask you to read into the record the document
`
`=%0a'"/%%5$&<*#'$<#&%.c
`you‘re looking at right now?
`
`MR. COSTAKOS:
`Read into the record?
` 
`
`@"*2$&#%#"'"6%'2c
`
`MR. HEINTZ: Yeah.
`   ]@,"*
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`MR. COSTAKOS:
`You mean the name of it?
` 
`
`@,%01"*&#"&*1"%4$#c
`
` ,   ]@
`
`25 BY MR. HEINTZ:
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`7
`
`
`0%
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`
`
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`b""3$:$#&01:"'
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`The exhibit number,
`the document you're looking at
`
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`right now.
`
`2024.
`
`
`b*&5=%0
`Thank you.
`
`5*= %0/2 *("#*#f0")#$%&%&"1%'"#$1"

`Okay. Could I have that question one more time,
`
`7/"*)"c
`please?
`
`8%//%.$&<f0")#$%&'"*2 9
`(Following question read.)
`
`
`
` b )&a#$##'0"#*##"%&/=
`Q
`Isn't it true that the only
`
`difference between the wide band
`- 2$44"'"&6":"#.""&#".$2":*&2
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`
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`band -- sorry,
`the narrow frequency
`
`12
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`band sweep referred to in paragraph
`
`13
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`122 is the band of frequencies used
`
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`when driving the flowtube?
`
` >  
`
`@>"//
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`THE WITNESS: Well, yes and no.
`No
`
`:"6*0)"#"6%170#"'
%'#"1$6'%7'%6"))%'

`because the computer, or the microprocessor,
`
`6%%)")"$#"'*.$2":*&2%'*&*''%.:*&2).""7
`chooses either a wide band or a narrow band sweep
`
`2"7"&2$&<%&#")$#0*#$%&$#7"'6"$(")$&#"
`depending on the situation it perceives in the
`
`4/%.#0:" 
`%#")$<&*/$)6%170#"2#.%2$44"'"&#
`flowtube.
`So the signal
`is computed two different
`
`.*=)2"7"&2$&<%&#"1%2"#*##"6%170#"'
`ways depending on the mode that the computer
`
`"17/%=)#%7"'4%'1#$))"*'6%')6*&%').""7
`employs to perform this search or scan or sweep.
`
`,"):"6*0)"#"!!#":*&2)*'":%#4'"f0"&6=
`Yes because the -- the bands are both frequency
`
`:*&2) &"$)"3#'*%'2$&*'$/=&*''%.
*&2%&"$)
`bands.
`One is extraordinarily narrow, and one is
`
`"3#'*%'2$&*'$/='")7"6#$("/=.$2"
`extraordinarily respectively wide.
`
`0%
`M6
`-@@
`
`
`
` ,   ]@
`
`25 BY MR. HEINTZ:
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`8
`
`
`-@@
`
`
`
`Is that it?
`b )#*#$#c
`
`-@@
`
`
`
`That‘s it.
`*#a)$#
`
`-@@
`
`
`
`b5*= 
`$'
."& *)5"2=%0*:%0#.*#=%0
`Okay. Sir, when I asked you about what you
`
`-@@
`
`
`
`2")6'$:"2$&7*'*<'*7%4=%0'"37"'#'"7%'#

`described in paragraph 122 of your expert report,
`
`-@@
`
`
`
`.=2$2=%04$&2$#&"6"))*'=#%/%%5*#3$:$#!!
`why did you find it necessary to look at Exhibit --
`
`-@@
`
`
`
`3$:$#
#" %*'2a)$&)#$#0#$%&2"6$)$%&4%'
`Exhibit 2024,
`the Board's institution decision for
`
`-@@
`
`
`
`#"a7*#"&#c
`the ‘854 patent?
`
`-@@
`
`
`
` 
`
`@;0)#4%'#"'"6%'2

`MR. COSTAKOS:
`Just for the record,
`I
`
`-@@
`
`-
`
`#$&5=%0)*$2d7*'*<'*7)*&2 d
`think you said "paragraphs 122 and 123."
`
`-@@
`
`
`
`BY MR. HEINTZ:
` ,   ]@
`
`-@@
`
`
`
`Q
`b5*=  *'*<'*7)*&2 >*#7'%17#"2=%0
`Okay.
`Paragraphs 122 and 123. What prompted you
`
`-@@
`
`
`
`to turn to the Board's institution decision to
`#%#0'&#%#" %*'2a)$&)#$#0#$%&2"6$)$%&#%
`
`-@@
`
`
`
`*&)."'#*#f0")#$%&c
`answer that question?
`
`-@@
`
`
`
`;0)##%'"4'")1=)"/4*:%0##"!!#"$))0")#*#
`Just to refresh myself about
`the -- the issues that
`
`-@@
`
`
`
`1*=:"6%&#'%("')$*/.$#'")7"6##%#*##%.*#
`may be controversial with respect
`to that to what
`I
`
`-@@
`
`
`
`)#*#"2$&#%)"7*'*<'*7))% 6%0/2<"#!!4%60)
`stated in those paragraphs so I could get -- focus
`
`-@@
`
`
`
`1=*&)."'1%'"2$'"6#/=#%.*# #%0<#=%01$<#
`my answer more directly to what
`I
`thought you might
`
`-@@
`
`
`
`:"#'=$&<#%<"#*#
`be trying to get at.
`
`-@@
`
`-
`
`b%")#"4*6##*##"$))0"1$<#:"6%&#'%("')$*/
`Does the fact that the issue might be controversial
`
`And
`
`
`-@@
`
`
`
`6*&<"=%0'*&)."'c
`change your answer?
`
`-@@
`
`
`
`No.
` %
`
`-@@
`
`
`
`b//'$<#  %.
$&'")7%&)"#%#"f0")#$%&*:%0#
`All right.
`Now,
`in response to the question about
`
`-@@
`
`
`
`what
`the difference was between the wide band
`.*##"2$44"'"&6".*):"#.""&#".$2":*&2
`
`-@@
`
`
`
`4'"f0"&6=).""7*&2#"&*''%.:*&24'"f0"&6=
`frequency sweep and the narrow band frequency
`
`-@@
`
`
`
`).""7
=%0<*("1"*d=")d*&2*d&%d*&)."' &2
`sweep, you gave me a "yes" and a "no" answer.
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`9
`-
`
`-@@
`
`
`
`#"d&%d7*'#*2#%2%
 #$&5
.$#.*##"!!
`the "no" part had to do,
`I
`think, with what
`the --
`
`-@@
`
`-@@
`
`-@@
`
`-@@
`
`-@@
`
`-@@
`
`-@@
`
`-@@-
`
`
`
`
`
`%.#"6%170#"'2"6$2"2.$61"#%2%4<"&"'*#$&<
`how the computer decided which method of generating
`
`
`
`#"2'$(")$<&*/#%0)"g$)#*#6%''"6#c
`the drive signal
`to use;
`is that correct?
`
`
`
`*#a)7*'#%4$#
`That‘s part of it.
`
`
`
`b5*= >*#a)#"%#"'7*'#c
`Okay. What's the other part?
`
`
`
`"%#"'7*'#$)$#)=&#")$^")*&"36$#*#$%&
`The other part is it synthesizes an excitation
`
`
`
`.*("4%'1$&#.%2$44"'"&#.*=)
`waveform in two different ways.
`
`
`
`b//'$<# &2$)&a#$##'0"#*##"%&/=
`All right.
`And isn't it true that the only
`
`-
`
`2$44"'"&6"$&#".*=)$&.$6#"2'$(")$<&*/$)
`difference in the ways in which the drive signal
`is
`
`
`
`)=&#")$^"2*)#%2%.$##"4'"f0"&6=:*&2)#*#
`synthesized has to do with the frequency bands that
`
`
`
`are used?
`*'"0)"2c
`
`band to sweep, and it sweeps a very narrow band
`
`-@@
`
`-@@
`
`-@@
`
`
`
` 
`
`@:e"6#$%& %'1
`MR. COSTAKOS: Objection.
`Form.
`
`-@@
`
`
`
` >  
`
`@"'"a)*/%#<%$&<%&
`THE WITNESS: There's a lot going on
`
`-@@
`
`
`
`.$#$&#"6%170#"'#%7"'4%'1#$).%/"7'%6"))
`within the computer to perform this whole process.
`
`-@@
`
`
`
` &$#$*//=
#"6%170#"'
%'#"7'%6"))%'
).""7)
`Initially,
`the computer, or the processor,
`sweeps
`
`-@@
`
`
`
`%("'*("'=.$2"'*&<"%44'"f0"&6$") >$/"$#a)
`over a very wide range of frequencies. While it's
`
`-@@
`
`
`
`2%$&<)%
$#a)#'=$&<#%2"#"'1$&"#"1*<&$#02"%4
`doing so,
`it‘s trying to determine the magnitude of
`
`-@@
`
`
`
`#"2$)7/*6"1"&#)$&#"($:'*#$&<#0:"0)$&<#"
`the displacements in the vibrating tube using the
`
`-@@
`
`-
`
`)#'*&<"<*#"!!)#'*$&<*0<")"&)%')  ##"&
`strange gate -- strain gauge sensors.
`It then
`
`-@@
`
`
`
`needs to make a determination as to how it
`&""2)#%1*5"*2"#"'1$&*#$%&*)#%%.$#
`
`-@@
`
`
`
`&*''%.)!!$#)0:)"f0"&#/=&*''%.)#")"*'6:*&2

`narrows -- it subsequently narrows the search band,
`
`-@@
`
`
`
`4%'"3*17/"
#"'*#"*#.$6#":*&2$)
`for example,
`the rate at which the band is
`
`-@@-
`
`
`
`&*''%."2  a1/%%5$&<"'"$&#"a-7*#"&#

`narrowed.
`I'm looking here in the '947 patent,
`
`-@@
`
`
`
`6%/01&
/$&"%')% "&$#2"6$2").*#
`column 13,
`line 12 or so.
`Then it decides what
`
`-@@
`
`
`
`:*&2#%).""7
*&2$#).""7)*("'=&*''%.:*&2
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`10
`
`
`-@@
`
`
`
`#"'"*4#"'  ##"&*)#%#'*656*&<")$&#"
`thereafter.
`It then has to track changes in the
`
`-@@
`
`
`
`'")%&*&#4'"f0"&6=%4#"($:'*#$&<#0:"
)%$#a)
`resonant frequency of the vibrating tube,
`so it's
`
`-@@
`
`
`
`&%#e0)#*1*##"'%4).$#6$&<:"#.""&*.$2"
`not just a matter of switching between a wide
`
`-@@
`
`
`
`4'"f0"&6=:*&2*&2*&*''%.4'"f0"&6=:*&2
`frequency band and a narrow frequency band.
`
`-@@
`
`
`
`BY MR. HEINTZ:
` ,   ]@
`
`-@@
`
`
`
`Q
`b5*= 
`$'
$&=%0'*&)."'
=%0'"4"''"2#%#"
`Okay. Sir,
`in your answer, you referred to the
`
`-@@
`
`
`
`'*#"*#.$6#":*&2$)&*''%."2#*#*77"*')$&
`rate at which the band is narrowed that appears in
`
`-@@
`
`
`
`#")"&#"&6")#*'#$&<*#/$&"%46%/01& %
`the sentence starting at
`line 12 of column 13.
`Do
`
`-@@-
`
`-
`
`=%0'"6*//#*#c
`you recall that?
`
`-@@-
`
`
`
`Yes.
`,")
`
`That‘s a very narrow band that the computer
`
`-@@
`
`
`
`b5*= *&=%0"37/*$&.*##"$//"'7*#"&#$)
`Okay.
`Can you explain what
`the Miller patent
`is
`
`-@@
`
`
`
`#*/5$&<*:%0#."&$#!!."&$#0)")#"#"'1!!
`talking about when it -- when it uses the term --
`
`-@@
`
`
`
` a1)%''=
#"7'*)"d#"'*#"*#.$6#":*&2
`I'm sorry,
`the phrase "the rate at which the band
`
`-@@
`
`
`
`is narrowed"?
`$)&*''%."2dc
`
`-@@
`
`
`
`>"//
$#)*=)$#a)*1*##"'%42")$<&6%$6"#%
`Well, it says it's a matter of design choice to
`
`-@@
`
`
`
`2"#"'1$&"#"'*#"*#.$6#":*&2$)&*''%."2

`determine the rate at which the band is narrowed,
`
`-@@
`
`
`
`1"*&$&<%.f0$65/=#"'*&<"%4)6*&&"2
`meaning how quickly the range of scanned
`
`-@@
`
`
`
`4'"f0"&6$")6*&:"&*''%."22%.&#%0/#$1*#"/=*
`frequencies can be narrowed down to ultimately a 20
`
`-@@
`
`-
`
`"'#^:*&26%("'$&<*77'%3$1*#"/="'#^%&"*6
`hertz band covering approximately 10 hertz on each
`
`-@@-
`
`
`
`)$2"%4#"40&2*1"&#*/4'"f0"&6=%4#")=)#"1
`side of the fundamental frequency of the system.
`
`-@@
`
`
`
`b5*= &2)%."&."#*/5*:%0##""'#^:*&2

`Okay.
`And so when we talk about
`the 20 hertz band,
`
`-@@-
`
`
`
`$)#*##".$2":*&24'"f0"&6=).""7%'#"&*''%.
`is that the wide band frequency sweep or the narrow
`
`-@@
`
`
`
`4'"f0"&6=:*&2).""7#*#=%0a'"'"4"''$&<#%$&
`frequency band sweep that you're referring to in
`
`-@@
`
`
`
`7*'*<'*7%4=%0'"6/*'*#$%&c
`paragraph 122 of your Declaration?
`
`-@@
`
`
`
`*#a)*("'=&*''%.:*&2#*##"6%170#"'
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`11
`
`
`-@@-
`
`
`
`0/#$1*#"/=
%7"40//=
*''$(")*#
`ultimately, hopefully, arrives at.
`
`-@@
`
`
`
`b
`%/"#1"*)5=%0#%"37/*$&*/$##/"1%'"*:%0#
`So let me ask you to explain a little more about
`
`-@@-
`
`
`
`%.#$).%'5) 
`%$&7*'*<'*7%4=%0'
`how this works.
`So in paragraph 122 of your
`
`-@@
`
`
`
`"6/*'*#$%&
=%0)#*#"
d$//"'2$)6/%)")d!! a1
`Declaration, you state, "Miller discloses" -
`I'm
`
`-@@
`
`
`
`)%''= %=%0*("$#c
`sorry.
`Do you have it?
`
`-@@
`
`
`
`Yeah.
`Go ahead.
`,"* %*"*2
`
`-@@
`
`
`
`b,%0)*=
d$//"'2$)6/%)")#.%1%2")%42'$("
`You say, "Miller discloses two modes of drive
`
`-@@-
`
`
`
`)$<&*/<"&"'*#$%&2'$($&<#"4/%.#0:"%)6$//*#$%&
`signal generation driving the flowtube oscillation
`
`-@@
`
`-
`
`.$#*.$2":*&24'"f0"&6=).""7
$&6/02$&<*'*&<"
`with a wide band frequency sweep,
`including a range
`
`-@@
`
`
`
`%44'"f0"&6$")'"7'")"&#$&<"17#=4/%.#0:"#%40//
`of frequencies representing empty flowtube to full
`
`-@@
`
`
`
`4/%.#0:"
."&#"4'"f0"&6=!!)%''=
."&#"
`flowtube, when the frequency -- sorry, when the
`
`-@@
`
`
`
`'")%&*&#4'"f0"&6=$)0&5&%.& d%=%0)""#*#c
`resonant frequency is unknown."
`Do you see that?
`
`-@@
`
`
`
`I do.
` 2%
`
`-@@
`
`
`
`b5*= 
`%2%")#*#1"*&#*##"4/%.#0:"$)
`Okay.
`So does that mean that the flowtube is
`
`-@@
`
`
`
`2'$("&*#2$44"'"&#4'"f0"&6$")#'%0<%0##$)
`driven at different frequencies throughout this
`
`-@@
`
`
`
`.$2"4'"f0"&6=:*&2).""7c
`wide frequency band sweep?
`
`-@@
`
`
`
` 
`
`@:e"6#$%& %'1
`MR. COSTAKOS: Objection.
`Form.
`
`-@@
`
`
`
` >  
`
`@>"//
20'$&<#").""7
#"
`THE WITNESS: Well, during the sweep,
`the
`
`-@@
`
`-
`
`4'"f0"&6=$)6%&)#*&#/=6*&<$&<
`frequency is constantly changing.
`
`-@@-
`
`
`
`BY MR. HEINTZ:
` ,   ]@
`
`-@@-
`
`
`
`Q
`b&2$)#"'"*'*#"*))%6$*#"2.$##*#6*&<"%4
`And is there a rate associated with that change of
`
`frequency sweep?
`
`-@@
`
`
`
`4'"f0"&6=c
`frequency?
`
`-@@
`
`
`
`Sure.
`
`0'"
`
`-@@
`
`
`
`b5*= >*#a)#")#*'#4'"f0"&6=%4#$).$2":*&2
`Okay. What's the start frequency of this wide band
`
`-@@
`
`
`
`4'"f0"&6=).""7c
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`12
`
`
`-@@-
`
`
`
`$//"'2$)6/%)")$&$)a-7*#"&##*##"
`Miller discloses in his '947 patent that the
`
`-@@
`
`
`
`$&$#$*/%'.$2").""7:*&2)7*&)#"'*&<"%4
`initial or wide sweep band spans the range of 2700
`
`-@@
`
`
`
`"'#^4%'/$f0$2.*#"'#%"'#^4%'*&
`hertz for liquid water to 4500 hertz for an
`
`-@@
`
`
`
`"(*60*#"2#0:" &2#*#a)'"4"'"&6$&<6%/01&

`evacuated tube.
`And that's referencing column 12,
`
`-@@
`
`
`
`line 55 and thereafter.
`/$&"*&2#"'"*4#"'
`
`-@@
`
`
`
`b5*= &2)%.%0/2$#:"4*$'#%6*//#")#*'#$&<
`Okay.
`And so would it be fair to call the starting
`
`-@@
`
`
`
`4'"f0"&6=*7*'*1"#"'c
`frequency a parameter?
`
`-@@
`
`
`
` 
`
`@:e"6#$%&#%4%'1
`MR. COSTAKOS: Objection to form.
`
`-@@
`
`-
`
` >  
`
`@>"//
 $1*<$&"#*#a)%&"
`THE WITNESS: Well,
`I
`imagine that's one
`
`-@@
`
`
`
`.*=#%6*'*6#"'$^"$#  %."("'
 2%&a#:"/$"("
`way to characterize it. However,
`I don't believe
`
`-@-@
`
`
`
`$//"'0)")#"#"'1d7*'*1"#"'d$&#"a-7*#"&#
`Miller uses the term "parameter" in the '947 patent
`
`-@-@
`
`
`
`0&/"))=%05&%.)%1"#$&< 2%&a#
`unless you know something I don't.
`
`-@-@
`
`
`
`BY MR. HEINTZ:
` ,   ]@
`
`-@-@
`
`
`
`b5*=
`Q
`Okay.
`
`It depends on how it's conducted --
`
`-@-@
`
`
`
` 2%&a#'"1"1:"')""$&<#*##"'1."&'"($".$&<
`I don't remember seeing that term when reviewing
`
`-@-@
`
`
`
`#"7*#"&#
`the patent.
`
`-@-@
`
`
`
`b %&"#"/"))
$#.%0/2:"*6%''"6##"'1#%0)"#%
`Nonetheless, it would be a correct term to use to
`
`-@-@
`
`
`
`6*'*6#"'$^"#*#f0*&#$#=
'$<#!!
`characterize that quantity, right --
`
`-@-@-
`
`-
`
`Well --
`>"//!!
`
`-@-@
`
`
`
`b!!)#*'#$&<4'"f0"&6=c
`-- starting frequency?
`
`-@-@
`
`
`
`>"//
#*#a)!!#*#a)=%0'6*'*6#"'$^*#$%&
`Well,
`that‘s -- that's your characterization.
`
`-@-@
`
`
`
`That‘s not Miller's characterization.
`*#a)&%#$//"'a)6*'*6#"'$^*#$%&
`
`-@-@
`
`
`
`b a1*)5$&<=%0$4#"6*'*6#"'$^*#$%&$)6%''"6#
`I'm asking you if the characterization is correct.
`
`-@-@-
`
`
`
` )$#$17'%7"'#%=%0#%0)"#*#6*'*6#"'$^*#$%&c
`Is it improper to you to use that characterization?
`
`-@-@
`
`
`
` #2"7"&2)%&%.$#a)6%&206#"2!!
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`13
`
`
`-@-@
`
`
`
`b// a1*)5$&<!!
`All I'm asking --
`
`-@-@
`
`
`
`!!$&#"6%170#"'7'%<'*1
`-- in the computer program.
`
`-@-@-
`
`
`
`b// a1*)5$&<=%04%'$)."#"'#")#*'#
`All I'm asking you for is whether the start
`
`-@-@
`
`
`
`4'"f0"&6=%4#$).$2":*&2).""7$)*7*'*1"#"'
`frequency of this wide band sweep is a parameter.
`
`-@-@
`
`
`
` #$&5$#!!"7"&2$&<%&%.#"6%170#"'1*=:"
`I
`think it -- Depending on how the computer may be
`
`-@-@
`
`
`
`7'%<'*11"2
=%06%0/2!!$#6%0/2%'!!%'$#
`programmed, you could -- it could or -- or it
`
`-@-@
`
`
`
`6%0/2&a#:"*7*'*1"#"'
`couldn‘t be a parameter.
`
`-@-@-
`
`
`
`b>=6*&a#$#!!
`Why can‘t it --
`
`-@@
`
`-
`
`So --
`
`%!!
`
`-@@
`
`
`
`b
`%''=
`Sorry.
`
`caveats you‘ve just applied to characterize the end
`
`-@@
`
`
`
`*#a)%5*= 
`%
4%'"3*17/"
$4#"$&$#$*/
`That‘s okay.
`So,
`for example,
`if the initial
`
`-@@
`
`
`
`4'"f0"&6=#*#=%06$#"2
"'#^
$)*'26%2"2
`frequency that you cited, 2700 hertz,
`is hard coded
`
`-@@
`
`
`
`$&#%#"7'%<'*1
 2%&a##$&5#*#.%0/2:"*
`into the program,
`I don't think that would be a
`
`-@@
`
`
`
`7*'*1"#"'  4$#.*))%1"#$&<#*#7"'*7)
`parameter.
`If it was something that perhaps
`
`-@@
`
`
`
`'")$2"2$&*#*:/"#*##"7'%<'*1*66"))"2

`resided in a table that the program accessed,
`I
`
`-@@
`
`
`
`)077%)"=%06%0/2#$&5%4$#*)*7*'*1"#"'
`suppose you could think of it as a parameter.
`
`-@@
`
`
`
` %."("'
#*#a)'"*2$&<$&:"#.""&#"/$&")
`However,
`that‘s reading in between the lines.
`
`-@@
`
`
`
`That‘s not what Miller discloses.
`He discloses
`*#a)&%#.*#$//"'2$)6/%)")  "2$)6/%)")
`
`-@@
`
`-
`
`.$2":*&2
*&$&$#$*/)"*'6
%' #$&5%4$#*)
`wide band, an initial search, or I
`think of it as
`
`-@@
`
`
`
`*&$&(")#$<*#$%&*&2#"&*&*''%.:*&2*&2#"&!!
`an investigation and then a narrow band and then --
`
`-@@-
`
`
`
`*&2#"&"(%/($&<$&#%*("'=&*''%.:*&2.$6$)
`and then evolving into a very narrow band which is
`
`-@@
`
`
`
`1%'"%4*#'*65$&<)$#0*#$%&#*#6%("')("'=)1*//
`more of a tracking situation that covers very small
`
`-@@
`
`
`
`6*&<")$&2"&)$#=
`changes in density.
`
`-@@
`
`
`
`b5*= 
`%.%0/2$#:"*/)%6%''"6#.$##")*1"
`Okay.
`So would it be also correct with the same
`
`-@@
`
`
`
`6*("*#)=%0a("e0)#*77/$"2#%6*'*6#"'$^"#""&2
`
`U.S. LEGAL SUPPORT
`
` 
` 
`713.653.7100
`  
`
`

`

`   
` 
  
`MICHAEL D. SIDMAN, Ph.D.
`
`
`8/7/2014
`
`14
`
`
`-@@
`
`
`
`4'"f0"&6=%4#".$2":*&2).""7*)*7*'*1"#"'c
`frequency of the wide band sweep as a parameter?
`
`-@@
`
`
`
` 
`
`@:e"6#$%& %'1
`MR. COSTAKOS: Objection.
`Form.
`
`-@@
`
`
`
`THE WITNESS:
`I would answer the
` >  
`
`@ .%0/2*&)."'#"!!#*#
`
`-@@
`
`
`
`f0")#$%&$&*)$1$/*'.*=
`question in a similar way.
`
`-@@
`
`
`
`BY MR. HEINTZ:
` ,   ]@
`
`have a software function that performs this sweep,
`
`-@@
`
`
`
`b5*= &2.*#*:%0##"'*#"*#.$6#").""7
`Q
`Okay.
`And what about
`the rate at which the sweep
`
`-@@
`
`
`
`$)6%&206#"2c )#*#*/)%*7*'*1"#"'c
`is conducted?
`Is that also a parameter?
`
`-@@
`
`
`
` 
`
`@:e"6#$%&#%4%'1
`MR. COSTAKOS: Objection to form.
`
`-@@
`
`-
`
`THE WITNESS: Miller didn't disclose that
` >  
`
`@$//"'2$2&a#2$)6/%)"#*#
`
`-@@
`
`
`
`*):"$&<*7*'*1"#"'"$#"'  %&"%4#%)"*'"
`as being a parameter either. None of those are
`
`-@@
`
`
`
`2")6'$:"2*):"$&<7*'*1"#"')
`described as being parameters.
`
`-@@
`
`
`
`BY MR. HEINTZ:
` ,   ]@
`
`-@@
`
`
`
`Q
`Would it be incorrect to characterize
`b>%0/2$#:"$&6%''"6##%6*'*6#"'$^"$#*)*
`
`-@@
`
`
`
`7*'*1"#"'c
`parameter?
`
`-@@
`
`
`
` 
`
`@:e"6#$%&#%4%'1
`MR. COSTAKOS: Objection to form.
`
`-@@
`
`
`
` >  
`
`@%6*'*6#"'$^"*&=%4
`THE WITNESS:
`To characterize any of
`
`-@@
`
`
`
`#%)"#'""#$&<)."e0)#2")6'$:"2
:"<$&&$&<
`those three things we just described, beginning
`
`-@@
`
`
`
`4'"f0"&6=
"&2$&<4'"f0"&6=*&2#"'*#"%4).""7

`frequency, ending frequency and the rate of sweep,
`
`-@@
`
`-
`
`I
`think reads an embodiment
`into the '947 that
` #$&5'"*2)*&"1:%2$1"&#$&#%#"a-#*#
`
`-@@-
`
`
`
`Miller doesn‘t disclose.
`And I
`think it narrows
`$//"'2%")

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