T h u r s da y m o r n i n g s G r a des K -5 Q 2 1 0 / 2 ... · G r a des K -5 Q 1 9 / 6 -1 0 / 4...

2
Thursday mornings 8-9 am! Grades K-5 Q1 9/6-10/4 Q2 10/25-12/20 Q3 1/10-3/21 Q4 4/11-6/6 Q1 $60, Q2 $96, Q3 $132, Q4 $108 Games Fitness Fun!

Transcript of T h u r s da y m o r n i n g s G r a des K -5 Q 2 1 0 / 2 ... · G r a des K -5 Q 1 9 / 6 -1 0 / 4...

Page 1: T h u r s da y m o r n i n g s G r a des K -5 Q 2 1 0 / 2 ... · G r a des K -5 Q 1 9 / 6 -1 0 / 4 Q 2 1 0 / 2 5 -1 2 / 2 0 Q 3 1 / 1 0 -3 / 2 1 Q 4 4 / 1 1 -6 / 6 Q 1 $ 6 0 , Q 2

Thursday mornings 

8-9 am!

Grades K-5

Q1 9/6-10/4

Q2 10/25-12/20

 Q3 1/10-3/21

Q4 4/11-6/6

 Q1 $60, Q2 $96, Q3

$132, Q4 $108

Games

Fitness

Fun!

Page 2: T h u r s da y m o r n i n g s G r a des K -5 Q 2 1 0 / 2 ... · G r a des K -5 Q 1 9 / 6 -1 0 / 4 Q 2 1 0 / 2 5 -1 2 / 2 0 Q 3 1 / 1 0 -3 / 2 1 Q 4 4 / 1 1 -6 / 6 Q 1 $ 6 0 , Q 2

Send this form back to school to sign up!

Child name: ___________________________________

Parent name: _________________________________

Parent email: _________________________________

Child's grade: _________________________________

Payment can be made online or by cash or

check made out to NapTown Fitness.

Scholarships are available- please reach out

to [email protected]. 


ANSWERS - IES MasterQ S 1 R a r Surface of sphere For Gaussian surface S 1 Q 0 enc E.ds 0 Q enclosed E 0 for 0 < r < R. For Gaussian surface S 2, enclosed Q E.ds Q 2 Q E 4 r

ANSWERS - IES MasterQ S 1 R a r Surface of sphere For Gaussian surface S 1 Q 0 enc E.ds 0 Q enclosed E 0 for 0 < r < R. For Gaussian surface S 2, enclosed Q E.ds Q 2 Q E 4 r

ELCT201: Digital Logic Design - German University …...Dr. Eng. Ahmed H. Madian 3 Flip-Flop Excitation Tables Q(t+1) 0 1 0 1 Q(t) 0 0 1 1 J 0 1 X X K X X 1 0 S 0 1 0 X R X 0 1 0 T

ELCT201: Digital Logic Design - German University …...Dr. Eng. Ahmed H. Madian 3 Flip-Flop Excitation Tables Q(t+1) 0 1 0 1 Q(t) 0 0 1 1 J 0 1 X X K X X 1 0 S 0 1 0 X R X 0 1 0 T

# *2p * ) - q $#c .*'0/$*) ) * 1 - 0(( -4

# *2p * ) - q $#c .*'0/$*) ) * 1 - 0(( -4

Q u e e r 1 0 1

Q u e e r 1 0 1

NFAtoDFAconversionandregularexpressionssiuon/csci3130-f17/slides/lec03.pdf · NFA: q 0 q 1 q 2 ",1 0 0 " Initialactivestates(beforereadinganyinput)? partial DFA: fq 0;q 1;q 2g 0 fq

NFAtoDFAconversionandregularexpressionssiuon/csci3130-f17/slides/lec03.pdf · NFA: q 0 q 1 q 2 ",1 0 0 " Initialactivestates(beforereadinganyinput)? partial DFA: fq 0;q 1;q 2g 0 fq

Registers and Shift Registers Discussion D8.2. D Flip-Flop 0 0 1 1 1 0 X 0 Q 0 ~Q 0 D CLK Q ~Q D gets latched to Q on the rising edge of the clock. Positive.

Registers and Shift Registers Discussion D8.2. D Flip-Flop 0 0 1 1 1 0 X 0 Q 0 ~Q 0 D CLK Q ~Q D gets latched to Q on the rising edge of the clock. Positive.

acuous, . logic, , miraculous. ardi)epacuit/papers/corelogic2.pdf · Structures Rea s o ning ab o ut co alitio ns April 29, 2 005 1 B ac kg r o und x = 0 x = 1 q 0 q 0 q 0 q 0 q 1

acuous, . logic, , miraculous. ardi)epacuit/papers/corelogic2.pdf · Structures Rea s o ning ab o ut co alitio ns April 29, 2 005 1 B ac kg r o und x = 0 x = 1 q 0 q 0 q 0 q 0 q 1

Equipotential and Electric Field Mapping1. Equipotential and Electric Field Mapping V = U q 2 V = 1 4ˇ 0 q 1 q 2 r 1 q 2 V = 1 4ˇ 0 q 1 r (1.5) Notice that the electric potential

Equipotential and Electric Field Mapping1. Equipotential and Electric Field Mapping V = U q 2 V = 1 4ˇ 0 q 1 q 2 r 1 q 2 V = 1 4ˇ 0 q 1 r (1.5) Notice that the electric potential

VOLUME 3 WINTER 2020 - TMA. Jan 2020 RSM Winter... · -4.0%-2.0% 0.0% 2.0% 4.0% 6.0% 8.0% 10.0% 12.0% Q 3 2 0 1 8 Q 4 2 0 1 8 Q 1 2 0 9 2 0 1 9 Q 3 2 0 1 9 Comp to-go Comp dine in

VOLUME 3 WINTER 2020 - TMA. Jan 2020 RSM Winter... · -4.0%-2.0% 0.0% 2.0% 4.0% 6.0% 8.0% 10.0% 12.0% Q 3 2 0 1 8 Q 4 2 0 1 8 Q 1 2 0 9 2 0 1 9 Q 3 2 0 1 9 Comp to-go Comp dine in

Q. 1 Q. 5 carry one mark each.gate.iitm.ac.in/gate2019/pdfs/QP/ME1_2019.pdf · Q.1 Consider the matrix P=[ 1 1 0 0 1 1 ... Q.9 For a hydrodynamically and thermally fully developed

Q. 1 Q. 5 carry one mark each.gate.iitm.ac.in/gate2019/pdfs/QP/ME1_2019.pdf · Q.1 Consider the matrix P=[ 1 1 0 0 1 1 ... Q.9 For a hydrodynamically and thermally fully developed

QDB:FromQuantumAlgorithmsTowardsCorrect QuantumPrograms · 2019-01-24 · Y.HuangandM.Martonosi 4:3 U q 0 q 1 C q 0 q 1 B A D = Figure1DecompositionofasimpleQCprogram.Timeflowslefttoright,showingsequencesof

QDB:FromQuantumAlgorithmsTowardsCorrect QuantumPrograms · 2019-01-24 · Y.HuangandM.Martonosi 4:3 U q 0 q 1 C q 0 q 1 B A D = Figure1DecompositionofasimpleQCprogram.Timeflowslefttoright,showingsequencesof

1 ON-OFF Privacy in the Presence of Correlation · 4 X 0 X 1 Q 1 = A Q 1 = B Q 1 = AB A A 0:25 0 0:75 A B 0 1 0 B A 1 0 0 B B 0 0:25 0:75 TABLE I: An example of our ON-OFF privacy

1 ON-OFF Privacy in the Presence of Correlation · 4 X 0 X 1 Q 1 = A Q 1 = B Q 1 = AB A A 0:25 0 0:75 A B 0 1 0 B A 1 0 0 B B 0 0:25 0:75 TABLE I: An example of our ON-OFF privacy

GA PCS Design Studies for ITER Include Analytic Ideal MHD ... · EXS/P6-37 D.Humphreys/IAEA FEC Kyoto/October 2016 q a » 1 q 0 20 - 0.5+ 2q 0 + 0.2sin(4p[q 0 - 0.5]) q 95 q 0 q 0

GA PCS Design Studies for ITER Include Analytic Ideal MHD ... · EXS/P6-37 D.Humphreys/IAEA FEC Kyoto/October 2016 q a » 1 q 0 20 - 0.5+ 2q 0 + 0.2sin(4p[q 0 - 0.5]) q 95 q 0 q 0

D:Documents and SettingsCamerataMis …q = 68 aprox q = 55 aprox 1 0 2 0 1 0 0 0 3 0 0 1 2 2 4 0 0 0 0 2 0 5 0 0 0 0 0 1 2 1 0 0 tm

D:Documents and SettingsCamerataMis …q = 68 aprox q = 55 aprox 1 0 2 0 1 0 0 0 3 0 0 1 2 2 4 0 0 0 0 2 0 5 0 0 0 0 0 1 2 1 0 0 tm

Q' - eFOTG-Document Locatorpg47... · 0..-t.., ~ '" ,-1 r-. ..~ ~ \Q .. Ooo~~~~~ ~ ,-1 \DO\N\DQ"'Q"'~ MNN~~QQo\o\ NNNNNNN~~ 0. 0 M 0. a-N an~r""'~~\Q""~ OOCl\alaI~~~~ …

Q' - eFOTG-Document Locatorpg47... · 0..-t.., ~ '" ,-1 r-. ..~ ~ \Q .. Ooo~~~~~ ~ ,-1 \DO\N\DQ"'Q"'~ MNN~~QQo\o\ NNNNNNN~~ 0. 0 M 0. a-N an~r""'~~\Q""~ OOCl\alaI~~~~ …

0 1 0 0 0 1 1 0 0 0 1 1 0 0 0 1 0 0 1 0 1 0 0 0 1 1 0 0 0 1 1 0 0 0 1 0 0 1 Q.

0 1 0 0 0 1 1 0 0 0 1 1 0 0 0 1 0 0 1 0 1 0 0 0 1 1 0 0 0 1 1 0 0 0 1 0 0 1 Q.

arXiv:1301.1025v1 [math.CA] 6 Jan 2013 · jjf jj ,q;K,X 0,X1 = (• 1 0 (t K(f,t,X 0,X1)) q dt t −1=q, q 0 t f K( ,t X 0,X1), q =1. We will call it just K-norm if

arXiv:1301.1025v1 [math.CA] 6 Jan 2013 · jjf jj ,q;K,X 0,X1 = (• 1 0 (t K(f,t,X 0,X1)) q dt t −1=q, q 0 t f K( ,t X 0,X1), q =1. We will call it just K-norm if

Evidence of a Strong Connection between Gamma-ray ......0528+13 Q 1 0 0 0827+24 Q 1 0 0 0836+71 Q 1 0 0 1127-14 Q 0 1 0 1156+29 Q 1 0 1 1222+21 Q 1 0 1 3C273 Q 4 1 1 3C279 Q 3 1 1

Evidence of a Strong Connection between Gamma-ray ......0528+13 Q 1 0 0 0827+24 Q 1 0 0 0836+71 Q 1 0 0 1127-14 Q 0 1 0 1156+29 Q 1 0 1 1222+21 Q 1 0 1 3C273 Q 4 1 1 3C279 Q 3 1 1

EFFICIENT MOLECULAR DYNAMICS: THERMOSTATS, BAROSTATS AND ...2017_uzh_cp2... · a(q →q 0) = min(1,e −β[V (q 0)−V (q )]) 1 High acceptance vs “making things happen”. 2 Curse

EFFICIENT MOLECULAR DYNAMICS: THERMOSTATS, BAROSTATS AND ...2017_uzh_cp2... · a(q →q 0) = min(1,e −β[V (q 0)−V (q )]) 1 High acceptance vs “making things happen”. 2 Curse

QDB:FromQuantumAlgorithmsTowardsCorrect QuantumProgramsyipenghuang.com/wp-content/uploads/2018/10/QDB__From_Quantum... · Y.HuangandM.MartonosiXX:3 U q 0 q 1 C q 0 q 1 B A D = Figure1DecompositionofasimpleQCprogram.Timeflowslefttoright,showingsequencesof

QDB:FromQuantumAlgorithmsTowardsCorrect QuantumProgramsyipenghuang.com/wp-content/uploads/2018/10/QDB__From_Quantum... · Y.HuangandM.MartonosiXX:3 U q 0 q 1 C q 0 q 1 B A D = Figure1DecompositionofasimpleQCprogram.Timeflowslefttoright,showingsequencesof