G CXg ©Á±¢¢ 790110-Gc x gc fid
!l Z Z v $Ï M & T b 4D _ cÆ á Ý 8 \ G @0b Z v S \ < d 7o ¶0° _ > 8 Z Â Â º6ë è7F ¢ á G E \ b0v ºV %± r O I } _ ò È ° c K { ?C _ g A \ /6ä &0° Õ 6ä &08o >0>, ¥ ç ô>1 º>/>/ v>0>/ ¥>& ¥>' S>7 ì6ä '>&>6 ì6ä >' >1>, ¹#ã /*ñ9 7¼ w ¹#ã#ë>/>4 7Á0ð>>6>3>1>>4>0>>0>6>>2
Solved If F And G Are The Functions Whose Graphs Are Given Chegg Com
Gc x gc fid
Gc x gc fid-G^g g" µg _ h fÜ0°3ufåg f¸fÛfô%& \ xfÜ vg g g g 0É Â º Ü »g" p °føfçfï w ¸ F÷FúFá G GFúG FúFÔF¹FíFþFïG F¸GeG{GkG GDGyFþ Fþ7 FûFÿ ¶ Ç _ Fþ 1¤Fû5 !lG"*(FÔFï0ÛG /°C ZAxis ±30 m g /°C NOISE PERFORMANCE Noise Density X OUT and Y OUT 27 m g /√Hz Z OUT 43 m g /√Hz FREQUENCY RESPONSE 4 Bandwidth 5 No external filter X OUT and Y OUT 1300 Hz Z OUT 1000 Hz R FILT Sensor Resonant Frequency 165 kHz SELFTEST 6 Logic Input Low 06 V Logic Input High 24 V
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x for L, C, X, and B accuracies When Q x 01, multiply Acal by √1Q2 x for R and G accuracies Under an AC magnetic field, the following equation is applied to the measurement accuracy A x (1 B x (2 05 / Vs))_ Q b z m í µ N4 K Û í $ª b (5 &k 2 "© A ?0{ M 4E m l g ,"á* _ X 8 Z c ° D7H 0¿ E í
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Massachusetts Institute of technology Department of Physics 8022 Fall Final Formula sheet a GG Potential φ() a −φ(b) =− ∫E ds b ⋅ Energy of E The energy of an electrostatic configuration U = 1 1 2 2 ∫ V ρφdV = 8π∫ E dV0 1 2 3 4 5 6 7 8 9) 3 /;―26― ` h Í H µ c x j I b ¤ ?
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Is a function of class C 1 As x 1 we have G x n X s 0a s 1 x t s a a 1 1 x t 1 from MATH at Bocconi UniversityMeasures acceleration with a minimum fullscale range of ±3 g It can measure the static acceleration of gravity in tiltsensing applications, as well as dynamic acceleration resulting from motion, shock, or vibration The user selects the bandwidth of the accelerometer using the C X, C Y, and C Z capacitors at the X OUT, Y OUT, and Z¹ B>0>5 º Ø 1 3 3Æ º b&k _ Ã b ì b p 8 ?
S s w Ø C x, Ú É ´ ß Þ ´ á ç º w status è ´ µ » t, § É ç w Ý 6 xglobal status è ´ µ » t ¨ ò ^ Ú É ´ ß Þ ´ á ç x,status è ´ µ » w t , n V, f w » µ «/ Ë ï Å å U î æ D ó s Ô ù t xstall ô ø 0 t, î æ >A>g ó °>g x)>g & è W 0d (Ù \ 8 8 r M >' u G _ ~ >A>g ó °>g x)>g >& è W § î Å « \ 8 8 r M >' f j K r M '¨ ²>& 0d(Ù b( V í f>' \&k c 0d(Ù>& 9(ì µ s r M >' b ²4 j c M4 Î(Ù* b 1Y G \ ^ C f j c ë F M G \ @ 6 ~ r M G b _ c q5 Q b Ú b f j ² ó c@ @ @ X A H s _ @ s n n C d M X j ګo h F C H ѭn B M A O Ϧl ` R ǤH A Q K B ͡A iť o n A O Ӥ Q h ç { l ڡA A J Ӥ@ q A ڡH I } ̯ ۪ ǤH A @ Q ªo G j l f b A n G A ح^ T A O Ӧ~ ͡A G Q K p l C H F A o O ^ ơH d ӤW ~ ٿ P k k A ͯ ͡A F o A y W A W i N h S ೱ ѤF C M c O ~ o ٥աC H L
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• Constant Multiple Rule g(x)=c·f(x)theng0(x)=c·f0(x) • Power Rule f(x)=x n thenf 0 (x)=nx n−1 • Sum and Difference Rule h(x)=f(x)±g(x)thenh 0 (x)=f 0 (x)±g 0 (x)W>2ÛµÝ Ç# Ô¹Ý_>E % 8 æ W>40l4ð Ø N #b 0 8 þ 0l 4ð Ø 95% W>5 9 É ß º ¥ Ý 0 10 min 1 2 3 4 5 6 7 30 40 50 60B 8 F4* ô ¤ G x F ¥ G @ ¤ L } S @ 4 µ P  _ X ^ @ } ^ ?
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