Cxg Ayi Ae T

Course Title ECON ECON1101;. U N I T E D S TAT E S S E C U R I T I E S A N D E X C H A N G E C O M M I S S I O N Was hi ngton, DC 549 F O R M 10Q (M ar k O ne ) ☒ Q UART E RLY RE P O RT P URS UANT TO S E CT I O N 13 O R 15 (d ) O F T H E S E CURI T I E S E XCH ANG E ACT O F 1934 F or the quar te r l y pe r i od e nde d Se pte mbe r 30,. Zdgh^Ya^ gXd_ `iarb^cVl^^, ^ hefr =dY ^gedarih shd, mhdWq dh`fqhr bc laiä c^XZVcciä gjfi edcVc^å Xd Pf^gh Gfi Z_ghX^å =d\r_ g^aq X \^c^ XfiäoYd defZaåh hd, X `V`d_ ghec^ Xåhd_ @ik iefVXaåh Yd \^crä dshdbi, dh gVbdYd cVmVaV bdYd gai\c^å, AYd efXdgheccqb imc^b Wqad imc^ d ^cqk åq`Vk.

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• Let’s consider V(t) to be a diraclike impulsion (not physical) at t=0 Then for t>0, V(t)=0 and the previous equation simplifies to • With solutions • Where the λare solutions of the characteristics polynomial is • The discriminant is • And the solutions are U(t) =Aeλt Beλ−t 2 2 0 2 0 2 U = dt dU dt d U ζ ω.

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()i t n i t n N n N n N n N n N n A e n B e n q t N q t q t q t Ω −Ω = 1 1 1 1 3 2 1 sin sin 3 sin 2 sin 1 π π π π M M, (7) where Ω =2~sinn 2()N 1 n ω π As we mentioned last time, these modes are essentially standing waves Let's see that this is the case by writing Eq. Zdgh^Ya^ gXd_ `iarb^cVl^^, ^ hefr =dY ^gedarih shd, mhdWq dh`fqhr bc laiä c^XZVcciä gjfi edcVc^å Xd Pf^gh Gfi Z_ghX^å =d\r_ g^aq X \^c^ XfiäoYd defZaåh hd, X `V`d_ ghec^ Xåhd_ @ik iefVXaåh Yd \^crä dshdbi, dh gVbdYd cVmVaV bdYd gai\c^å, AYd efXdgheccqb imc^b Wqad imc^ d ^cqk åq`Vk. E C X g 1 _ ɂ 1,050 T C Y F ^ e ~ R10cm ȓ @jpeg ` 300dpi C X g 5 _ 炲 w B l X ȃv Ɏg C X g W I.

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