Class Notes 1-5-2010: Difference between revisions

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:<math> x(t) = \sum^\infty_{n=1} \left[ b_n \sin \left( \left( \frac {2\pi n} {T} \right) t \right) \right] </math>
:<math> x(t) = \sum^\infty_{n=1} \left[ b_n \sin \left( \left( \frac {2\pi n} {T} \right) t \right) \right] </math>


1) Use vector analogy
:<math> x(t) \cdot \sin \left( \frac {2\pi mt} {T} \right) = \sum^\infty_{n=1} \left[ b_n \sin \left( \left( \frac {2\pi n} {T} \right) t \right) \cdot \sin \left( \frac {2\pi mt} {T} \right) \right] </math>
:<math> \int_{\frac {-T} {2}}^{\frac {T} {2}} x(t) \sin \left( \frac {2\pi mt} {T} \right) \,dt = v_m</math>





Revision as of 15:53, 17 January 2010

Subjects Covered

1) Linear Systems

2) Functions as Vectors


Functions graphed in vector form.


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Modeling functions as vectors. Using function approximations, the vector path is described.


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Function waves with varying periods based on the function x(t) = x(t+T)
vx=v→⋅i^
v^=vxi^+vyj^
v^=∑ivia^i
⟨vx,vy⟩
u^⋅v^=|u^||v^|cos⁡θ
x(t)=∑n=1∞[bnsin⁡((2πnT)t)]

1) Use vector analogy

x(t)⋅sin⁡(2πmtT)=∑n=1∞[bnsin⁡((2πnT)t)⋅sin⁡(2πmtT)]
∫−T2T2x(t)sin⁡(2πmtT)dt=vm


External Links

Authors

Colby Fullerton

Brian Roath