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∫ v•n dA .
∫ dq
∫ dq
−q q
− − − = ) cos cos sin tan cos 1
− q q − q q q − q
− 6xy − y , where V has
∑ ∫ Problem Solving 1: Line Integrals and Surface Integrals A. Line Integrals
∑ Calculation of the Vortex Pinning Energy in a Long Periodically
∆V, we can calculate C for a given pair of... From the definition of C = Q/
→ π A Precise Measurement of the π e ν Branching Ratio
Ω T L
Ω RESONANCE Project for Studies of Wave-Particle Interactions in the Inner Magnetosphere
⃗F = q ⃗v × ⃗B F = qvB sin (θ) F = (1.6 × 10 −19 C) (1.0
⁄ James “Scott” Groenier Merv Eriksson Sharon Kosmalski
′x =γ(x−vt) ′y = y ′z = z ′t =γ t − x =γ( ′x +v ′t ) y= ′y z= ′z t
•Final Exam (40% of grade) on Monday December 7 two
• ~e::i:~ I I I I I I ...
• ~:~::~:~ I I I I I ... I
• V)u + Vp = f V •u = 0 x G @ t > 0 x G С R3 (0о H) (0о V )ΠL2
• This week: parallel-plate capacitor • motion of charged particle and
• Position, Velocity, Acceleration • Significant Figures, Measurements, Errors
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