Consider the semicircle r(t) = a cos(t)i + a sin(t)j with 0 0. For a given vector field F, the flux across r(t) is (F N) d: (a) ds = Σ dt (b) N = Σ If our vector field is F1 = 9xi 6yj, then we have the flux being (F1 N)ds. (c) F1(r(t)) Σ (d) As such, (F1 N) ds = Σ Now, if our vector field is F2 = 5xi + 3(x - y)j, then we have the flux being| (F2 N)ds.

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
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Consider the semicircle r(t)
a cos(t)i + a sin(t)j with 0<t<r and a > 0. For a given vector field F, the flux across r(t) is
(F N) ds.
(a) ds =
Σ dt.
(b) N =
Σ
If our vector field is F1 = 9xi – 6yj, then we have the flux being
(F1 N)ds.
(c) F1(r(t))
Σ
(d) As such,
F1 N) ds =
Σ
Now, if our vector field is F2 = 5xi + 3( – y)j, then we have the flux being
(F2 N)ds.
(e) F2(r(t))
Σ
!!
(f) As such,
(F2 N) ds =
Σ
Transcribed Image Text:Consider the semicircle r(t) a cos(t)i + a sin(t)j with 0<t<r and a > 0. For a given vector field F, the flux across r(t) is (F N) ds. (a) ds = Σ dt. (b) N = Σ If our vector field is F1 = 9xi – 6yj, then we have the flux being (F1 N)ds. (c) F1(r(t)) Σ (d) As such, F1 N) ds = Σ Now, if our vector field is F2 = 5xi + 3( – y)j, then we have the flux being (F2 N)ds. (e) F2(r(t)) Σ !! (f) As such, (F2 N) ds = Σ
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