ds = a Σ dt. N = Σ ector field is F1 = 10xi – 7yj, then we have the flux being / (F1 · N)ds. F,(r(t)) (10a(cost))i-(7a(sint))j Σ As such, / . (F1 · N) ds = (10(cos^2t))-(7a(sin^2t)) E our vector field is F2 = 3xi + 9(x – y)j, then we have the flux being (F2 · N)ds.
ds = a Σ dt. N = Σ ector field is F1 = 10xi – 7yj, then we have the flux being / (F1 · N)ds. F,(r(t)) (10a(cost))i-(7a(sint))j Σ As such, / . (F1 · N) ds = (10(cos^2t))-(7a(sin^2t)) E our vector field is F2 = 3xi + 9(x – y)j, then we have the flux being (F2 · N)ds.
Algebra & Trigonometry with Analytic Geometry
13th Edition
ISBN:9781133382119
Author:Swokowski
Publisher:Swokowski
Chapter6: The Trigonometric Functions
Section6.6: Additional Trigonometric Graphs
Problem 77E
Related questions
Question
![Consider the semicircle r(t)
= a cos(t)i + a sin(t)j with 0 <t < n and a > 0. For a given vector field F, the flux across r(t) is / (1
· N) ds.
(a) ds :
Σ dt.
a
(b) N =
<cost,sint>
Σ
If our vector field is F1 = 10xi – 7 yj, then we have the flux being
(F1 · N)ds.
(c) F1(r(t)) | (10a(cost))i-(7a(sint))j
Σ
o
(d) As such,
(F1 · N) ds = (10(cos^2t))-(7a(sin^2t)) E
Now, if our vector field is F2 = 3xi + 9(x - y)j, then we have the flux being
(F2 · N)ds.
(e) F2(r(t)) =
Σ
(f) As such,
(F2 · N) ds =
Σ](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F3d01a12a-1ab5-4b5b-8ac9-ffcff6df37dc%2Fae0610b5-a747-4a44-9fcd-ef153fe5e555%2Fhbafc6p_processed.png&w=3840&q=75)
Transcribed Image Text:Consider the semicircle r(t)
= a cos(t)i + a sin(t)j with 0 <t < n and a > 0. For a given vector field F, the flux across r(t) is / (1
· N) ds.
(a) ds :
Σ dt.
a
(b) N =
<cost,sint>
Σ
If our vector field is F1 = 10xi – 7 yj, then we have the flux being
(F1 · N)ds.
(c) F1(r(t)) | (10a(cost))i-(7a(sint))j
Σ
o
(d) As such,
(F1 · N) ds = (10(cos^2t))-(7a(sin^2t)) E
Now, if our vector field is F2 = 3xi + 9(x - 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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