The magnetic field B due to a small current loop (which is placed at the origin) is called a magnetic dipole, Let p = (x² + y² +₂²) 1/2 For large, B P = curl(A), where ^= (-3.₂0) A $ Current loop (a) Let C be a horizontal circle of radius R with center (0, 0, c), and parameterization c(1) where c is large. O Which of the following correctly explains why A is tangent to C? =(-Rsi A(c(t)) = COS(1), 0) and c'(t)= (-R sin(t), R cos(1), 0) So, A(c(1)) = c(1). Therefore, A is parallel to c'() and tangent to C. A(c(t)) = R sin(1) R cos(1) A(c(t)) = ) = (-R So, A(c(1)) = -c'(1). Therefore, A is parallel to c'(t) and tangent to C. R sin(t) R cos(t) =(. and c'(t) = (R cos(t), -R sin(t), 0) 3 So, A(c(t)) c'(t) = 0. Therefore, A is perpendicular to c'(t) and tangent to C. R cos(1) R sin(1) and c'(1) = (R cos(1), - R sin(t), 0)
The magnetic field B due to a small current loop (which is placed at the origin) is called a magnetic dipole, Let p = (x² + y² +₂²) 1/2 For large, B P = curl(A), where ^= (-3.₂0) A $ Current loop (a) Let C be a horizontal circle of radius R with center (0, 0, c), and parameterization c(1) where c is large. O Which of the following correctly explains why A is tangent to C? =(-Rsi A(c(t)) = COS(1), 0) and c'(t)= (-R sin(t), R cos(1), 0) So, A(c(1)) = c(1). Therefore, A is parallel to c'() and tangent to C. A(c(t)) = R sin(1) R cos(1) A(c(t)) = ) = (-R So, A(c(1)) = -c'(1). Therefore, A is parallel to c'(t) and tangent to C. R sin(t) R cos(t) =(. and c'(t) = (R cos(t), -R sin(t), 0) 3 So, A(c(t)) c'(t) = 0. Therefore, A is perpendicular to c'(t) and tangent to C. R cos(1) R sin(1) and c'(1) = (R cos(1), - R sin(t), 0)
Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
Problem 1RQ
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