Derive the constant A for a normalized one-dimensional Maxwellian. distribution f (u) = Aexp(-mu² /2KT) %3D such that f (u)du = 1
Derive the constant A for a normalized one-dimensional Maxwellian. distribution f (u) = Aexp(-mu² /2KT) %3D such that f (u)du = 1
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![a Derive the constant A for a normalized one-dimensional Maxwellian.
distribution
ĵ (u) = Aexp(-mu² /2KT)
such that
(u)du=
Hint: To save writing, replace (2KT/m)² by vh (Eq. 1.6)
1.2a. (Advanced problem). Find A for a two-dimensional distribution which inte-
grates to unity. Extra credit for a solution in cylindrical coordinates.
1/2
j (4, v) = Aexp[-m(u + v²)/2KT]
1.4 Debye Shielding
A fundamental characteristic of the behavior of plasma is its ability to shield out](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Fc462cb94-d566-400e-94ff-d9d61ca4b933%2F7ed183ec-5d32-46f8-bd28-561073e4237e%2F0bsqzao_processed.jpeg&w=3840&q=75)
Transcribed Image Text:a Derive the constant A for a normalized one-dimensional Maxwellian.
distribution
ĵ (u) = Aexp(-mu² /2KT)
such that
(u)du=
Hint: To save writing, replace (2KT/m)² by vh (Eq. 1.6)
1.2a. (Advanced problem). Find A for a two-dimensional distribution which inte-
grates to unity. Extra credit for a solution in cylindrical coordinates.
1/2
j (4, v) = Aexp[-m(u + v²)/2KT]
1.4 Debye Shielding
A fundamental characteristic of the behavior of plasma is its ability to shield out
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