A small object with electric dipole moment p → is placed in a nonuniform electric field E → = E ( x ) i ^ . That is, the field is in the x direction, and its magnitude depends only on the coordinate x . Let θ represent the angle between the dipole moment and the x direction. Prove that the net force on the dipole is F = p ( d E d x ) cos θ acting in the direction of increasing field.
A small object with electric dipole moment p → is placed in a nonuniform electric field E → = E ( x ) i ^ . That is, the field is in the x direction, and its magnitude depends only on the coordinate x . Let θ represent the angle between the dipole moment and the x direction. Prove that the net force on the dipole is F = p ( d E d x ) cos θ acting in the direction of increasing field.
Solution Summary: The author explains that the net force on the dipole is F=p(dE)mathrmcostheta .
A small object with electric dipole moment
p
→
is placed in a nonuniform electric field
E
→
=
E
(
x
)
i
^
. That is, the field is in the x direction, and its magnitude depends only on the coordinate x. Let θ represent the angle between the dipole moment and the x direction. Prove that the net force on the dipole is
Part A
m
2πkT
) 3/2
Calculate the integral (v) = f vƒ (v)dv. The function f(v) describing the actual distribution of molecular speeds is called the Maxwell-Boltzmann distribution,
=
ƒ(v) = 4π (· v²e-mv²/2kT
. (Hint: Make the change of variable v² =x and use the tabulated integral foxne
integer and a is a positive constant.)
Express your answer in terms of the variables T, m, and appropriate constants.
-ax dx
n!
-
an+1
where n is a positive
(v)
=
ΕΠΙ ΑΣΦ
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