(c) Find the complementary function (CF) and the particular integral (PI) of the differential equation (11). (d) Hence or otherwise, show that the general solution can be written as r(t) = L cosh wt + M sinh wt + sin wt (12) (e) Identify the initial conditions from the description in part (b) and use them to find L and M. Hence show that r(t) = a cosh wt + -) sinh ut - (13) sin wt 2w

Advanced Engineering Mathematics
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ISBN:9780470458365
Author:Erwin Kreyszig
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Chapter2: Second-order Linear Odes
Section: Chapter Questions
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Hello I have done A and B. Please help me solving C, D and E. Please also take 3 questions from me as well. But DON'T SOLVE a and b.

3. Rotating Tube
(a) In a Cartesian plane, if the position vector of a moving particle is given
by ř = rỉ + yj, then the r and y components of velocity is given by #
and # respectively. On the other hand, the polar components, i.e., the r
and ö components of velocity is given by and r. Using these, prove
that the r component of acceleration is
dr
de
f.
dt?
(10)
(b) A smooth straight thin tube revolves with uniform angular velocity w in
a vertical plane about one end which is fixed. A particle inside the tube is
sliding along the tube with a constant velocity v. At time t = 0, the tube
was horizontal and the particle was at a distance a from the fixed end.
Show that the motion of the particle can be described by the differential
equation
dr
- rw? = -g sin wt
(11)
dt?
[Hint: Use formula (10)|
(c) Find the complementary function (CF) and the particular integral (PI)
of the differential equation (11).
(d) Hence or otherwise, show that the general solution can be written as
r(t) = L cosh wt + M sinh wt +
sin wt
(12)
%3D
(e) Identify the initial conditions from the description in part (b) and use
them to find L and M. Hence show that
r(t) = a cosh wt + (-
sinh wt + sin wt
2w
(13)
Transcribed Image Text:3. Rotating Tube (a) In a Cartesian plane, if the position vector of a moving particle is given by ř = rỉ + yj, then the r and y components of velocity is given by # and # respectively. On the other hand, the polar components, i.e., the r and ö components of velocity is given by and r. Using these, prove that the r component of acceleration is dr de f. dt? (10) (b) A smooth straight thin tube revolves with uniform angular velocity w in a vertical plane about one end which is fixed. A particle inside the tube is sliding along the tube with a constant velocity v. At time t = 0, the tube was horizontal and the particle was at a distance a from the fixed end. Show that the motion of the particle can be described by the differential equation dr - rw? = -g sin wt (11) dt? [Hint: Use formula (10)| (c) Find the complementary function (CF) and the particular integral (PI) of the differential equation (11). (d) Hence or otherwise, show that the general solution can be written as r(t) = L cosh wt + M sinh wt + sin wt (12) %3D (e) Identify the initial conditions from the description in part (b) and use them to find L and M. Hence show that r(t) = a cosh wt + (- sinh wt + sin wt 2w (13)
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