5. The motion of a mass attached to a dashpot and a spring as it experiences a force can be represented by dx d?x Fr = -kx Fg = -B- dt Fm = m dt2 As the net force (F) is equal to 1, the following differential equation can be written: FB + Fm + Fx = 1 d?x dx m dt2 -B- kx = 1 dt Where m = 1, B = 1 and k = 6, Solve the above differential equation using the Laplace Transform method at the following initial conditions, x(0) = 0, x'(0) = 0. %3!

Algebra: Structure And Method, Book 1
(REV)00th Edition
ISBN:9780395977224
Author:Richard G. Brown, Mary P. Dolciani, Robert H. Sorgenfrey, William L. Cole
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Chapter12: Quadratic Functions
Section12.8: Joint And Combined Variation
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5. The motion of a mass attached to a dashpot and a spring as it experiences a
force can be represented by
dx
d²x
Fm = m at?
Fr = -kx
FB = -B
dt
As the net force (F) is equal to 1, the following differential equation can be written:
Fg + Fm + Fr = 1
d?x
dx
B- kx = 1
m
dt2
dt
Where m = 1, B = 1 and k = 6,
Solve the above differential equation using the Laplace Transform method at the
following initial conditions, x(0) = 0, x'(0) = 0.
Transcribed Image Text:5. The motion of a mass attached to a dashpot and a spring as it experiences a force can be represented by dx d²x Fm = m at? Fr = -kx FB = -B dt As the net force (F) is equal to 1, the following differential equation can be written: Fg + Fm + Fr = 1 d?x dx B- kx = 1 m dt2 dt Where m = 1, B = 1 and k = 6, Solve the above differential equation using the Laplace Transform method at the following initial conditions, x(0) = 0, x'(0) = 0.
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