How do you find the position function #x(t)# if you suppose that the mass in a mass-spring-dashpot system with #m=25#, #c=10# and #k=226# is set in motion with #x(0)=20# and #x'(0)=41#?

Answer 1

#x = (21.1062 cos(3t)+ 15.0737sin(3t))e^{-t/5}-1.10619#

In those considerations that follow, the positive axis is oriented from down-up for forces, velocities and displacements.

Supposing the mass #m# vertically placed over the spring-dashpot, the mass is actuated by
#f-m g = m ddot x#
where #f# is the force exerted by the spring-dashpot.

The spring-dashpot reacts according to

#-f = kx + c dot x#

Joining both equations we have

#m ddot x + c dot x + k x = -mg#

This is a linear non-homogeneous differential equation whose solution is given by

#x = x_h + x_p#
where #x_h# is the homogeneous solution
#m ddot x_h + c dot x_h + k x_h = 0#

and

#x_p# is a particular solution for
#m ddot x_p + c dot x_p + k x_p = -mg#
In this case #x_p = -(mg)/k#

The homogeneous equation has the general solution

#x_h = e^{lambda t}#

Substituting this generic solution we get at

#(m lambda^2+c lambda + k)e^{lambda t} = 0#
The feasible #lambda# are given by
#lambda=(-c pm sqrt(c^2-4mk))/(2m)#. For our case we have
#lambda = (-10 pm sqrt(100-4 xx 25 xx 226))/(50) = -1/5 pm 3i#

so

#x_h = e^{-t/5} e^{pm i 3 t} = e^{-t/5}(cos(3t)pm i sin(3t))#
when #lambda# is a complex conjugate pair, for each pair the solution proposal is as follows.
#x_h = (C_1 cos(3t)+ C_2sin(3t))e^{-t/5}#

(This can be demostrated but requires a lot of algebra.)

The general solution is given by

#x = (C_1 cos(3t)+ C_2sin(3t))e^{-t/5}-(m g)/k# The constants #C_1,C_2# are determined according to the movement initial conditions. So

#{(x(0) = C_1-(m g)/k = 20), (dot x(0) = -C_1/5+3C_2=41) :}#

From this system, we obtain the constants

#C_1 = (m g)/k + 20, C_2 = (m g)/(15k) + 15# assuming #g = 10# we have
#C_1 = 21.1062, C_2 = 15.0737#

So finally

#x = (21.1062 cos(3t)+ 15.0737sin(3t))e^{-t/5}-1.10619#
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Answer 2

To find the position function ( x(t) ) for the mass-spring-dashpot system, we first need to solve the second-order linear ordinary differential equation (ODE) governing the system's motion. The equation is given by:

[ m\frac{{d^2x}}{{dt^2}} + c\frac{{dx}}{{dt}} + kx = 0 ]

Given the values ( m = 25 ), ( c = 10 ), and ( k = 226 ), and the initial conditions ( x(0) = 20 ) and ( x'(0) = 41 ), we substitute these values into the differential equation.

The solution to this second-order ODE is a linear combination of exponential functions. The general form of the solution is:

[ x(t) = e^{rt} ]

where ( r ) is a constant.

To find ( r ), we substitute ( x(t) = e^{rt} ) into the differential equation:

[ m\frac{{d^2}}{{dt^2}}e^{rt} + c\frac{{d}}{{dt}}e^{rt} + ke^{rt} = 0 ]

After differentiation, we get:

[ m(r^2e^{rt}) + c(re^{rt}) + ke^{rt} = 0 ]

This simplifies to:

[ mr^2 + cr + k = 0 ]

Now, substitute the given values of ( m ), ( c ), and ( k ) into the equation:

[ 25r^2 + 10r + 226 = 0 ]

Solve this quadratic equation for ( r ). Once you have the values of ( r ), the solution for ( x(t) ) will be:

[ x(t) = Ae^{r_1t} + Be^{r_2t} ]

where ( A ) and ( B ) are constants determined by the initial conditions, and ( r_1 ) and ( r_2 ) are the roots of the quadratic equation obtained earlier.

Finally, use the initial conditions ( x(0) = 20 ) and ( x'(0) = 41 ) to solve for ( A ) and ( B ), and plug them back into the solution ( x(t) ).

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Answer 3

To find the position function ( x(t) ) for the mass-spring-dashpot system, you need to solve the second-order linear differential equation that governs the system. The equation is:

[ m\frac{d^2x}{dt^2} + c\frac{dx}{dt} + kx = 0 ]

Given ( m = 25 ), ( c = 10 ), and ( k = 226 ), and the initial conditions ( x(0) = 20 ) and ( x'(0) = 41 ), you can use these values to solve for ( x(t) ).

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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