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Black_prince [1.1K]
3 years ago
12

A brick of mass 4 kg hangs from the end of a spring. When the brick is at rest, the spring is stretched by 3 cm. The spring is t

hen stretched an additional 2 cm and released. Assume there is no air resistance. Note that the acceleration due to gravity, g, is g = 980 cm/s2. Set up a differential equation with initial conditions describing the motion and solve it for the displacement s(t) of the mass from its equilibrium position (with the spring stretched 3 cm). s(t) = cm(Note that your answer should measure t in seconds and s in centimeters.)
Mathematics
2 answers:
Zielflug [23.3K]3 years ago
7 0

Answer:

Step-by-step explanation:

In this system we have the force of the spring and the gravitational force. The equation that describes that is

F_{s}+F{g}=ma\\k(y_0+y)-mg=ma

where y0 is the equilibrium position when the string is free and y0+y is the new equilibrium position when the object is hanged of the string. By replacing by derivatives we have

ky_0+ky-mg=ma\\mg+ky-mg=ky=ma\\\\ky=m\frac{d^2y}{dt^2}\\\\my''+ky=0

the solution for this differential equation is (by using the characterisic polynomial)

y(x)=Acos(kt)+Bsin(kt)\\k=\omega^2m

hope this helps!!

DanielleElmas [232]3 years ago
5 0

Answer:

A) d²x/dt² = -326.67x

At time t = 0,the spring is stretched to 5cm and and released.

Thus, the initial velocity is zero. Thus, the initial condition is;

x(0) = -5 and x'(0) = 0

B) The solution to the equation is;

x(t) = -5cos 18.07t

Step-by-step explanation:

A) Due to stretching, the force due to gravity and that due to stretching of spring will be the same. Thus;

mg = -kx

m = 4kg ; x = -3cm and g=980 cm/s²

Thus,

k = mg/x = 4x980/3 = 1306.67

The motion of mass attached to a spring is given as;

d²x/dt² = -ω²x

Where, ω² = k/m = 1306.67/4 = 326.67

Thus, the differential equation for the problem would be;

d²x/dt² = -326.67x

At time t = 0,the spring is stretched to 5cm and and released.

Thus, the initial velocity is zero. Thus, the initial condition is;

x(0) = -5 and x'(0) = 0

B) The general solution would be given by;

x(t) = C1cos ωt + C2sinωt

From earlier, ω² = 326.67

So, ω = √326.67 = 18.07

Thus,

x(t) = C1cos 18.07t + C2sin 18.07t

Now, applying initial conditions ;

At x(0) = -5;

-5 = C1cos 0 + C2sin 0

C1 = -5

x'(t) = -18.07C1Sin18.07t + 18.07C2Cos18.08t

Thus, at x'(0) = 0

0 = -18.07C1Sin 0 + 18.07C2Cos0

18.07C2 = 0

So,C2 = 0

Thus,the solution to the equation is;

x(t) = -5cos 18.07t

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For this problem we are going to use principles, concepts and calculations from multivariable calculus; mainly we are going to use the Lagrange multipliers method. This method is thought to help us to find a extreme value of a multivariable function 'F' given a restriction 'G'. F represents the function that we want to optimize and G is just a relation between the variables of which F depends. The Lagrange method for just one restriction is:

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First, let's build the function that we want to optimize, that is the cost. The cost is a function that must sum the cost of the sides material and the cost of the top and bottom material. The cost of the sides material is the unitary cost (0.03) multiplied by the sides area, which is A_s=2\pi rh for a cylinder; while the cost of the top and bottom material is the unitary cost (0.05) multiplied by the area of this faces, which is A_{TyB}=2\pi r^2 for a cylinder.

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\nabla C=\lambda \nabla V\\\frac{\partial C}{\partial r}=0.06\pi h+0.2\pi r\\\frac{\partial C}{\partial h}=0.06\pi r\\\frac{\partial V}{\partial r}=2\pi rh\\\frac{\partial V}{\partial h}=\pi r^2\\(0.06\pi h+0.2\pi r,0.06\pi r)=\lambda (2\pi rh,\pi r^2)

At this point we have a three variable (h,r, λ)-three equation system, which solution will be the optimum point for the cost (the minimum). Let's write the system:

0.06\pi h+0.2\pi r=2\lambda \pi rh\\0.06\pi r=\lambda \pi r^2\\500=\pi hr^2

(In this kind of problems always the additional equation is the restricion, in this case, V=500).

Let's divide the first and second equations by π:

0.06h+0.2r=2\lambda rh\\0.06r=\lambda r^2\\500=\pi hr^2

Isolate λ from the second equation:

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Isolate h from the third equation:

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And then, replace λ and h in the first equation:

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Multiply all the resultant equation by \pi r^{2}:

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h=\frac{500}{\pi r^2}\\h=\frac{500}{\pi (3.628)^2}=12.093cm

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