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Determine the amount of salt in the tank at time tin Example 5if the concentration of salt in the inflow is variable and given by cin(t)=2+sin(t/4)lb/gal. Without actually graphing,conjecture what the solution curve of the IVP should look like.Then use a graphing utility to plot the graph of the solution on the interval [0,300]. Repeat for the [0,600]intervaland compare your graph with that in Figure 3.1.6(a).

Short Answer

Expert verified

The number of pounds of salt in the tank at time is A=600+350313sint4-1250313cost4-168,400313e-t100. The amount of salt in the tank depends on the sine function and so, it will increase and decrease with time locally like a sine wave.

Step by step solution

01

Define mixtures.

The mixing of two fluids sometimes gives rise to a linear first-order differential equation.

dAdt=(input rate of salt)-(output rate of salt)=Rin-Rout

02

Solve for first order number of pounds.

Let the concentration of the solution entering in the tank becin(t)=2+sin(t/4)lb/galat the rate of3gal/min. Then the rate at which the salt enters the tank is,

Rin=2+sint4lbgal×3galmin=6+3sint4lbmin

And, the rate at which the salt leaves the tank is,

Rout=A100lbmin

Let the differential equation with the amount of salt in pounds A as be,

dAdt= Input rate of salt - Input rate of salt=FinCin-FoutCout

dAdt=6+3sint4-A100… (1)

03

Multiply the equation by the IF.

Let the integrating factor be,

e11000dt=et1010

dAdyet100+A100et100=6+3sint4et100IddtAet100=6e1100+3sint4et100ddtAet100=6et100+3sint4et100Aet100=6et1001100+3sint4et100=600et100+3100et100sint4-25et100cost4dt=600et100+3100et100sint4-250025626etI00sint4+1626et100cost4Aet100=600et100+350313et100sint4-1250313etI00cost4+C

A=600+350313sint4-1250313cost4+Ce-t100… (3)

04

Obtain the values of constants.

To find the values of constants, apply the pointA(0)=30in the equation (3), then

50=600+350313sin04-1250313cos04+Ce-0100-550=30-1250313+CC=-550-3750313=-168,400313

Substitute the value of cin the equation (3).

A=600+350313sint4-1250313cost4-168,400313e-t100

05

Obtain the graph of the obtained solution.

Let the graph of the solution on the interval (0,300)be,

Let the graph of the solution on the interval (0,600)be,

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An LR-series circuit has a variable inductor with the inductance defi­ned by

L(t)={1-110t,0t100,t>10

Find the current i(t) if the resistance is 0.2 ohm, the impressed voltage is E(t) 5 4, and i(0) 5 0. Graph i(t).

Question: Sawing Wood A long uniform piece of wood (cross sections are the same) is cut through perpendicular to its length by a vertical saw blade. See Figure 3.R.6. If the friction between the sides of the saw blade and the wood through which the blade passes is ignored, then it can be assumed that the rate at which the saw blade moves through the piece of wood is inversely proportional to the width of the wood in contact with its cutting edge. As the blade advances through the wood (moving, say, left to right) the width of a cross section changes as a nonnegative continuous function\(w\). If a cross section of the wood is described as a region in the\(xy\)-plane defined over an interval \((a,b)\)then, as shown in Figure 3.R.6(c), the position\(x\)of the saw blade is a function of time \(t\)and the vertical cut made by the blade can be represented by a vertical line segment. The length of this vertical line is the width\(w(x)\)of the wood at that point. Thus the position\(x(t)\)of the saw blade and the rate \(dx/dt\)at which it moves to the right are related to\(w(x)\)by\(w(x)\frac{{dx}}{{dt}} = k,x(0) = a\)

Here\(k\) represents the number of square units of the material removed by the saw blade per unit time.

  1. Suppose the saw is computerized and can be programmed so that\(k = 1\). Find an implicit solution of the foregoing initial-value problem when the piece of wood is a circular\(\log \). Assume a cross section is a circle of radius 2 centered at\((0,0)\) (Hint: To save time see formula 41 in the table of integrals given on the right inside page of the front cover.)
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mdvdt=mg-kv

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(c) If the distance s, measured from the point where the mass was released above ground, is related to velocity v by ds/dt=v(t), nd an explicit expression for s(t) if s(0)=0.

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When all the curves in a familyG(x,y,c1)=0 intersect orthogonally all the curves in another family localid="1667974378968" H(x,y,c1)=0, the families are said to be orthogonal trajectories of each other. See Figure 3.R.5. If localid="1667974383247" dydx=f(x,y) is the differential equation of one family, then the differential equation for the orthogonal trajectories of this family is localid="1667974387852" dydx=1f(x,y).Find the differential equation of the given family by computing localid="1667974392147" dydx and eliminating localid="1667974397114" c1from this equation. Then find the orthogonal trajectories of the family. Use a graphing utility to graph both families on the same set of coordinate axes.

y=c1x

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