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Elodia [21]
4 years ago
15

If a cylindrical tank holds 100,00 gallons of water which can be drained from thebottom of the tank in an hour, then Torricelli’

s Law gives the volumeVof waterremaining in the tank aftertminutes asV(t) = 100,000(1−160t)20≤t≤60(a) What is the physical meaning ofV′(t)? What are the units?(b) Find and interpret the quantityV′(10).
Mathematics
1 answer:
tatyana61 [14]4 years ago
5 0

Answer:

First, I think the right formula is:

V(t) = 100,000(1-\frac{t}{60} ),20\leq t\leq 60

A) We first derive the formula given above:

V'(t)=-\frac{100000}{60}

V'(t) represent the drain rate of the tank volume.

B) the units is: gallons/time

C) at V'(10) = 100000/60 = 1666.66 gallons/time.

because the formula V'(t) is constant so it doesn't depend of time.

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Solve the initial value problem 2ty" + 10ty' + 8y = 0, for t &gt; 0, y(1) = 1, y'(1) = 0.
Eva8 [605]

I think you meant to write

2t^2y''+10ty'+8y=0

which is an ODE of Cauchy-Euler type. Let y=t^m. Then

y'=mt^{m-1}

y''=m(m-1)t^{m-2}

Substituting y and its derivatives into the ODE gives

2m(m-1)t^m+10mt^m+8t^m=0

Divide through by t^m, which we can do because t\neq0:

2m(m-1)+10m+8=2m^2+8m+8=2(m+2)^2=0\implies m=-2

Since this root has multiplicity 2, we get the characteristic solution

y_c=C_1t^{-2}+C_2t^{-2}\ln t

If you're not sure where the logarithm comes from, scroll to the bottom for a bit more in-depth explanation.

With the given initial values, we find

y(1)=1\implies1=C_1

y'(1)=0\implies0=-2C_1+C_2\implies C_2=2

so that the particular solution is

\boxed{y(t)=t^{-2}+2t^{-2}\ln t}

# # #

Under the hood, we're actually substituting t=e^u, so that u=\ln t. When we do this, we need to account for the derivative of y wrt the new variable u. By the chain rule,

\dfrac{\mathrm dy}{\mathrm dt}=\dfrac{\mathrm dy}{\mathrm du}\dfrac{\mathrm du}{\mathrm dt}=\dfrac1t\dfrac{\mathrm dy}{\mathrm du}

Since \frac{\mathrm dy}{\mathrm dt} is a function of t, we can treat \frac{\mathrm dy}{\mathrm du} in the same way, so denote this by f(t). By the quotient rule,

\dfrac{\mathrm d^2y}{\mathrm dt^2}=\dfrac{\mathrm d}{\mathrm dt}\left[\dfrac ft\right]=\dfrac{t\frac{\mathrm df}{\mathrm dt}-f}{t^2}

and by the chain rule,

\dfrac{\mathrm df}{\mathrm dt}=\dfrac{\mathrm df}{\mathrm du}\dfrac{\mathrm du}{\mathrm dt}=\dfrac1t\dfrac{\mathrm df}{\mathrm du}

where

\dfrac{\mathrm df}{\mathrm du}=\dfrac{\mathrm d}{\mathrm du}\left[\dfrac{\mathrm dy}{\mathrm du}\right]=\dfrac{\mathrm d^2y}{\mathrm du^2}

so that

\dfrac{\mathrm d^2y}{\mathrm dt^2}=\dfrac{\frac{\mathrm d^2y}{\mathrm du^2}-\frac{\mathrm dy}{\mathrm du}}{t^2}=\dfrac1{t^2}\left(\dfrac{\mathrm d^2y}{\mathrm du^2}-\dfrac{\mathrm dy}{\mathrm du}\right)

Plug all this into the original ODE to get a new one that is linear in u with constant coefficients:

2t^2\left(\dfrac{\frac{\mathrm d^2y}{\mathrm du^2}-\frac{\mathrm d y}{\mathrm du}}{t^2}\right)+10t\left(\dfrac{\frac{\mathrm dy}{\mathrm du}}t\right)+8y=0

2y''+8y'+8y=0

which has characteristic equation

2r^2+8r+8=2(r+2)^2=0

and admits the characteristic solution

y_c(u)=C_1e^{-2u}+C_2ue^{-2u}

Finally replace u=\ln t to get the solution we found earlier,

y_c(t)=C_1t^{-2}+C_2t^{-2}\ln t

4 0
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