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Show that \(V=(A / r)+B\) is a solution of the differential equation \(\frac{\mathrm{d}^{2} \mathrm{~V}}{\mathrm{dr}^{2}}+\frac{2}{\mathrm{r}} \frac{\mathrm{dV}}{\mathrm{dr}}=0\).

Short Answer

Expert verified
Question: Prove that the function \(V = (A / r) + B\) is a solution to the given differential equation \(\frac{\mathrm{d^2V}}{\mathrm{dr^2}}+\frac{2}{\mathrm{r}}\frac{\mathrm{dV}}{\mathrm{dr}}=0\). Answer: We have found the first derivative of V with respect to r as \(\frac{\mathrm{dV}}{\mathrm{dr}} = - \frac{A}{r^2}\) and the second derivative as \(\frac{\mathrm{d^2V}}{\mathrm{dr^2}} = \frac{2A}{r^3}\). By substituting these derivatives back into the differential equation and simplifying the equation, we obtain \(0 = 0\), which confirms that the function \(V = (A / r) + B\) is a solution to the given differential equation.

Step by step solution

01

Find the first derivative of the function V with respect to r

To find the first derivative \(\frac{\mathrm{dV}}{\mathrm{dr}}\), we will use the power rule and the constant rule of derivatives. We have: \(\frac{\mathrm{dV}}{\mathrm{dr}} = \frac{\mathrm{d}}{\mathrm{dr}}(A / r) + \frac{\mathrm{d}}{\mathrm{dr}} B = - \frac{A}{r^2}\) The first derivative of V with respect to r is \(\frac{\mathrm{dV}}{\mathrm{dr}} = - \frac{A}{r^2}\).
02

Find the second derivative of the function V with respect to r

To find the second derivative \(\frac{\mathrm{d^2V}}{\mathrm{dr^2}}\), we will differentiate the first derivative with respect to r. Again, we will use the power rule: \(\frac{\mathrm{d^2V}}{\mathrm{dr^2}} = \frac{\mathrm{d}}{\mathrm{dr}}(- \frac{A}{r^2}) = \frac{2A}{r^3}\) The second derivative of V with respect to r is \(\frac{\mathrm{d^2V}}{\mathrm{dr^2}} = \frac{2A}{r^3}\).
03

Plug the derivatives into the differential equation

Now, we will substitute our first and second derivatives back into the given differential equation: \(\frac{\mathrm{d^2V}}{\mathrm{dr^2}}+\frac{2}{\mathrm{r}}\frac{\mathrm{dV}}{\mathrm{dr}}=0\) Plugging in our derivatives: \(\frac{2A}{r^3}+\frac{2}{r}(-\frac{A}{r^2})=0\)
04

Simplify the equation

Now, we will simplify the equation to see if it is true: \(\frac{2A}{r^3}+\frac{-2A}{r^3}=\frac{2A-2A}{r^3}=0\) The equation holds true, as the left side simplifies to 0, which equals the right side. Thus, the function \(V = (A / r) + B\) is a solution to the given differential equation \(\frac{\mathrm{d^2V}}{\mathrm{dr^2}}+\frac{2}{\mathrm{r}}\frac{\mathrm{dV}}{\mathrm{dr}}=0\).

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Most popular questions from this chapter

Solve the following differential equations: (i) \(y^{\prime}-y \tan x=\frac{1}{\cos ^{3} x}, y(0)=0\). (ii) \(t\left(1+t^{2}\right) d x=\left(x+x t^{2}-t^{2}\right) d t ; x(1)=\frac{\pi}{4}\). (iii) \(\mathrm{y}^{\prime}-\frac{\mathrm{y}}{1-\mathrm{x}^{2}}=1+\mathrm{x}, \mathrm{y}(0)=1\) (iv) \(2 x y^{\prime}=y+6 x^{5 / 2}-2 \sqrt{x}, y(1)=3 / 2\)

A body in a room at \(60^{\circ}\) cools from \(200^{\circ}\) to \(120^{\circ}\) in halfan hour. (a) Show that its tmperature after \(\mathrm{t}\) minutes is \(60+140 \mathrm{e}^{-\mathrm{lt}}\), where \(\mathrm{k}=(\ln 7-\ln 3) / 30\) (b) Show that the time \(t\) required to reach a temperature of \(\mathrm{T}\) degrees is given by the formula \(\mathrm{t}=[\ln 140-\ln (\mathrm{T}-60)] / \mathrm{k}\), where \(60<\mathrm{T} \leq 200\). (c) Find the time at which the temperature is \(90^{\circ}\). (d) Find a formula for the temperature of the body at time \(t\) if the room temperature is not kept constant but falls at a rate of \(1^{\circ}\) each ten minutes. Assume the room temperature is \(60^{\circ}\) when the body temperature is \(200^{\circ}\).

\(\left(\mathrm{y}-\frac{\mathrm{xdy}}{\mathrm{d} x}\right)=3\left(1-\mathrm{x}^{2} \frac{\mathrm{dy}}{\mathrm{dx}}\right)\)

Solve the following differential equations: (i) \(y^{\prime}-y \ln 2=2^{\sin x}(\cos x-1) \ln 2, y\) being bounded when \(\mathrm{x} \rightarrow \infty\). (ii) \(y^{\prime} \sin x-y \cos x=-\frac{\sin ^{2} x}{x^{2}}, y \rightarrow 0\) as \(x \rightarrow \infty\) (iii) \(x^{2} y^{\prime} \cos \frac{1}{x}-y \sin \frac{1}{x}=-1, y \rightarrow 1\) as \(x \rightarrow \infty\). (iv) \(x^{2} y^{\prime}+y=\left(x^{2}+1\right) e^{x}, y \rightarrow 1\) as \(x \rightarrow \infty\)

\(\mathrm{e}^{x} \sin ^{3} y+\left(1+\mathrm{e}^{2 x}\right) \cos y \cdot y^{\prime}=0\)

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