Question
Gravitational fielda. Find a potential function for the gravitational field$$\mathbf{F}=-G m M \frac{x \mathbf{i}+y \mathbf{j}+z \mathbf{k}}{\left(x^{2}+y^{2}+z^{2}\right)^{3 / 2}}$$b. Let $P_{1}$ and $P_{2}$ be points at distances $s_{1}$ and $s_{2}$ from the origin. Show that the work done by the gravitational field in part (a) in moving a particle from $P_{1}$ to $P_{2}$ is$$G m M\left(\frac{1}{s_{2}}-\frac{1}{s_{1}}\right)$$
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This means we need to find a function $f$ such that $\nabla f = \mathbf{F}$. Show more…
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Gravitational field \begin{equation}\begin{array}{c}{\text { a. Find a potential function for the gravitational field }} \\ {\mathbf{F}=-G m M \frac{x \mathbf{i}+y \mathbf{j}+z \mathbf{k}}{\left(x^{2}+y^{2}+z^{2}\right)^{3 / 2}}} \\ {(G, m, \text { and } M \text { are constants })}\\{\text { b. Let } P_{1} \text { and } P_{2} \text { be points at distance } s_{1} \text { and } s_{2} \text { from the origin. }} \\ {\text { Show that the work done by the gravitational field in part (a) }} \\ {\text { in moving a particle from } P_{1} \text { to } P_{2} \text { is }}\end{array}\end{equation} \begin{equation}\operatorname{GmM}\left(\frac{1}{s_{2}}-\frac{1}{s_{1}}\right).\end{equation}
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Path Independence Conservative Fields and Potential
a. Find a potential function for the gravitational field $$\mathbf{F}=-G m M \frac{x \mathbf{i}+y \mathbf{j}+z \mathbf{k}}{\left(x^{2}+y^{2}+z^{2}\right)^{3 / 2}}$$ $(G, m, \text { and } M$ are constants). b. Let $P_{1}$ and $P_{2}$ be points at distance $s_{1}$ and $s_{2}$ from the origin. Show that the work done by the gravitational field in part (a) in moving a particle from $P_{1}$ to $P_{2}$ is
Path Independence, Conservative Fields, and Potential Functions
a. Find a potential function for the gravitational field $$\mathbf{F}=-G m M \frac{x \mathbf{i}+y \mathbf{j}+z \mathbf{k}}{\left(x^{2}+y^{2}+z^{2}\right)^{3 / 2}}$$ $(G, m,$ and $M$ are constants $)$ b. Let $P_{1}$ and $P_{2}$ be points at distance $s_{1}$ and $s_{2}$ from the origin. Show that the work done by the gravitational field in part (a) in moving a particle from $P_{1}$ to $P_{2}$ is $$\operatorname{GmM}\left(\frac{1}{S_{2}}-\frac{1}{S_{1}}\right)$$
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