Find the work done as the particle moves along a straight line from (2, 0, 0) to (2, 1, 5).
Understand the Problem
The question asks for the work done by an electric force as a particle moves from one point to another in space. To solve this, we will apply the work done formula in the context of vector fields, using the given force function and the specific path along which the particle moves.
Answer
$$ W = K\left( \frac{1}{2} - \frac{1}{\sqrt{30}} \right) $$
Answer for screen readers
The work done as the particle moves is:
$$ W = K\left( \frac{1}{2} - \frac{1}{\sqrt{30}} \right) $$
Steps to Solve
- Identify the force vector
The force exerted on the charged particle is given by:
$$ F(\mathbf{r}) = K \frac{\mathbf{r}}{|\mathbf{r}|^3} $$
Where $\mathbf{r} = \langle x, y, z \rangle$. To compute the force at any point, we need to calculate $|\mathbf{r}| = \sqrt{x^2 + y^2 + z^2}$.
- Determine the path of motion
The particle moves from point A $(2, 0, 0)$ to point B $(2, 1, 5)$. We can parameterize the path using a variable $t$ where:
$$ \mathbf{r}(t) = \langle 2, t, 5t \rangle \quad \text{for} \quad t \in [0, 1] $$
This parameterization describes a straight line from A to B.
- Calculate the force along the path
Substitute the parameterization into the force function:
$$ \mathbf{r}(t) = \langle 2, t, 5t \rangle $$
Now, compute the magnitude:
$$ |\mathbf{r}(t)| = \sqrt{2^2 + t^2 + (5t)^2} = \sqrt{4 + t^2 + 25t^2} = \sqrt{4 + 26t^2} $$
Then, the force becomes:
$$ F(t) = K \frac{\langle 2, t, 5t \rangle}{(4 + 26t^2)^{3/2}} $$
- Find the differential displacement vector
To find the work done, we need the differential displacement vector:
$$ d\mathbf{r} = \frac{d\mathbf{r}}{dt} dt = \langle 0, 1, 5 \rangle dt $$
- Calculate the work done
The work done is given by the integral of the force along the path:
$$ W = \int_{0}^{1} F(t) \cdot d\mathbf{r} $$
Substituting in our expressions:
$$ W = \int_{0}^{1} K \frac{\langle 2, t, 5t \rangle}{(4 + 26t^2)^{3/2}} \cdot \langle 0, 1, 5 \rangle dt $$
Calculate the dot product:
$$ W = \int_{0}^{1} K \frac{t + 25t}{(4 + 26t^2)^{3/2}} dt = \int_{0}^{1} K \frac{26t}{(4 + 26t^2)^{3/2}} dt $$
- Evaluate the integral
To evaluate the integral, use a substitution method. Let ( u = 4 + 26t^2 ), then ( du = 52t dt ) or ( dt = \frac{du}{52t} ).
Transform the limits for $t = 0$ to $t = 1$:
When $t = 0$, ( u = 4 ) and when ( t = 1 ), ( u = 30 ).
The adjusted integral becomes:
$$ W = K \int_{4}^{30} \frac{26}{u^{3/2}} \cdot \frac{1}{52} du = \frac{K}{2} \int_{4}^{30} u^{-3/2} du $$
Evaluate the integral:
$$ W = \frac{K}{2} \left[-2 u^{-1/2}\right]_{4}^{30} = K \left[-1/\sqrt{30} + \frac{1}{2}\right] $$
- Final expression for work done
After evaluating, the expression for work done is:
$$ W = K\left( \frac{1}{2} - \frac{1}{\sqrt{30}} \right) $$
The work done as the particle moves is:
$$ W = K\left( \frac{1}{2} - \frac{1}{\sqrt{30}} \right) $$
More Information
This result shows the dependency of work done on both the constant $K$ and the path taken by the charged particle through the electric field. The work done against electric forces can vary significantly based on the path followed.
Tips
- Misunderstanding the parameterization of the path: Ensure that the parameter corresponds to the movement between the two points correctly.
- Forgetting the dot product: Always compute the dot product of the force vector and the displacement vector.
- Incorrect limits during substitution in integrals: Carefully adjust the limits when making a substitution in an integral.
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