The Fundamental Connection
In electrostatics, the electric field and electric potential are intimately connected. The electric field is essentially the negative gradient of the electric potential. This means that if we know the electric field in a region, we can find the potential difference between any two points by integrating the field along the path connecting them.
The fundamental equation governing this relationship is dV=−E⋅dx. The negative sign is crucial here; it physically signifies that the electric field always points in the direction of decreasing electric potential. Imagine a ball rolling down a hill—the field points "downhill" towards lower potential.
Setting Up the Integral
To find the potential difference between two specific points, we integrate our differential equation. Integrating from an initial position x1 to a final position x2 gives us V2−V1=−∫x1x2E⋅dx.
However, the question specifically asks for V1−V2. By multiplying both sides of our integrated equation by −1, we elegantly absorb the negative sign on the right side. This leaves us with a much cleaner expression: V1−V2=∫x1x2E⋅dx.
Executing the Math
Now, we substitute the given electric field E=(20x+10)i^ into our integral. Since the displacement dx is also along the x-axis (dxi^), the dot product simplifies to just the product of their magnitudes. Our integral becomes V1−V2=∫1−5(20x+10)dx.
Performing the integration is straightforward polynomial calculus. The integral of 20x is 10x2, and the integral of 10 is 10x. Factoring out the 10 for simplicity, we get 10[x2+x] evaluated from 1 to −5.
Finally, we carefully substitute our upper and lower limits. Plugging in −5 gives ((−5)2−5)=20, and plugging in 1 gives (12+1)=2. Subtracting the lower limit evaluation from the upper limit evaluation yields 20−2=18. Multiplying this by our factored 10 gives the final potential difference of 180 V.