Analyzing the Setup
Imagine a particle constrained to move along a straight line, specifically the y-axis. It starts its journey at the origin, where y=0, and travels upwards until it reaches y=10.
During this journey, it experiences a force given by F=(5y+20)j^.
Notice how the force is not a simple constant number. Because it contains the variable y, the magnitude of the force changes as the particle changes its position. This is the defining characteristic of a variable force.
The Master Equation
When dealing with a constant force, we can simply multiply force by displacement. However, for a variable force, we must sum up the infinitesimally small amounts of work done over tiny displacements.
This requires the power of integration. The fundamental formula for work done by a variable force is:
Since our particle is moving exclusively along the y-axis, our infinitesimal displacement vector is simply dr=dyj^.
Substituting our given force and displacement into the integral, and setting our limits from the starting position to the final position, we get:
Because the dot product of j^⋅j^ is exactly 1, the vector equation beautifully simplifies into a standard scalar integral:
Executing the Integration
Now, we perform the mathematical heavy lifting. We integrate the polynomial term by term.
The integral of 5y with respect to y is 25y2. The integral of the constant 20 is simply 20y.
Applying these rules, our expression becomes:
Final Calculation
The final step is to evaluate this expression at our upper and lower limits. We substitute y=10 into the expression first, and then subtract the expression evaluated at y=0.
W=(25(10)2+20(10))−(25(0)2+20(0))
The lower limit evaluates entirely to zero, making our lives easier. For the upper limit, 102 is 100.
Multiplying 100 by 25 gives 250. Adding this to 20×10, which is 200, we arrive at our final destination.
The total work done by this variable force is exactly 450 Joules.