Analyzing the Setup
The curve is defined by the integral function:
y=∫0x∣t∣dt
The function ∣t∣ represents a V-shaped graph. Integrating this from 0 to x calculates the signed area under this graph.
For
x≥0, the area is the integral of
t, which yields:
y=2x2
For
x<0, the area accumulates as the integral of
−t, which yields:
y=−2x2
This results in a continuous curve composed of two parabolic segments joined at the origin.
The Power of Newton-Leibniz
We seek tangents to this curve that are parallel to the line y=2x. Since parallel lines share the same slope, our target slope is m=2.
To find the slope of the curve at any point, we apply the
Newton-Leibniz rule. This rule states that the derivative of an integral with respect to its upper limit is the integrand evaluated at that limit:
dxdy=∣x∣
This confirms that the slope of the curve at any point x is exactly the absolute value of x.
Finding the Points of Tangency
We set the derivative equal to our target slope:
∣x∣=2
This equation yields two points of interest: x=2 and x=−2. We now calculate the corresponding y-coordinates by evaluating the original integral at these points.
For
x=2:
y=∫02tdt=[2t2]02=2
For
x=−2:
y=∫0−2(−t)dt=[−2t2]0−2=−2
The points of tangency are (2,2) and (−2,−2).
The Final Intercepts
Using the point-slope form y−y1=m(x−x1) with m=2, we construct the equations for the tangent lines.
For the point
(2,2):
y−2=2(x−2)⇒y=2x−2
For the point
(−2,−2):
y−(−2)=2(x−(−2))⇒y=2x+2
To find the x-intercepts, we set y=0 in both equations. For y=2x−2, we find x=1. For y=2x+2, we find x=−1.
The final x-intercepts are ±1.