Analyzing the Setup
The given curve is defined by the equation:
While the expression appears complex, we can dismantle it systematically to find the equation of the normal line at x=0.
Phase 1
Finding the Point of Contact
To find the point of contact P(x1,y1), we substitute x=0 into the original equation:
Since 1y=1 for any finite y and sin−1(0)=0, we find y=1+0=1. Thus, our anchor point is P(0,1).
Phase 2
The Divide and Conquer Strategy
We need the slope of the tangent, mt=dxdy. To avoid messy differentiation, we define y=u+v, where:
u=(1+x)yandv=sin−1(sin2x)
The derivative is then simply:
Phase 3
Taming the Variable Exponent
For u=(1+x)y, we apply logarithmic differentiation:
Differentiating implicitly with respect to x gives:
u1dxdu=dxdyln(1+x)+y⋅1+x1
Substituting x=0,y=1,u=1 into this expression, the term ln(1+0) vanishes, leaving:
Phase 4
The Chain Rule Dance
Next, we differentiate v=sin−1(sin2x) using the chain rule:
dxdv=1−(sin2x)21⋅dxd(sin2x) The derivative of sin2x is 2sinxcosx. Substituting x=0 makes the numerator 2sin(0)cos(0)=0, so:
Phase 5
The Final Assembly
We combine our results to find the slope of the tangent:
Since the normal is perpendicular to the tangent, its slope mn must satisfy mn⋅mt=−1, yielding mn=−1.
Using the point-slope form y−y1=mn(x−x1) with P(0,1) and mn=−1:
The final equation of the normal line is x+y=1.