Analyzing the Identity
We are presented with the trigonometric identity:
This expression is a functional identity, meaning it holds true for all values of θ. Because it is an identity, we are free to choose specific values for θ or apply operations like differentiation to isolate the coefficients br.
The Hunt for b0
To isolate the constant term b0, we examine the expanded form:
sinnθ=b0+b1sinθ+b2sin2θ+⋯+bnsinnθ
Notice that every term on the right side, except for b0, contains at least one factor of sinθ. By choosing θ=0, we force all terms involving sinθ to zero.
Substituting θ=0 into the identity yields:
sin(n⋅0)=b0+b1sin(0)+⋯+bnsinn(0)
Thus, we find that b0=0.
The Liberation of b1
To isolate b1, we cannot simply set θ=0, as b1sin(0) would also vanish. Instead, we employ the power of calculus by differentiating both sides of the identity with respect to θ.
Applying the chain rule to the left side and the power rule to the right side, we obtain:
dθd(sinnθ)=dθd(r=0∑nbrsinrθ)
ncosnθ=b1cosθ+2b2sinθcosθ+3b3sin2θcosθ+…
Now, we substitute θ=0 into this differentiated identity. Every term on the right side containing a factor of sinθ will vanish:
ncos(n⋅0)=b1cos(0)+0+0+…
Since cos(0)=1, the equation simplifies to:
Therefore, we conclude that b1=n.
Final Reflection
By utilizing the properties of identities, we successfully determined the coefficients without resorting to complex expansions. Through the strategic use of substitution and differentiation, we found:
b0=0 and b1=n.
Remember that in competitive mathematics, the most elegant path is often found by manipulating the structure of the equation rather than brute-forcing the algebra.