Each part is proved from the Law of Sines/Cosines/Projection-formula toolkit; the recurring trick is replacing an angle sum by its supplement (A+B+C=π) and applying sum-to-product identities.
Part (i): asin(2A+B)=(b+c)sin2A.
Step 1. Simplify the RHS: b+c=2R(sinB+sinC)=4Rsin2B+Ccos2B−C. Since B+C=π−A, 2B+C=90∘−2A, so sin2B+C=cos2A. Hence b+c=4Rcos2Acos2B−C, and
(b+c)sin2A=4Rcos2Asin2Acos2B−C=2RsinAcos2B−C=acos2B−C
(using 2sin2Acos2A=sinA and 2RsinA=a).
Step 2. Simplify the LHS: 90∘−(2A+B)=2π−2A−B=2B+C−B=2C−B (using 2π−2A=2B+C). So sin(2A+B)=cos(2C−B)=cos(2B−C) (cosine is even). Hence LHS =acos2B−C, matching Step 1.
Part (ii): a(cosB+cosC)=2(b+c)sin22A.
Step 1. By the projection formula, c=acosB+bcosA⇒acosB=c−bcosA, and b=acosC+ccosA⇒acosC=b−ccosA.
Step 2. Add: acosB+acosC=(c−bcosA)+(b−ccosA)=(b+c)−(b+c)cosA=(b+c)(1−cosA).
Step 3. Use 1−cosA=2sin22A: a(cosB+cosC)=(b+c)⋅2sin22A=2(b+c)sin22A.
Part (iii): b2a2−c2=sin(A+C)sin(A−C).
Step 1. Convert to sines: b2a2−c2=4R2sin2B4R2sin2A−4R2sin2C=sin2Bsin2A−sin2C.
Step 2. Use sin2X−sin2Y=sin(X+Y)sin(X−Y) with X=A,Y=C: sin2A−sin2C=sin(A+C)sin(A−C).
Step 3. Since B=π−(A+C), sinB=sin(A+C), so sin2B=sin2(A+C).
Step 4. Combine: b2a2−c2=sin2(A+C)sin(A+C)sin(A−C)=sin(A+C)sin(A−C).
Part (iv): b2−c2asin(B−C)=c2−a2bsin(C−A)=a2−b2csin(A−B).
Step 1. Show the first fraction equals the constant 2R1. Using b2−c2=4R2(sin2B−sin2C)=4R2sin(B+C)sin(B−C), and sin(B+C)=sinA (since B+C=π−A), b2−c2=4R2sinAsin(B−C). …