Each result cited below is universally quantified over the data in its own statement; it is applied to the data named at the point of use. Throughout, R is a field, so its addition and multiplication are commutative and associative, multiplication distributes over addition, and s+(βs)=0; these are used below in rearranging the finite sums that occur. Let u,vβR.
Claim 1 (the formulas for a difference).
cos(uβv)=cosucosv+sinusinv,sin(uβv)=sinucosvβcosusinv.
Since uβv=u+(βv), clause Addition Formulas for Sine and Cosine Β§cosine, applied with a=u and x=βv, gives
cos(uβv)=cosucos(βv)βsinusin(βv),
and clause Addition Formulas for Sine and Cosine Β§sine gives
sin(uβv)=sinucos(βv)+cosusin(βv).
By Uniform Convergence, Continuity, Parity and Derivatives of Sine and Cosine Β§parity, cos(βv)=cosv and sin(βv)=βsinv. Claim 2 of Zero Products and Elementary Identities in a Field gives s(βr)=β(sr) for all s,rβR, so βsinusin(βv)=sinusinv and cosusin(βv)=β(cosusinv), which yields the two displayed identities.
Claim 2 (doubling). For every wβR, w+w=2w.
Indeed w+w=1β
w+1β
w=(1+1)w=2w, by the multiplicative identity of R, distributivity, and the abbreviation 2=1+1 of the statement.
Claim 3 (clause 1). By Claim 1 and Addition Formulas for Sine and Cosine Β§cosine applied with a=u and x=v,
cos(uβv)+cos(u+v)=(cosucosv+sinusinv)+(cosucosvβsinusinv).
Rearranging the four summands, the two terms sinusinv and βsinusinv sum to 0, so the right-hand side is cosucosv+cosucosv, which is 2cosucosv by Claim 2.
Claim 4 (clause 2). From the same two expansions,
cos(uβv)βcos(u+v)=(cosucosv+sinusinv)β(cosucosvβsinusinv),
and now the two terms cosucosv and βcosucosv sum to 0, leaving sinusinv+sinusinv, which is 2sinusinv by Claim 2.
Claim 5 (clause 3). By Addition Formulas for Sine and Cosine Β§sine applied with a=u and x=v, and by Claim 1,
sin(u+v)+sin(uβv)=(sinucosv+cosusinv)+(sinucosvβcosusinv).
The two terms cosusinv and βcosusinv sum to 0, leaving sinucosv+sinucosv, which is 2sinucosv by Claim 2.
As u,vβR were arbitrary, the three clauses hold for all u,vβR.