the hyperbolic sibling of the tangent addition formula — with a + where trigonometry has a −. A dividend: since ∣tanh∣<1, the right-hand side is a “velocity addition” rule that never leaves (−1,1): if u,v∈(−1,1) then 1+uvu+v∈(−1,1) as well (write u=tanha, v=tanhb, possible by bijectivity, and read the formula backwards). Checking that algebraically, without hyperbolic functions, is a slightly painful exercise; parametrizing by tanh makes it one line — the same strategy that circular functions provide for the unit circle.
Example 4.22(Closed forms at work)
The solution of cosht=2 with t≥0 is, by the closed form, t=arcosh2=ln(2+3)≈1.317; the other solution is −t, by evenness — and indeed ln(2−3)=ln2+31=−ln(2+3): the two roots u=et of the quadratic u2−4u+1=0 are reciprocals, as their product 1 (Vieta) demands. This tiny computation displays the general pattern: hyperbolic equations convert to quadratics in et, and the symmetry t↦−t appears as the symmetry u↦1/u of the quadratic — worth remembering when solving Exercise 4.7.