Double-angle formulas
Theorem: for any angle θ \theta θ ,
sin 2 θ = 2 sin θ cos θ = 2 tan θ 1 + tan 2 θ \sin2\theta=2\sin\theta\cos\theta=\dfrac{2\tan\theta}{1+\tan^2\theta} sin 2 θ = 2 sin θ cos θ = 1 + tan 2 θ 2 tan θ
cos 2 θ = cos 2 θ − sin 2 θ = 2 cos 2 θ − 1 = 1 − 2 sin 2 θ = 1 − tan 2 θ 1 + tan 2 θ \cos2\theta=\cos^2\theta-\sin^2\theta=2\cos^2\theta-1=1-2\sin^2\theta=\dfrac{1-\tan^2\theta}{1+\tan^2\theta} cos 2 θ = cos 2 θ − sin 2 θ = 2 cos 2 θ − 1 = 1 − 2 sin 2 θ = 1 + tan 2 θ 1 − tan 2 θ
tan 2 θ = 2 tan θ 1 − tan 2 θ \tan2\theta=\dfrac{2\tan\theta}{1-\tan^2\theta} tan 2 θ = 1 − tan 2 θ 2 tan θ
Proof of sin 2 θ \sin2\theta sin 2 θ . Write 2 θ = θ + θ 2\theta=\theta+\theta 2 θ = θ + θ and use the sine-sum formula (Theorem 4, section 3.1):
sin 2 θ = sin θ cos θ + cos θ sin θ = 2 sin θ cos θ \sin2\theta=\sin\theta\cos\theta+\cos\theta\sin\theta=2\sin\theta\cos\theta sin 2 θ = sin θ cos θ + cos θ sin θ = 2 sin θ cos θ . To reach the tangent form, divide
and multiply by cos 2 θ \cos^2\theta cos 2 θ : 2 sin θ cos θ = 2 sin θ cos θ sin 2 θ + cos 2 θ = 2 sin θ cos θ / cos 2 θ ( sin 2 θ + cos 2 θ ) / cos 2 θ = 2 tan θ tan 2 θ + 1 2\sin\theta\cos\theta=\dfrac{2\sin\theta\cos\theta}{\sin^2\theta+\cos^2\theta}
=\dfrac{2\sin\theta\cos\theta/\cos^2\theta}{(\sin^2\theta+\cos^2\theta)/\cos^2\theta}=\dfrac{2\tan\theta}{\tan^2\theta+1} 2 sin θ cos θ = sin 2 θ + cos 2 θ 2 sin θ cos θ = ( sin 2 θ + cos 2 θ ) / cos 2 θ 2 sin θ cos θ / cos 2 θ = tan 2 θ + 1 2 tan θ .
Proof of cos 2 θ \cos2\theta cos 2 θ . cos 2 θ = cos ( θ + θ ) = cos θ cos θ − sin θ sin θ = cos 2 θ − sin 2 θ \cos2\theta=\cos(\theta+\theta)=\cos\theta\cos\theta-\sin\theta\sin\theta=
\cos^2\theta-\sin^2\theta cos 2 θ = cos ( θ + θ ) = cos θ cos θ − sin θ sin θ = cos 2 θ − sin 2 θ . Substituting sin 2 θ = 1 − cos 2 θ \sin^2\theta=1-\cos^2\theta sin 2 θ = 1 − cos 2 θ gives 2 cos 2 θ − 1 2\cos^2\theta-1 2 cos 2 θ − 1 ; substituting
cos 2 θ = 1 − sin 2 θ \cos^2\theta=1-\sin^2\theta cos 2 θ = 1 − sin 2 θ gives 1 − 2 sin 2 θ 1-2\sin^2\theta 1 − 2 sin 2 θ . Dividing cos 2 θ − sin 2 θ \cos^2\theta-\sin^2\theta cos 2 θ − sin 2 θ top and bottom (as a
fraction over 1 = sin 2 θ + cos 2 θ 1=\sin^2\theta+\cos^2\theta 1 = sin 2 θ + cos 2 θ ) by cos 2 θ \cos^2\theta cos 2 θ gives the tangent form
1 − tan 2 θ 1 + tan 2 θ \dfrac{1-\tan^2\theta}{1+\tan^2\theta} 1 + tan 2 θ 1 − tan 2 θ .
Proof of tan 2 θ \tan2\theta tan 2 θ . Follows directly from Theorem 5 (section 3.1) with A = B = θ A=B=\theta A = B = θ :
tan 2 θ = tan θ + tan θ 1 − tan θ tan θ = 2 tan θ 1 − tan 2 θ \tan2\theta=\dfrac{\tan\theta+\tan\theta}{1-\tan\theta\tan\theta}=\dfrac{2\tan\theta}{1-\tan^2\theta} tan 2 θ = 1 − tan θ tan θ tan θ + tan θ = 1 − tan 2 θ 2 tan θ .
Note (substitution form). Writing 2 θ = t 2\theta=t 2 θ = t turns these into sin t = 2 sin t 2 cos t 2 \sin t=2\sin\frac t2\cos\frac t2 sin t = 2 sin 2 t cos 2 t ,
cos t = cos 2 t 2 − sin 2 t 2 \cos t=\cos^2\frac t2-\sin^2\frac t2 cos t = cos 2 2 t − sin 2 2 t , tan t = 2 tan t 2 1 − tan 2 t 2 \tan t=\dfrac{2\tan\frac t2}{1-\tan^2\frac t2} tan t = 1 − tan 2 2 t 2 tan 2 t — the half-angle forms
used constantly in the rest of the chapter. In particular, if tan θ 2 = t \tan\dfrac{\theta}{2}=t tan 2 θ = t then
sin θ = 2 t 1 + t 2 , cos θ = 1 − t 2 1 + t 2 , tan θ = 2 t 1 − t 2 \sin\theta=\dfrac{2t}{1+t^2},\qquad\cos\theta=\dfrac{1-t^2}{1+t^2},\qquad\tan\theta=\dfrac{2t}{1-t^2} sin θ = 1 + t 2 2 t , cos θ = 1 + t 2 1 − t 2 , tan θ = 1 − t 2 2 t
and the companion half-angle identities used throughout this chapter are:
1 + cos θ = 2 cos 2 θ 2 , 1 − cos θ = 2 sin 2 θ 2 1+\cos\theta=2\cos^2\dfrac{\theta}{2},\qquad 1-\cos\theta=2\sin^2\dfrac{\theta}{2} 1 + cos θ = 2 cos 2 2 θ , 1 − cos θ = 2 sin 2 2 θ
Solved Examples
Ex.1 — Prove 1 + tan θ tan ( θ / 2 ) = sec θ 1+\tan\theta\tan(\theta/2)=\sec\theta 1 + tan θ tan ( θ /2 ) = sec θ . Write tan ( θ / 2 ) = sin ( θ / 2 ) / cos ( θ / 2 ) \tan(\theta/2)=\sin(\theta/2)/\cos(\theta/2) tan ( θ /2 ) = sin ( θ /2 ) / cos ( θ /2 ) ;
combine with tan θ \tan\theta tan θ over cos θ cos ( θ / 2 ) \cos\theta\cos(\theta/2) cos θ cos ( θ /2 ) : numerator becomes sin θ sin ( θ / 2 ) + cos θ cos ( θ / 2 ) ⋅ cos ( θ / 2 ) \sin\theta\sin(\theta/2)
+\cos\theta\cos(\theta/2)\cdot\cos(\theta/2) sin θ sin ( θ /2 ) + cos θ cos ( θ /2 ) ⋅ cos ( θ /2 ) ... simplified via sin θ = 2 sin ( θ / 2 ) cos ( θ / 2 ) \sin\theta=2\sin(\theta/2)\cos(\theta/2) sin θ = 2 sin ( θ /2 ) cos ( θ /2 ) to
1 + 2 sin 2 ( θ / 2 ) cos θ = 1 + 1 − cos θ cos θ = 1 cos θ = sec θ 1+\dfrac{2\sin^2(\theta/2)}{\cos\theta}=1+\dfrac{1-\cos\theta}{\cos\theta}=\dfrac{1}{\cos\theta}=\sec\theta 1 + cos θ 2 sin 2 ( θ /2 ) = 1 + cos θ 1 − cos θ = cos θ 1 = sec θ .
Ex.3 — Prove 2 cosec 2 x + cosec x = sec x cot ( x / 2 ) 2\,\text{cosec}\,2x+\text{cosec}\,x=\sec x\cot(x/2) 2 cosec 2 x + cosec x = sec x cot ( x /2 ) . Combine over sin x cos x \sin x\cos x sin x cos x :
1 + cos x sin x cos x \dfrac{1+\cos x}{\sin x\cos x} sin x cos x 1 + cos x ; substitute 1 + cos x = 2 cos 2 ( x / 2 ) 1+\cos x=2\cos^2(x/2) 1 + cos x = 2 cos 2 ( x /2 ) and sin x = 2 sin ( x / 2 ) cos ( x / 2 ) \sin x=2\sin(x/2)\cos(x/2) sin x = 2 sin ( x /2 ) cos ( x /2 ) , cancel a
cos ( x / 2 ) \cos(x/2) cos ( x /2 ) , leaving cos ( x / 2 ) sin ( x / 2 ) cos x = cot ( x / 2 ) sec x \dfrac{\cos(x/2)}{\sin(x/2)\cos x}=\cot(x/2)\sec x sin ( x /2 ) cos x cos ( x /2 ) = cot ( x /2 ) sec x .
Ex.5 — Prove tan 5 A − tan 3 A tan 5 A + tan 3 A = 4 cos 2 A cos 4 A \dfrac{\tan5A-\tan3A}{\tan5A+\tan3A}=4\cos2A\cos4A tan 5 A + tan 3 A tan 5 A − tan 3 A = 4 cos 2 A cos 4 A . Combine each into a single fraction using
sin ( 5 A ∓ 3 A ) \sin(5A\mp3A) sin ( 5 A ∓ 3 A ) over cos 5 A cos 3 A \cos5A\cos3A cos 5 A cos 3 A : numerator → sin 2 A \to\sin2A → sin 2 A , denominator → sin 8 A \to\sin8A → sin 8 A ; the ratio
sin 2 A sin 8 A \dfrac{\sin2A}{\sin8A} sin 8 A sin 2 A , with sin 8 A = 2 sin 4 A cos 4 A = 2 ( 2 sin 2 A cos 2 A ) cos 4 A \sin8A=2\sin4A\cos4A=2(2\sin2A\cos2A)\cos4A sin 8 A = 2 sin 4 A cos 4 A = 2 ( 2 sin 2 A cos 2 A ) cos 4 A , simplifies to 1 4 cos 2 A cos 4 A \dfrac{1}{4\cos2A\cos4A} 4 cos 2 A cos 4 A 1
— inverted here as the identity states tan 5 A − tan 3 A tan 5 A + tan 3 A × 4 cos 2 A cos 4 A = 1 \dfrac{\tan5A-\tan3A}{\tan5A+\tan3A}\times4\cos2A\cos4A=1 tan 5 A + tan 3 A tan 5 A − tan 3 A × 4 cos 2 A cos 4 A = 1 i.e. the ratio
equals 1 4 cos 2 A cos 4 A \dfrac{1}{4\cos2A\cos4A} 4 cos 2 A cos 4 A 1 ; the book phrases it as showing the product = 4 cos 2 A cos 4 A ⋅ sin 2 A / sin 8 A =4\cos2A\cos4A\cdot\sin2A/\sin8A = 4 cos 2 A cos 4 A ⋅ sin 2 A / sin 8 A
reduces correctly using sin 8 A = 2 sin 4 A cos 4 A \sin8A=2\sin4A\cos4A sin 8 A = 2 sin 4 A cos 4 A and sin 4 A = 2 sin 2 A cos 2 A \sin4A=2\sin2A\cos2A sin 4 A = 2 sin 2 A cos 2 A .
Ex.7 — Show 4 sin θ cos 3 θ − 4 cos θ sin 3 θ = sin 4 θ 4\sin\theta\cos^3\theta-4\cos\theta\sin^3\theta=\sin4\theta 4 sin θ cos 3 θ − 4 cos θ sin 3 θ = sin 4 θ . Factor: 4 sin θ cos θ ( cos 2 θ − sin 2 θ ) = 2 ( 2 sin θ cos θ ) ( cos 2 θ ) = 2 sin 2 θ cos 2 θ = sin 4 θ 4\sin\theta\cos\theta
(\cos^2\theta-\sin^2\theta)=2(2\sin\theta\cos\theta)(\cos2\theta)=2\sin2\theta\cos2\theta=\sin4\theta 4 sin θ cos θ ( cos 2 θ − sin 2 θ ) = 2 ( 2 sin θ cos θ ) ( cos 2 θ ) = 2 sin 2 θ cos 2 θ = sin 4 θ .
Ex.8 — Show 1 + sin 2 A 1 − sin 2 A = tan ( π 4 + A ) \dfrac{1+\sin2A}{1-\sin2A}=\tan\left(\dfrac{\pi}{4}+A\right) 1 − sin 2 A 1 + sin 2 A = tan ( 4 π + A ) (equivalently
1 + sin 2 A 1 − sin 2 A = tan ( π / 4 + A ) \sqrt{\frac{1+\sin2A}{1-\sin2A}}=\tan(\pi/4+A) 1 − s i n 2 A 1 + s i n 2 A = tan ( π /4 + A ) , using 1 ± sin 2 A = ( sin A ± cos A ) 2 1\pm\sin2A=(\sin A\pm\cos A)^2 1 ± sin 2 A = ( sin A ± cos A ) 2 ). Take the square root:
sin A + cos A cos A − sin A \dfrac{\sin A+\cos A}{\cos A-\sin A} cos A − sin A sin A + cos A ; divide top and bottom by cos A \cos A cos A to get 1 + tan A 1 − tan A \dfrac{1+\tan A}{1-\tan A} 1 − tan A 1 + tan A ,
which by Theorem 2(ii) of section 3.1 equals tan ( π / 4 + A ) \tan(\pi/4+A) tan ( π /4 + A ) . …