y = esin x
Outer function: e( ); inner function: sin x; inner derivative: cos x.
dy/dx = cos x · esin x
y = ln(tan x)
Outer function: ln( ); inner function: tan x; inner derivative: sec²x.
dy/dx = sec²x / tan x
Since sec²x = 1/cos²x and tan x = sin x/cos x:
dy/dx = (1/cos²x) ÷ (sin x/cos x) = 1/(cos x · sin x) = 1/(sin x cos x)
y = sin3x = (sin x)3
Outer function: ( )3; inner function: sin x; inner derivative: cos x.
dy/dx = 3(sin x)2 · cos x = 3 sin²x cos x
y = cos4(3x) = (cos(3x))4
This requires two applications of the chain rule (or the power-chain rule applied carefully):
Step 1: Outer power rule → 4(cos(3x))3
Step 2: Derivative of cos(3x) = −3 sin(3x)
dy/dx = 4(cos(3x))3 × (−3 sin(3x)) = −12 cos3(3x) sin(3x)
y = e2x+1
Outer function: e( ); inner function: 2x + 1; inner derivative: 2.
dy/dx = 2e2x+1
At x = 0: gradient = 2e2(0)+1 = 2e1 = 2e
y = sin(2x)
At x = π/4: y = sin(2 × π/4) = sin(π/2) = 1. Point: (π/4, 1).
dy/dx = 2 cos(2x)
At x = π/4: gradient = 2 cos(π/2) = 2 × 0 = 0
Tangent: y − 1 = 0(x − π/4) ⇒ y = 1
This is a horizontal tangent because x = π/4 is the maximum of sin(2x).
y = ln(sin²x)
Apply log law first: ln(sin²x) = 2 ln(sin x)
Now differentiate: dy/dx = 2 × (cos x / sin x) = 2 cot x
(Alternatively without log laws: inner function sin²x, inner derivative 2 sin x cos x;
dy/dx = 2 sin x cos x / sin²x = 2 cos x / sin x = 2 cot x ✓)
Setting v = 0: e−t ≠ 0 for all t, so:
2 cos(2t) − sin(2t) = 0
tan(2t) = 2
2t = arctan(2) + nπ (for integer n)
First solution for t > 0: t = arctan(2)/2 ≈ 1.107/2 ≈ 0.554 s