\(x^3 = θ ⇒ \frac{θ}{2} ∈\bigg(\frac{π}{4}, \frac{3π}{4}\bigg)\)
\(∴ y = tan^{–1} (secθ – tanθ)\)
= \(tan^{−1}(\frac{1−sinθ}{cos θ} )\)
\(∴y=\frac{π}{4}−\frac{θ}{2}.\)
\(y=\frac{π}{4}−\frac{x^3}{2}\)
\(∴y′=\frac{−3x^2}{2}\)
\(y'' = – 3x\)
\(∴ x^2y''-6y+\frac{3π}{2}=0\)
Hence, the correct option is (B): \(x^2y''-6y+\frac{3π}{2}\)
The number of solutions of the equation $ \cos 2\theta \cos \left( \frac{\theta}{2} \right) + \cos \left( \frac{5\theta}{2} \right) = 2 \cos^3 \left( \frac{5\theta}{2} \right) $ in the interval \(\left[ -\frac{\pi}{2}, \frac{\pi}{2} \right ]\) is:
In the given circuit the sliding contact is pulled outwards such that the electric current in the circuit changes at the rate of 8 A/s. At an instant when R is 12 Ω, the value of the current in the circuit will be A.
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
For $ \alpha, \beta, \gamma \in \mathbb{R} $, if $$ \lim_{x \to 0} \frac{x^2 \sin \alpha x + (\gamma - 1)e^{x^2} - 3}{\sin 2x - \beta x} = 3, $$ then $ \beta + \gamma - \alpha $ is equal to:
Trigonometric equation is an equation involving one or more trigonometric ratios of unknown angles. It is expressed as ratios of sine(sin), cosine(cos), tangent(tan), cotangent(cot), secant(sec), cosecant(cosec) angles. For example, cos2 x + 5 sin x = 0 is a trigonometric equation. All possible values which satisfy the given trigonometric equation are called solutions of the given trigonometric equation.
A list of trigonometric equations and their solutions are given below:
Trigonometrical equations | General Solutions |
sin θ = 0 | θ = nπ |
cos θ = 0 | θ = (nπ + π/2) |
cos θ = 0 | θ = nπ |
sin θ = 1 | θ = (2nπ + π/2) = (4n+1) π/2 |
cos θ = 1 | θ = 2nπ |
sin θ = sin α | θ = nπ + (-1)n α, where α ∈ [-π/2, π/2] |
cos θ = cos α | θ = 2nπ ± α, where α ∈ (0, π] |
tan θ = tan α | θ = nπ + α, where α ∈ (-π/2, π/2] |
sin 2θ = sin 2α | θ = nπ ± α |
cos 2θ = cos 2α | θ = nπ ± α |
tan 2θ = tan 2α | θ = nπ ± α |