Step 1: Determine where \(\sin x\) and \(\cos x\) intersect and which is larger.
We solve \(\sin x = \cos x\) for \(x\in[-\pi,\pi]\). This gives
\(\tan x = 1 \implies x = -\frac{3\pi}{4}\) and \(x=\frac{\pi}{4}\) (within \([-\pi,\pi]\)).
Hence, the interval \([-\pi,\pi]\) is split into three subintervals:
\([-\pi,-\frac{3\pi}{4}], [-\frac{3\pi}{4},\frac{\pi}{4}], [\frac{\pi}{4},\pi]\).
A quick check in each interval shows:
On \([-\pi,-\frac{3\pi}{4}]\), we have \(\sin x > \cos x\), so \(f(x)=\sin x\).
On \([-\frac{3\pi}{4},\frac{\pi}{4}]\), we have \(\cos x \ge \sin x\), so \(f(x)=\cos x\).
On \([\frac{\pi}{4},\pi]\), again \(\sin x \ge \cos x\), so \(f(x)=\sin x\).
Step 2: Find where these maxima are nonnegative (so they contribute positive “area”).
In \([-\pi,-\frac{3\pi}{4}]\), \(\sin x\) is actually negative, so the region above the \(x\)–axis is zero there.
In \([-\frac{3\pi}{4},-\frac{\pi}{2}]\), \(\cos x\) is also negative, so again no area above the axis.
In \([-\frac{\pi}{2},\frac{\pi}{4}]\), \(\cos x\) becomes nonnegative, so the area is \(\int_{-\pi/2}^{\pi/4}\cos x\,dx\).
Finally, in \([\frac{\pi}{4},\pi]\), \(\sin x\) is nonnegative, so the area is \(\int_{\pi/4}^{\pi}\sin x\,dx\).
Step 3: Compute these two integrals and sum.
\(\text{Area}_1 = \int_{-\pi/2}^{\pi/4}\cos x\,dx = [\sin x]_{-\pi/2}^{\pi/4} = \sin(\frac{\pi}{4}) - \sin(-\frac{\pi}{2}) = \frac{\sqrt{2}}{2} - (-1) = 1 + \frac{\sqrt{2}}{2}\).
\(\text{Area}_2 = \int_{\pi/4}^{\pi}\sin x\,dx = [-\cos x]_{\pi/4}^{\pi} = [-\cos(\pi)] - [-\cos(\frac{\pi}{4})] = [-(-1)] - [-\frac{\sqrt{2}}{2}] = 1 + \frac{\sqrt{2}}{2}\).
Hence the total area is
\(\text{Area} = (1 + \frac{\sqrt{2}}{2}) + (1 + \frac{\sqrt{2}}{2}) = 2 + \sqrt{2}\).
But we must not forget the small intervals \([-\pi,-\frac{3\pi}{4}]\) and \([-\frac{3\pi}{4},-\frac{\pi}{2}]\) where the function is negative; the “enclosed area” is the absolute value of that portion. Computing directly (or by symmetry arguments), one finds that adding those negative‐region contributions precisely yields a net of \(+2 - \sqrt{2}\), which combines with the above \(2+\sqrt{2}\) to total 4.
A quicker (and more careful) piecewise‐analysis shows the final sum of absolute areas is exactly:
\(4\).
Thus the region between \(y=f(x)\) and the \(x\)–axis has total area \(\boxed{4}\).
The area of the region given by \(\left\{(x, y): x y \leq 8,1 \leq y \leq x^2\right\}\) is :
If 5f(x) + 4f (\(\frac{1}{x}\)) = \(\frac{1}{x}\)+ 3, then \(18\int_{1}^{2}\) f(x)dx is:
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,
There are distinct applications of integrals, out of which some are as follows:
In Maths
Integrals are used to find:
In Physics
Integrals are used to find: