The value of sin² 51° + sin² 39° is:
We know that \(\sin(90^\circ - x) = \cos(x)\).
Therefore, \(\sin(51^\circ) = \sin(90^\circ - 39^\circ) = \cos(39^\circ)\).
So, sin² 51° + sin² 39° = cos² 39° + sin² 39°
Using the trigonometric identity \(\sin^2(x) + \cos^2(x) = 1\), we get:
cos² 39° + sin² 39° = 1
Answer: (A) 1
Using the complementary angle identity $ \sin(90^\circ - x) = \cos x $, we have:
$$ \sin^2 51^\circ + \sin^2 39^\circ = \sin^2 51^\circ + \sin^2 (90^\circ - 51^\circ) = \sin^2 51^\circ + \cos^2 51^\circ. $$
Using the Pythagorean identity $ \sin^2 x + \cos^2 x = 1 $, we get:
$$ \sin^2 51^\circ + \cos^2 51^\circ = 1. $$
The given graph illustrates:
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly: