Given: Right-angled triangle \( \Delta ABC \) with right angle at \( C \).
Step 1: Label the sides.
Let:
Step 2: Express \(\tan A\) and \(\tan B\).
\[ \tan A = \frac{\text{opposite}}{\text{adjacent}} = \frac{a}{b} \] \[ \tan B = \frac{\text{opposite}}{\text{adjacent}} = \frac{b}{a} \]
Step 3: Compute \(\tan A + \tan B\).
\[ \tan A + \tan B = \frac{a}{b} + \frac{b}{a} = \frac{a^2 + b^2}{ab} \]
Step 4: Apply Pythagorean theorem.
\[ a^2 + b^2 = c^2 \Rightarrow \tan A + \tan B = \frac{c^2}{ab} \]
Option Analysis:
(A) \( a + b \) - Incorrect (sum of sides, not tangent sum)
(B) \( \frac{a^2}{bc} \) - Incorrect form
(C) \( \frac{c^2}{ab} \) - Correct (matches our derivation)
(D) \( \frac{b^2}{ac} \) - Incorrect form
Final Answer: \(\boxed{C}\)
In a right-angled triangle \( \triangle ABC \), right-angled at \( C \), we have:
\[ \tan A = \frac{a}{c}, \quad \tan B = \frac{b}{a} \]
Therefore,
\[ \tan A + \tan B = \frac{a}{c} + \frac{b}{a} = \frac{a^2 + bc}{ac} \]
Using the trigonometric identities in a right-angled triangle:
\[ a = c \sin A, \quad b = c \cos A, \quad \tan A = \frac{a}{b}, \quad \tan B = \frac{b}{a} \] \[ \tan A + \tan B = \frac{a}{b} + \frac{b}{a} = \frac{a^2 + b^2}{ab} \]
Since the triangle is right-angled at \( C \), we have \( a^2 + b^2 = c^2 \) (Pythagorean theorem).
\[ \tan A + \tan B = \frac{c^2}{ab} \]
So the correct expression for \( \tan A + \tan B \) is indeed \( \frac{c^2}{ab} \).
Final Answer: The final answer is \( {\frac{c^2}{ab}} \).
The given graph illustrates:
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:
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