We are given the following probabilities: \[ P(A) = 0.59, \quad P(B) = 0.30, \quad P(A \cap B) = 0.21 \] The probability of the complement \( P(A' \cap B') \), i.e., the probability that neither A nor B occurs, is given by the formula: \[ P(A' \cap B') = 1 - P(A \cup B) \] Using the formula for the union of two sets: \[ P(A \cup B) = P(A) + P(B) - P(A \cap B) \] Substituting the known values: \[ P(A \cup B) = 0.59 + 0.30 - 0.21 = 0.68 \] Therefore: \[ P(A' \cap B') = 1 - 0.68 = 0.32 \]
We are given that P(A) = 0.59, P(B) = 0.30, and P(A ∩ B) = 0.21.
We need to find P(A' ∩ B').
By De Morgan's Law, we know that \(A' ∩ B' = (A ∪ B)'\). Therefore, \(P(A' ∩ B') = P((A ∪ B)')\).
We also know that \(P((A ∪ B)') = 1 - P(A ∪ B)\).
The formula for \(P(A ∪ B)\) is \(P(A ∪ B) = P(A) + P(B) - P(A ∩ B)\).
Substituting the given values, we get \(P(A ∪ B) = 0.59 + 0.30 - 0.21 = 0.89 - 0.21 = 0.68\).
Now, we can find \(P(A' ∩ B') = 1 - P(A ∪ B) = 1 - 0.68 = 0.32\).
Therefore, P(A' ∩ B') = 0.32.
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: