\( \dfrac{1}{4} \)
To find the probability \( P(T) \), we start by considering the definition of each event and how they interrelate:
We have the following probabilities given:
Since \( U \) is the event that at least one of the students can solve the problem, we also have the complementary event \( \bar{U} \), which is that none can solve it.
The probability of \( U \) can be broken down as:
\( P(U) = 1 - P(\bar{U}) = 1 - \left( 1-P(T)-P(V)-P(W) \right) \)
Rearranging, we get:
\( P(U) = 1 - \left( 1 - P(T) - \frac{1}{10} - \frac{1}{12} \right) \)
We simplify the equation knowing \( P(U) = \frac{1}{2} \):
\( \frac{1}{2} = 1 - \left( 1 - P(T) - \frac{1}{10} - \frac{1}{12} \right) \)
\( \frac{1}{2} = P(T) + \frac{1}{10} + \frac{1}{12} \)
We need a common denominator to add the fractions. The least common multiple of 10 and 12 is 60:
\( \frac{1}{2} = P(T) + \frac{6}{60} + \frac{5}{60} \)
\( \frac{1}{2} = P(T) + \frac{11}{60} \)
Express \( \frac{1}{2} \) as \( \frac{30}{60} \) to have a common denominator:
\( \frac{30}{60} = P(T) + \frac{11}{60} \)
Subtract \( \frac{11}{60} \) from both sides:
\( P(T) = \frac{30}{60} - \frac{11}{60} = \frac{19}{60} \)
Therefore, the probability \( P(T) \) is: \( \frac{19}{60} \)
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
A temperature difference can generate e.m.f. in some materials. Let $ S $ be the e.m.f. produced per unit temperature difference between the ends of a wire, $ \sigma $ the electrical conductivity and $ \kappa $ the thermal conductivity of the material of the wire. Taking $ M, L, T, I $ and $ K $ as dimensions of mass, length, time, current and temperature, respectively, the dimensional formula of the quantity $ Z = \frac{S^2 \sigma}{\kappa} $ is: