To solve the problem, we need to prove that \( a^{\log_b c} - c^{\log_b a} = 0 \) using logarithmic identities.
1. Define the Initial Expression:
Let \( y = c \log_b a \). This represents a logarithmic relationship between the variables.
2. Take the Logarithm of Both Sides:
Taking the logarithm (base \( c \)) on both sides:
\( \log_c y = \log_b a \).
3. Apply the Change of Base Formula:
Using the logarithmic identity \( \log_k m = \frac{\log m}{\log k} \), we convert both sides to natural logarithms (or base-10):
\( \frac{\log y}{\log c} = \frac{\log a}{\log b} \).
4. Rearrange the Equation:
Cross-multiply to isolate \( \log y \):
\( \frac{\log y}{\log a} = \frac{\log c}{\log b} \).
5. Rewrite in Logarithmic Form:
This implies \( \log_a y = \log_b c \), which means \( y = a^{\log_b c} \).
6. Substitute Back the Original Expression:
Since \( y = c \log_b a \), we substitute to get:
\( c \log_b a = a^{\log_b c} \).
7. Prove the Given Identity:
By symmetry, \( c^{\log_b a} = a^{\log_b c} \).
Therefore: \( a^{\log_b c} - c^{\log_b a} = 0 \).
Final Answer:
The proof shows that \( \boxed{a^{\log_b c} - c^{\log_b a} = 0} \).
We are given the expression \( a^{\log_b c} - c^{\log_b a} \).
Let's simplify it step by step.
First, recall the logarithmic identity that \( a^{\log_b c} = c^{\log_b a} \), which is a general property of logarithms. Therefore, the given expression becomes: \[ a^{\log_b c} - c^{\log_b a} = 0. \]
Thus, the value of the given expression is 0.
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: