Questions: A lab student applies a force to an air puck equal to that shown in the figure at the right. If the mass of the puck is m=3.5 kg and its initial velocity is vi=0 m / s, find the puck's final velocity. (Hint: you can assume there is no friction acting on the puck)
Transcript text: 1. A lab student applies a force to an air puck equal to that shown in the figure at the right. If the mass of the puck is $m=3.5 \mathrm{~kg}$ and its initial velocity is $v_{i}=0 \mathrm{~m} / \mathrm{s}$, find the puck's final velocity. (Hint: you can assume there is no friction acting on the puck) (5 pts.)
Solution
Solution Steps
Step 1: Understanding the Problem
We need to find the final velocity of an air puck given its mass, initial velocity, and the force applied to it. The mass of the puck is \( m = 3.5 \, \text{kg} \) and the initial velocity is \( v_i = 0 \, \text{m/s} \). We assume there is no friction acting on the puck.
Step 2: Applying Newton's Second Law
Newton's second law states that the force applied to an object is equal to the mass of the object multiplied by its acceleration:
\[ F = m \cdot a \]
Step 3: Finding the Acceleration
To find the acceleration, we rearrange the equation:
\[ a = \frac{F}{m} \]
Step 4: Using Kinematic Equation
Since the initial velocity \( v_i = 0 \, \text{m/s} \), we can use the kinematic equation to find the final velocity \( v_f \):
\[ v_f = v_i + a \cdot t \]
Step 5: Integrating Force Over Time
If the force applied is not constant, we need to integrate the force over time to find the change in velocity. However, without the specific force-time function, we assume a constant force for simplicity.
Step 6: Calculating Final Velocity
Assuming a constant force \( F \) over a time \( t \), the final velocity can be calculated as:
\[ v_f = \frac{F \cdot t}{m} \]
Final Answer
Since the specific force \( F \) and time \( t \) are not provided in the problem, we cannot calculate a numerical value for the final velocity. However, the formula for the final velocity is:
\[ \boxed{v_f = \frac{F \cdot t}{m}} \]