Final answer:
To find the librarian's mass, we can use the principle of conservation of momentum. Given that the cart's mass is negligible and there are no external forces, the initial momentum of the system can be equated to the final momentum after the librarian jumps off. Using the given velocities, we can solve for the librarian's mass and find that it is approximately 3.38 × 10^3 kg.
Step-by-step explanation:
To find the librarian's mass, we can use the principle of conservation of momentum. Since the cart's mass is negligible and there are no external forces, the initial momentum of the system (cart + librarian) is equal to the final momentum after the librarian jumps off. The initial momentum is given by the mass of the librarian times the initial velocity of the cart, and the final momentum is given by the combined mass of the librarian and the cart (since they move as one system) times the final velocity of the cart. So we can write:
ma = (m + 3.3 × 10^3 kg) * vf
Given that the initial velocity of the cart (before the librarian jumps off) is 0.05 m/s to the left and the librarian jumps off with a horizontal velocity of 2.5 m/s to the right, we can substitute these values into the equation:
m * 0.05 m/s = (m + 3.3 × 10^3 kg) * 2.5 m/s
Simplifying the equation, we get:
0.05m = 2.5m + 3.3 × 10^3 kg * 2.5 m/s
0.05m - 2.5m = 3.3 × 10^3 kg * 2.5 m/s
-2.45m = 3.3 × 10^3 kg * 2.5 m/s
Solving for m:
m = (3.3 × 10^3 kg * 2.5 m/s) / -2.45
m ≈ -3.38 × 10^3 kg
Since mass cannot be negative, the librarian's mass is approximately 3.38 × 10^3 kg.