Determine the distance to which the 90 kg painter can climb without causing the 4 m ladder to slip at its lower end A as shown in Figure 1. The top of the 15 kg ladder has a smaller roller, and at the ground the coefficient of static friction is 0.25. The mass center of the painter is directly above his feet.

To determine the distance to which the 90 kg painter can climb without causing the ladder to slip at its lower end, we need to consider the forces acting on the ladder.

First, let's find the normal force, which is the force exerted by the ground on the ladder. The normal force is equal to the weight of the ladder, which is the sum of the weight of the 90 kg painter (90 kg * 9.8 m/s^2) and the weight of the 15 kg ladder (15 kg * 9.8 m/s^2).

Weight of the painter = 90 kg * 9.8 m/s^2 = 882 N
Weight of the ladder = 15 kg * 9.8 m/s^2 = 147 N

Therefore, the total weight of the ladder is 882 N + 147 N = 1029 N.

Now, let's consider the forces that might cause the ladder to slip. There are two forces at play: the force of static friction and the force of gravity pulling down the ladder.

The force of gravity pulling down the ladder can be split into two components: one that is perpendicular to the ladder's surface and one that is parallel to the surface. The perpendicular component contributes to the normal force, while the parallel component can cause the ladder to slip.

The perpendicular component of the force of gravity is equal to the weight of the ladder (1029 N), and it is balanced by the normal force exerted by the ground.

The parallel component of the force of gravity is equal to the weight of the ladder multiplied by the sine of the angle between the ladder and the ground (let's call this angle θ). The maximum angle θ that the ladder can make with the ground without slipping is determined by the coefficient of static friction.

The formula for the force of static friction is F(static friction) = μ(static friction) * N, where μ(static friction) is the coefficient of static friction and N is the normal force.

In this case, μ(static friction) = 0.25 and N = 1029 N.

Therefore, the maximum parallel component of the force of gravity is F(static friction) = 0.25 * 1029 N = 257.25 N.

The maximum angle θ that the ladder can make with the ground without slipping can be determined by taking the inverse sine of the ratio of the maximum parallel component of the force of gravity to the weight of the ladder:

sin(θ) = (maximum parallel component of gravity) / (weight of ladder)
sin(θ) = 257.25 N / 1029 N

Solving for θ, we find that θ ≈ 0.249 radians (or approximately 14.27 degrees).

Now, to determine the distance to which the painter can climb, we need to consider the ladder's length (4 meters) and the change in height as the painter climbs.

Let's assume the painter climbs up a vertical distance of h meters. In this case, the horizontal distance the painter can climb will be 4 * tan(θ).

So, if the painter climbs up a vertical distance of h meters, the horizontal distance can be calculated as 4 * tan(θ):

Horizontal distance = 4 m * tan(θ) = 4 m * tan(0.249) ≈ 0.963 m.

Therefore, the painter can climb horizontally up to a distance of approximately 0.963 meters without causing the ladder to slip at its lower end.