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chapter 5 forces in two dimensions practice problems lesson 2 friction …

Question

chapter 5 forces in two dimensions practice problems
lesson 2 friction
example problem 3 - balanced friction forces

  1. owen exerts a 36 - n horizontal force as she pulls a 52 - n sled across a cement sidewalk at constant speed. what is the coefficient of kinetic friction between the sidewalk and the metal sled runners? ignore air resistance.
  2. mr. ames is dragging a box full of books from his office to his car. the box and books together have a combined weight of 134 n. if the coefficient of static friction between the pavement and the box is 0.55, how hard must mr. ames push horizontally on the box in order to start it moving?
  3. thomas sits on a small rug on a polished wooden floor. the coefficient of kinetic friction between the rug and the slippery wooden floor is only 0.12. if thomas weighs 650 n, what horizontal force is needed to pull the rug and thomas across the floor at a constant speed?
  4. you want to move a 41 - kg bookcase to a different place in the living room. if you push with a force of 65 n and the bookcase accelerates at 0.12 m/s², what is the coefficient of kinetic friction between the bookcase and the carpet?
  5. consider the force pushing the box in example problem 4. how long would it take for the velocity of the box to double to 2.0 m/s?
  6. ke min is driving at 23 m/s. he sees a tree branch lying across the road. he slams on the brakes when the branch is 60.0 m in front of him. if the coefficient of kinetic friction between the cars locked tires and the road is 0.41, will the car stop before hitting the branch? the car has a mass of 1200 kg.

Explanation:

Response

1.

Step1: Analyze forces at constant - speed

Since the sled is moving at a constant speed, the net force in the horizontal direction is zero. The horizontal force $F = 36N$ is equal to the kinetic - friction force $F_f$. The weight of the sled $W = 52N$, and the normal force $N$ on the sled is equal to its weight ($N = W$) because there is no acceleration in the vertical direction. The formula for kinetic - friction force is $F_f=\mu_kN$.
$F = F_f=\mu_kN$ and $N = W$, so $\mu_k=\frac{F}{N}=\frac{F}{W}$.

Step2: Calculate the coefficient of kinetic friction

Substitute $F = 36N$ and $W = 52N$ into the formula: $\mu_k=\frac{36}{52}\approx0.69$.

Step1: Determine the normal force

The combined weight of the box and books is $W = 134N$. The normal force $N$ on the box is equal to its weight ($N = W$) since there is no acceleration in the vertical direction.

Step2: Calculate the static - friction force

The formula for static - friction force is $F_{s,max}=\mu_sN$. Substitute $\mu_s = 0.55$ and $N = 134N$ into the formula: $F_{s,max}=0.55\times134 = 73.7N$. To start the box moving, the applied force must be at least equal to the maximum static - friction force.

Step1: Determine the normal force

The weight of Thomas is $W = 650N$. The normal force $N$ on the rug (which supports Thomas) is equal to his weight ($N = W$) since there is no acceleration in the vertical direction.

Step2: Calculate the kinetic - friction force

The formula for kinetic - friction force is $F_f=\mu_kN$. Substitute $\mu_k = 0.12$ and $N = 650N$ into the formula: $F_f=0.12\times650 = 78N$. Since the rug and Thomas are moving at a constant speed, the net force in the horizontal direction is zero, and the applied horizontal force $F$ is equal to the kinetic - friction force $F_f$.

Answer:

$\mu_k\approx0.69$

2.