You need to push as much as the force of friction is.
You should push with a force equal to the force of friction acting on the crate. This will counteract the friction force and allow the crate to continue moving at a constant velocity. Pushing with a greater force will accelerate the crate, while pushing with a force lower than the frictional force will cause it to decelerate.
It is more difficult to slide a crate starting from rest because static friction exists between the crate and the surface, requiring a greater force to overcome. Once the crate is already sliding, kinetic friction is less than static friction, making it easier to keep moving with a lower force.
The net force on the crate sliding at a constant speed is zero. This is because the applied force of 75 N is balanced by the frictional force opposing the motion. As a result, the crate does not accelerate, and the net force is zero.
The acceleration of the crate will be zero since it is moving at a constant speed. This means that the net force acting on the crate is zero, so the forces pushing it forward are balanced by the forces resisting its motion.
The force of friction acting on a crate sliding across the floor is equal in magnitude but opposite in direction to the force applied to move the crate. It depends on the coefficient of friction between the crate and the floor, as well as the weight of the crate.
If the crate is in dynamic equilibrium, the frictional force acting on it is equal in magnitude but opposite in direction to the applied force. Therefore, the frictional force acting on the crate is also 140 N.
To someone on the airplane, the crate would appear to fall straight down due to its initial horizontal velocity matching the airplane's speed. To someone on the ground, the crate would follow a parabolic path because of gravity acting on it vertically while it moves horizontally due to its initial velocity.
If the crate is in dynamic equilibrium, the frictional force acting on it is equal in magnitude but opposite in direction to the applied force. Therefore, the frictional force acting on the crate is also 140 N.
The acceleration of the crate will be zero since it is moving at a constant speed. This means that the net force acting on the crate is zero, so the forces pushing it forward are balanced by the forces resisting its motion.
The direction of friction on the crate is opposite to the direction in which it is sliding. In this case, since you are pushing the crate to the right, the friction will act to the left in order to oppose the motion.
In my opinion you should start with the dog crate next to you, and start moving it away from you little by little.
The net force on the crate sliding at a constant speed is zero. This is because the applied force of 75 N is balanced by the frictional force opposing the motion. As a result, the crate does not accelerate, and the net force is zero.
To determine the speed of the crate after 6 seconds, we first need to calculate the net force acting on the crate on the inclined plane. This can be done by resolving the weight of the crate into components parallel and perpendicular to the plane. Then, using Newton's second law, F = ma, where F is the net force, m is the mass of the crate, and a is the acceleration, we can find the acceleration down the incline. After finding this acceleration, we can use the kinematic equation v = u + at to calculate the final speed of the crate after 6 seconds, where v is the final velocity, u is the initial velocity (assumed to be 0), a is the acceleration, and t is the time.
not on the car because they are not moving at the same speed
No, the crate being stationary on an incline does not necessarily mean it is in equilibrium. Equilibrium requires not only that the crate is stationary but also that the forces acting on it are balanced. Without knowing the exact forces acting on the crate, we cannot conclude that it is in equilibrium.
If the box is sliding at a constant speed, the net force on the box is zero. The force of friction (100N) is balanced by an equal and opposite force exerted on the box to keep it moving at a constant speed.
80%
The force of static friction acts to prevent the crate from moving when at rest. To overcome this force and start the crate moving, a force larger than the force of static friction must be applied. The force required to get the crate moving can be calculated as the product of the coefficient of static friction and the weight of the crate, which is 40 kg * 9.8 m/s^2 = 392 N. So, the horizontal force required would be 0.69 * 392 N = 270.48 N.