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Frank is pushing a block of 50 kg over the floor, with a force of 600 N downward and forward, making a 20Â° angle with the horizontal. The coefficient of sliding friction between the block and the floor is 0.39.

Find the *acceleration* of the block and the *friction force* acting on the block.

Let's try to sketch what is happening.

We need to draw a horizontal surface, a block on that surface, and indicate that the block is pushed by a downward-forward force that makes 20Â° with the horizontal. We also need to indicate that there is friction between the block and the floor:

Next, we look at our sketch, and try to list all the forces that act on the block.

There are 4 forces acting:

- Frank's pushing force, which we'll indicate with F
- the friction force, F
_{f} - the force of gravity, mg
- and the normal force N, which the surface exerts on the block

Knowing the forces, let's draw a free-body diagram for the block:

Let's take a step back and examine what we know, and what the need to find:

We *know* the mass of the block (50 kg), the push (600 N at 20Â° downward-forward), and the coefficient of friction (0.39).

We need to *find* the acceleration of the block and the force of friction.

m = 50 kg

F = 600 N

Î¸ = 20Â°

Î¼ = 0.39

a = ?

F_{f} = ?

Since we know the mass of the block, if we first find the resultant force, we can then apply **Newton's 2 ^{nd} Law** to get the block's acceleration.

Let's start by drawing the coordinate axes on our free-body diagram, and determine the x and y components of all the forces acting on the block.

F_{x} = F cos 20Â°

F_{fx} = âˆ’F_{f}

N_{x} = 0

mg_{x} = 0

F_{y} = âˆ’F sin 20Â°

F_{fy} = 0

N_{y} = N

mg_{y} = âˆ’mg

We can now find the x and y components of the resultant force:

x:

R_{x} = F_{x} + F_{fx} + N_{x} + mg_{x}

R_{x} = F cos 20Â° + (âˆ’F_{f}) + 0 + 0

R_{x} = F cos 20Â° âˆ’ F_{f} (1)

y:

R_{y} = F_{y} + F_{fy} + N_{y} + mg_{y}

R_{y} = (âˆ’F sin 20Â°) + 0 + N + (âˆ’mg)

R_{y} = N âˆ’ F sin 20Â° âˆ’ mg (2)

For Eq. (1) we need to find the friction force F_{f}.

By definition, the direction of the sliding friction force will be opposite to the motion of the block, and its magnitude will be equal to the product between the coefficient of sliding friction and the normal force:

F_{f} = Î¼N

We know Î¼, but we don't know N.

Where did we see N before?

We saw N in Eq. (2):

R_{y} = N âˆ’ F sin 20Â° âˆ’ mg

Since the block is moving along the floor, R_{y} must be zero (otherwise there would be a vertical acceleration):

R_{y} = 0

Therefore:

0 = N âˆ’ F sin 20Â° âˆ’ mg

The only unknown in this equation is N, so we can solve it:

0 = N âˆ’ F sin 20Â° âˆ’ mg

N âˆ’ F sin 20Â° âˆ’ mg = 0

N = F sin 20Â° + mg

Having found N, we can calculate F_{f}:

F_{f} = Î¼N

F_{f} = Î¼ (F sin 20Â° + mg)

F_{f} = (0.39) [(600 N) (sin 20Â°) + (50 kg) (9.8 N/kg)]

F_{f} = (0.39) (205 N + 490 N)

F_{f} = 270 N

Now that we know F_{f}, we can find R_{x} from Eq. (1):

R_{x} = F cos 20Â° âˆ’ F_{f}

R_{x} is positive (since the block accelerates in the positive x direction), and we have shown that R_{y} is *zero*. This means that R will have direction in the positive x axis, and its magnitude will be equal to R_{x}:

R = R_{x}

R = F cos 20Â° âˆ’ F_{f}

Now that we finally found the resultant force, let's apply **Newton's 2 ^{nd} Law** to find the acceleration of the block:

R = ma

a = | R |

m |

a = | R |

m |

a = | F cos 20Â° âˆ’ F_{f} |

m |

a = | (600 N) (cos 20Â°) âˆ’ 270 N |

50 kg |

a = | 294 N |

50 kg |

a = 5.9 N/kg = 5.9 m/s^{2}

And with that we have found everything we needed:

a = 5.9 m/s^{2}

F_{f} = 270 N

- As you may have noticed, we didn't find the value of every unknown, but only of those that were required by the problem. This is generally a good practice. The obvious advantage of this is that you use your calculator
*less often*and you*don't spend*your time finding unknowns you're not asked to find. Another advantage is that you*can see*what*relationships*exist between different variables under particular circumstances. This is useful because whenever you will encounter a similar problem, when you are in the middle of solving it, you will be able to*recognize equations*, and thus know that you're solving it correctly.

Robert is pushing a block of 61 kg over a horizontal surface. He pushes downward and forward, making an angle of 30Â° with the horizontal. Assuming that the push has magnitude 490 N, and that the coefficient of sliding friction between the block and the surface is 0.44, find the acceleration of the block, and the force of friction acting on the block.

a = 0.89 m/s^{2}

F_{f} = 370 N

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