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F net = m a .

From the free-body diagram, we see that F net = F s w , so we have

F s w = m a .

Solving for F s gives us an equation with only one unknown:

F s = m a + w ,

or, because w = m g , simply

F s = m a + m g .

No assumptions were made about the acceleration, so this solution should be valid for a variety of accelerations in addition to those in this situation. ( Note: We are considering the case when the elevator is accelerating upward. If the elevator is accelerating downward, Newton’s second law becomes F s w = m a . )

Solution

  1. We have a = 1.20 m/s 2 , so that
    F s = ( 75.0 kg ) ( 9.80 m/s 2 ) + ( 75.0 kg ) ( 1.20 m/s 2 )

    yielding
    F s = 825 N .
  2. Now, what happens when the elevator reaches a constant upward velocity? Will the scale still read more than his weight? For any constant velocity—up, down, or stationary—acceleration is zero because a = Δ v Δ t and Δ v = 0 . Thus,
    F s = m a + m g = 0 + m g

    or
    F s = ( 75.0 kg ) ( 9.80 m/s 2 ) ,

    which gives
    F s = 735 N .

Significance

The scale reading in [link] (a) is about 185 lb. What would the scale have read if he were stationary? Since his acceleration would be zero, the force of the scale would be equal to his weight:

F net = m a = 0 = F s w
F s = w = m g
F s = ( 75.0 kg ) ( 9.80 m/s 2 ) = 735 N .

Thus, the scale reading in the elevator is greater than his 735-N (165-lb.) weight. This means that the scale is pushing up on the person with a force greater than his weight, as it must in order to accelerate him upward. Clearly, the greater the acceleration of the elevator, the greater the scale reading, consistent with what you feel in rapidly accelerating versus slowly accelerating elevators. In [link] (b), the scale reading is 735 N, which equals the person’s weight. This is the case whenever the elevator has a constant velocity—moving up, moving down, or stationary.

Check Your Understanding Now calculate the scale reading when the elevator accelerates downward at a rate of 1.20 m/s 2 .

F s = 645 N

Got questions? Get instant answers now!

The solution to the previous example also applies to an elevator accelerating downward, as mentioned. When an elevator accelerates downward, a is negative, and the scale reading is less than the weight of the person. If a constant downward velocity is reached, the scale reading again becomes equal to the person’s weight. If the elevator is in free fall and accelerating downward at g , then the scale reading is zero and the person appears to be weightless.

Two attached blocks

[link] shows a block of mass m 1 on a frictionless, horizontal surface. It is pulled by a light string that passes over a frictionless and massless pulley. The other end of the string is connected to a block of mass m 2 . Find the acceleration of the blocks and the tension in the string in terms of m 1 , m 2 , and g .

(a)  Block m sub 1 is on a horizontal surface. It is connected to a string that passes over a pulley then hangs straight down and connects to  block m sub 2. Block m sub 1 has acceleration a sub 1 directed to the right. Block m sub 2 has acceleration a sub 2 directed downward. (b) Free body diagrams of each block. Block m sub 1 has force w sub 1 directed vertically down, N directed vertically up, and T directed horizontally to the right. Block m sub 2 has force w sub 2 directed vertically down, and T directed vertically up. The x y coordinate system has positive x to the right and positive y up.
(a) Block 1 is connected by a light string to block 2. (b) The free-body diagrams of the blocks.

Strategy

We draw a free-body diagram for each mass separately, as shown in [link] . Then we analyze each one to find the required unknowns. The forces on block 1 are the gravitational force, the contact force of the surface, and the tension in the string. Block 2 is subjected to the gravitational force and the string tension. Newton’s second law applies to each, so we write two vector equations:

Questions & Answers

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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