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Apparent Weight. A \(550 \mathrm{~N}\) physics student stands on a bathroom scale in an elevator that is supported by a cable. The combined mass of student plus elevator is \(850 \mathrm{~kg}\). As the elevator starts moving, the scale reads \(450 \mathrm{~N}\). (a) Find the acceleration of the elevator (magnitude and direction). (b) What is the acceleration if the scale reads \(670 \mathrm{~N}\) ? (c) If the scale reads zero, should the student worry? Explain. (d) What is the tension in the cable in parts (a) and (c)?

Short Answer

Expert verified
For Part (a), the acceleration is downwards and approximately \(1.18\) m/s². For Part (b), the acceleration is upwards and is roughly \(0.64\) m/s². For Part (c), the student should worry as the elevator could be in free-fall or in space without any gravity. For Part (d), the tension in the cable is roughly \(5300\) N when the scale reads \(450 \mathrm{~N}\) and it is zero when the scale reads zero.

Step by step solution

01

Find the Acceleration for Part (a)

Firstly, find the real weight of the student plus the elevator, which is the product of the mass and gravitational acceleration. This can be done by the formula: \(W = m \cdot g\). Here, \(m = 850\) kg and \(g = 9.8\) m/s². Secondly, apparent weight is the force the scale reads, which can be found using the formula for net force \(F_{net} = m \cdot a\). Therefore, acceleration \(a = \frac{F_{net}}{m}\). Use the given force of 450N for \(F_{net}\) to calculate \(a\).
02

Find the Acceleration for Part (b)

Similarly, calculate the acceleration \(a\) using the formula mentioned above. But this time, use the given force of 670N for \(F_{net}\).
03

Analysis for Part (c)

If the scale reads zero, it means the apparent weight of the student is zero. This happens only in two cases - when the elevator is free-falling or when it's in space without any gravity. In both cases, the student should worry.
04

Calculate the Tension for Part (d)

Find the tension in the cable which supports the elevator by using the force equation, \( \Sigma F = m \cdot a \). The forces involved here are the weight downward and the tension upward. i. When the scale reads 450N (Part a),you have: \[ T - W = m \cdot a \] \[ T = m \cdot a + W \]Extract the calculated acceleration from Step 1 and substitute into the equation to find \( T \).ii. When the scale reads 0N (Part c), the elevator is in free fall. Hence, \( a = g \). Substitute into the equation to calculate \( T \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Newton's Second Law
Newton's Second Law of Motion is a fundamental principle in physics that tells us how the motion of an object changes when it is subjected to an external force. The law states that the force acting on an object is equal to the mass of the object multiplied by its acceleration. This can be mathematically expressed as:\[ F = m \cdot a \]Where:
  • \( F \) is the net force acting on the object.
  • \( m \) represents the mass of the object.
  • \( a \) is the acceleration produced.
In the context of an elevator situation, we apply this law to find the acceleration based on changes in apparent weight. The apparent weight is what the scale reads and can differ from the actual weight when the elevator is accelerating. By understanding that the apparent weight represents the net force, we can rearrange the formula to solve for acceleration:\[ a = \frac{F_{net}}{m} \]This re-arrangement assists in determining the difference in force measured by a scale while taking into account the direction and magnitude of the elevator’s movement.
Elevator Physics
Elevator physics deals with how forces interact within an elevator scenario, especially concerning apparent weight. Apparent weight refers to the force a person feels due to acceleration; it's the weight that scales register. When standing on a scale in a moving elevator, what you feel is not just your body weight but the net effect of all forces, including the movement of the elevator.For instance:
  • When the elevator accelerates upwards, you feel heavier because the force of acceleration adds to your weight.
  • When it accelerates downwards, you feel lighter since the force of acceleration acts against your weight.
Understanding these changes in apparent weight helps explain scenarios observed in the exercise, such as when the scale reads 450N or 670N. It represents how different accelerations influence the reading, allowing us to calculate the corresponding accelerations using:\[ F_{net} = \text{apparent weight} - ext{actual weight} \]These dynamics also explain why the reading might be zero, suggesting either free fall or absence of gravity, situations that should certainly concern a person in a real-world context!.
Tension in Physics
Tension within a cable in an elevator scenario describes the force exerted to keep the elevator moving in a desired manner. When determining tension, consider both the force due to gravity and the force due to acceleration.The formula for tension in the elevator cable is:\[ T = m \cdot g + m \cdot a \]Where:
  • \( T \) is the tension in the cable.
  • \( m \) is the total mass supported by the cable.
  • \( g \) is the acceleration due to gravity, typically \(9.8 \text{ m/s}^2\).
  • \( a \) is the elevator's acceleration.
In the exercise:- When the elevator has an acceleration derived from the 450N reading, you can compute the tension by substituting the acceleration back into the formula.- When the scale reads zero (implying free fall), this greatly reduces tension on the cable, calculated by recognizing that in free fall, the acceleration equals \( g \), leading to minimal tension.Understanding tension is crucial in maintaining the safety and functionality of elevators, keeping the forces balanced and ensuring smooth operation.

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Most popular questions from this chapter

An \(8.00 \mathrm{~kg}\) box sits on a ramp that is inclined at \(33.0^{\circ}\) above the horizontal. The coefficient of kinetic friction between the box and the surface of the ramp is \(\mu_{\mathrm{k}}=0.300 .\) A constant horizontal force \(F=26.0 \mathrm{~N}\) is applied to the box (Fig. \(\mathbf{P} 5.73),\) and the box moves down the ramp. If the box is initially at rest, what is its speed \(2.00 \mathrm{~s}\) after the force is applied?

DATA You are an engineer working for a manufacturing company. You are designing a mechanism that uses a cable to drag heavy metal blocks a distance of \(8.00 \mathrm{~m}\) along a ramp that is sloped at \(40.0^{\circ}\) above the horizontal. The coefficient of kinetic friction between these blocks and the incline is \(\mu_{\mathrm{k}}=0.350 .\) Each block has a mass of \(2170 \mathrm{~kg}\). The block will be placed on the bottom of the ramp, the cable will be attached, and the block will then be given just enough of a momentary push to overcome static friction. The block is then to accelerate at a constant rate to move the \(8.00 \mathrm{~m}\) in \(4.20 \mathrm{~s}\). The cable is made of wire rope and is parallel to the ramp surface. The table gives the breaking strength of the cable as a function of its diameter; the safe load tension, which is \(20 \%\) of the breaking strength; and the mass per meter of the cable: $$ \begin{array}{cccc} \begin{array}{c} \text { Cable Diameter } \\ \text { (in.) } \end{array} & \begin{array}{c} \text { Breaking Strength } \\ (\mathbf{k N}) \end{array} & \begin{array}{c} \text { Safe Load } \\ (\mathbf{k N}) \end{array} & \begin{array}{c} \text { Mass per Meter } \\ (\mathbf{k g} / \mathbf{m}) \end{array} \\ \hline \frac{1}{4} & 24.4 & 4.89 & 0.16 \\ \frac{3}{8} & 54.3 & 10.9 & 0.36 \\ \frac{1}{2} & 95.2 & 19.0 & 0.63 \\ \frac{5}{8} & 149 & 29.7 & 0.98 \\ \frac{3}{4} & 212 & 42.3 & 1.41 \\ \frac{7}{8} & 286 & 57.4 & 1.92 \\ 1 & 372 & 74.3 & 2.50 \\ \hline \end{array} $$ (a) What is the minimum diameter of the cable that can be used to pull a block up the ramp without exceeding the safe load value of the tension in the cable? Ignore the mass of the cable, and select the diameter from those listed in the table. (b) You need to know safe load values for diameters that aren't in the table, so you hypothesize that the breaking strength and safe load limit are proportional to the cross-sectional area of the cable. Draw a graph that tests this hypothesis, and discuss its accuracy. What is your estimate of the safe load value for a cable with diameter \(\frac{9}{16}\) in.? (c) The coefficient of static friction between the crate and the ramp is \(\mu_{\mathrm{s}}=0.620,\) which is nearly twice the value of the coefficient of kinetic friction. If the machinery jams and the block stops in the middle of the ramp, what is the tension in the cable? Is it larger or smaller than the value when the block is moving? (d) Is the actual tension in the cable, at its upper end, larger or smaller than the value calculated when you ignore the mass of the cable? If the cable is \(9.00 \mathrm{~m}\) long, how accurate is it to ignore the cable's mass?

Block \(B,\) with mass \(5.00 \mathrm{~kg},\) rests on block \(A,\) with mass \(8.00 \mathrm{~kg}\), which in turn is on a horizontal tabletop (Fig. P5.92). There is no friction between block \(A\) and the tabletop, but the coefficient of static friction between blocks \(A\) and \(B\) is \(0.750 .\) A light string attached to block \(A\) passes over a friction less, massless pulley, and block \(C\) is suspended from the other end of the string. What is the largest mass that block \(C\) can have so that blocks \(A\) and \(B\) still slide together when the system is released from rest?

A racetrack curve has radius \(120.0 \mathrm{~m}\) and is banked at an angle of \(18.0^{\circ} .\) The coefficient of static friction between the tires and the roadway is \(0.300 .\) A race car with mass \(900 \mathrm{~kg}\) rounds the curve with the minimum speed needed to not slide down the banking. (a) As the car rounds the curve, what is the normal force exerted on it by the road? (b) What is the car's speed?

\(\mathrm{CP}\) A \(5.00 \mathrm{~kg}\) box sits at rest at the bottom of a ramp that is \(8.00 \mathrm{~m}\) long and is inclined at \(30.0^{\circ}\) above the horizontal. The coefficient of kinetic friction is \(\mu_{\mathrm{k}}=0.40,\) and the coefficient of static friction is \(\mu_{\mathrm{s}}=0.43 .\) What constant force \(F,\) applied parallel to the surface of the ramp, is required to push the box to the top of the ramp in a time of \(6.00 \mathrm{~s} ?\)

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