/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 93 The girl has a mass of \(50 \mat... [FREE SOLUTION] | 91Ó°ÊÓ

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The girl has a mass of \(50 \mathrm{~kg}\). She is seated on the horse of the merry-go-round which undergoes constant rotational motion \(\dot{\theta}=1.5 \mathrm{rad} / \mathrm{s}\). If the path of the horse is defined by \(r=4 \mathrm{~m}, z=(0.5 \sin \theta) \mathrm{m},\) determine the maximum and minimum force \(F_{z}\) the horse exerts on her during the motion.

Short Answer

Expert verified
The maximum and minimum forces the horse exerts on the girl are \(1053 \mathrm{~N}\) and \(828 \mathrm{~N}\) respectively.

Step by step solution

01

Calculate Gravitational Force

First, calculate the force due to gravity \(F_{g}\). Use the equation \(F_{g}=m \cdot g\), where \(m\) is the mass of the girl and \(g\) is the acceleration due to gravity, given as \(9.81 \mathrm{~m/s^2}\). Therefore, \(F_{g}= 50 \mathrm{~kg} \cdot 9.81 \mathrm{~m/s^2} = 490.5 \mathrm{~N}\).
02

Calculate Centripetal Force

Next, calculate the centripetal force \(F_{c}\) using the equation \(F_{c}= m \cdot r \cdot \dot{\theta}^2\), where \(r\) is the radius of rotation and \(\dot{\theta}\) is the angular velocity. Therefore, \(F_{c}= 50 \mathrm{~kg} \cdot 4 \mathrm{~m} \cdot (1.5 \mathrm{rad/s})^2 = 450 \mathrm{~N}\). This force will always be upward as it resists the gravitational force in this frame of reference.
03

Calculate Maximum and Minimum Force

The total force exerted by the horse \(F_{z}\) is the sum of the centripetal force \(F_{c}\), the gravitational force \(F_{g}\) and the force due to the vertical motion. This last force is \(m \cdot r \cdot \dot{\theta}^2 \cdot (0.5 \sin \theta)\), which can take values between \(-m \cdot r \cdot \dot{\theta}^2 / 2\) and \(m \cdot r \cdot \dot{\theta}^2 / 2\). Adding all these forces yields the maximum and minimum forces. Maximum \(F_{z}=F_{g}+F_{c}+m \cdot r \cdot \dot{\theta}^2 / 2 = 490.5 \mathrm{~N} + 450 \mathrm{~N} + 112.5 \mathrm{~N} = 1053 \mathrm{~N}\). Minimum \(F_{z}=F_{g}+F_{c}-m \cdot r \cdot \dot{\theta}^2 / 2 = 490.5 \mathrm{~N} + 450 \mathrm{~N} - 112.5 \mathrm{~N} = 828 \mathrm{~N}\).

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Key Concepts

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

Centripetal Force
When an object moves in a circular path, it experiences a force directed towards the center of the circle, known as centripetal force. This force keeps the object on its curved trajectory by continually pulling it inwards. In our merry-go-round example, which involves rotational motion, the centripetal force is calculated using the formula:\[ F_{c} = m \cdot r \cdot \dot{\theta}^2 \]where:- \( m \) is the mass of the rotating object (the girl) at 50 kg,- \( r \) is the radius of the circular path at 4 m,- \( \dot{\theta} \) is the angular velocity at 1.5 rad/s. Plug the values into the formula to find the centripetal force:\[ F_{c} = 50 \cdot 4 \cdot (1.5)^2 = 450 \text{ N} \]This force is crucial for maintaining the circular motion of objects. It doesn't act as a separate force but is the resultant of various physical forces experienced, mainly due to the tension or normal force from the path or surface.
Gravitational Force
Gravitational force is a fundamental force acting on every object with mass. It pulls objects towards the center of the Earth. For any object sitting or moving around Earth's surface, this force is always acting downwards, towards the ground. To calculate the gravitational force acting on an object, use the following equation:\[ F_{g} = m \cdot g \]where:- \( m \) represents the object's mass, - \( g \) denotes the acceleration due to gravity, roughly 9.81 m/s².For our exercise, where the girl has a mass of 50 kg, calculate:\[ F_{g} = 50 \cdot 9.81 = 490.5 \text{ N} \]This is the force exerted by the earth on the girl, pulling her downward toward the ground.
Rotational Motion
Rotational motion refers to the movement of an object around a center or an axis. Unlike linear motion, rotational motion involves movements along a circular path, so the angular position of an object is key. In a merry-go-round scenario like the one described, the entire system of the girl on the horse undergoes rotational motion as it moves about the central pivot of the ride. This motion is governed by parameters such as: - Angular velocity, which is the rate of change of angular displacement. - Radius, which is the distance from the center to the point of interest (where the girl sits). A key component of rotational motion is that every point on the rotating object follows a curved path, and thus it constantly changes direction, inducing centripetal acceleration, which is directly linked to centripetal force.
Angular Velocity
Angular velocity is a measure of the rate at which an object rotates around an axis. It's a crucial concept in rotational dynamics as it helps us understand how fast something is spinning and how often it completes a rotation.It is commonly denoted by \( \dot{\theta} \) and is measured in radians per second (rad/s), a unit that quantifies angles in terms of pi (\( \pi \)). In our exercise involving the merry-go-round, the given angular velocity is 1.5 rad/s.Angular velocity establishes a relationship with both centripetal and tangential aspects of rotational motion. It determines how frequently the object retraces its path and directly impacts centripetal force as in the formula:\[ F_{c} = m \cdot r \cdot \dot{\theta}^2 \]In the context of the merry-go-round, angular velocity remains constant, simplifying our calculations and allowing us to understand how it affects other dynamic variables involved in the rotational motion.

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Most popular questions from this chapter

A car of mass \(m\) is traveling at a slow velocity \(v_{0}\) If it is subjected to the drag resistance of the wind, which is proportional to its velocity, i.e., \(F_{D}=k v\), determine the distance and the time the car will travel before its velocity becomes \(0.5 v_{0}\). Assume no other frictional forces act on the car.

The \(300-\mathrm{kg}\) bar \(B\), originally at rest, is being towed over a series of small rollers. Determine the force in the cable when \(t=5 \mathrm{~s}\), if the motor \(M\) is drawing in the cable for a short time at a rate of \(v=\left(0.4 t^{2}\right) \mathrm{m} / \mathrm{s},\) where \(t\) is in seconds \((0 \leq t \leq 6 \mathrm{~s}) .\) How far does the bar move in \(5 \mathrm{~s} ?\) Neglect the mass of the cable, pulley, and the rollers.

A crate having a mass of \(60 \mathrm{~kg}\) falls horizontally off the back of a truck which is traveling at \(80 \mathrm{~km} / \mathrm{h}\). Determine the coefficient of kinetic friction between the road and the crate if the crate slides \(45 \mathrm{~m}\) on the ground with no tumbling along the road before coming to rest. Assume that the initial speed of the crate along the road is \(80 \mathrm{~km} / \mathrm{h}\).

A collar having a mass \(0.75 \mathrm{~kg}\) and negligible size slides over the surface of a horizontal circular rod for which the coefficient of kinetic friction is \(\mu_{k}=0.3 .\) If the collar is given a speed of \(4 \mathrm{~m} / \mathrm{s}\) and then released at \(\theta=0^{\circ}\), determine how far, \(s,\) it slides on the rod before coming to rest.

Using a forked rod, a \(0.5-\mathrm{kg}\) smooth peg \(P\) is forced to move along the vertical slotted path \(r=(0.5 \theta) \mathrm{m}\), where \(\theta\) is in radians. If the angular position of the arm is \(\theta=\left(\frac{\pi}{8} t^{2}\right) \mathrm{rad},\) where \(t\) is in seconds, determine the force of the rod on the peg and the normal force of the slot on the peg at the instant \(t=2 \mathrm{~s}\). The peg is in contact with only one edge of the rod and slot at any instant.

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