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Two small variable-thrust jets are actuated to keep the spacecraft angular velocity about the \(z\) -axis constant at \(\omega_{0}=1.25 \mathrm{rad} / \mathrm{s}\) as the two telescoping booms are extended from \(r_{1}=1.2 \mathrm{m}\) to \(r_{2}=4.5 \mathrm{m}\) at a constant rate over a 2 -min period. Determine the necessary thrust \(T\) for each jet as a function of time where \(t=0\) is the time when the telescoping action is begun. The small \(10-\mathrm{kg}\) experiment modules at the ends of the booms may be treated as particles, and the mass of the rigid booms is negligible.

Short Answer

Expert verified
The necessary thrust is approximately 10.833 N for each jet to maintain the spacecraft's angular velocity constant.

Step by step solution

01

Understand the Problem

We need to maintain a constant angular velocity \(\omega_0 = 1.25 \mathrm{rad/s}\) while extending booms with masses at the ends. We know the initial and final radii, the mass of the objects, and the time over which extension occurs.
02

Use Conservation of Angular Momentum

The angular momentum \(L\) of the system is conserved. Initially, \(L = 2mr_1^2\omega_0\). As the radii change, at time \(t\), \(r(t) = r_1 + \frac{(r_2 - r_1)t}{T_{total}}\). Hence, at time \(t\), \(L = 2m[r(t)]^2\omega_0\).
03

Calculate Change in Angular Momentum

Thus, for angular momentum conservation: \(2mr_1^2\omega_0 = 2m[r(t)]^2\omega_0 + \Delta L\). Since \(\Delta L = r(t)^2 \cdot dm/dt \cdot \omega_0\) with negligible \(dm/dt\), differentiate \((2m[r(t)]^2)\) with respect to time.
04

Find Necessary Torque

Torque \(\tau = \frac{dL}{dt} = \text{net force} \times r(t)\). Thus, \(\tau = 2m\cdot\omega_0 \cdot \frac{d[r(t)]^2}{dt}\). We then differentiate \(r(t)^2\) with respect to time: \(2r(t)\frac{dr(t)}{dt}\).
05

Relate Torque to Thrust Force

The force exerted by the jets, or thrust \(T\), provides the torque: \(T \times r(t) = 2m\omega_0\cdot2r(t)\frac{dr(t)}{dt}\). Solve for \(T\): \[ T(t) = \frac{4m\omega_0}{r(t)} \cdot r(t) \cdot \frac{dr(t)}{dt} = 4m\omega_0\frac{(r_2 - r_1)}{T_{total}} \].
06

Substitute and Simplify

Substitute values: \(m = 10 \text{kg}, r_1 = 1.2 \text{m}, r_2 = 4.5 \text{m}, \omega_0 = 1.25 \text{rad/s}, T_{total} = 120 \text{s}\). Substitution gives \[ T(t) = \frac{4 \times 10 \times 1.25 \times (4.5 - 1.2)}{120} \approx 10.833\text{ N} \].

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Key Concepts

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

Variable-Thrust Jets
Variable-thrust jets are used in aerospace applications to control the movement and orientation of spacecraft. These jets provide a force, known as thrust, that can be varied according to the spacecraft's needs. This adaptability is essential in tasks such as maintaining a constant angular velocity during complex maneuvers, where conditions can change rapidly.
In our problem, variable-thrust jets are tasked with ensuring that the spacecraft's angular velocity remains constant while telescoping booms extend outward. This involves adjusting the thrust dynamically, as the spacecraft's moment of inertia changes with the extension of the booms. The thrust needs to be calculated over time to balance the varying moment of inertia and maintain a constant angular velocity. Because the jets' thrust can be adjusted continuously, it makes them highly effective in achieving precise spacecraft control.
This variable thrust compensates for changes in angular momentum, which would otherwise alter the spacecraft's rotation. A proper understanding of how these jets function can help in designing systems that ensure stability and precision in space operations.
Angular Velocity
Angular velocity is a measure of how quickly an object is rotating around a particular axis. It is an important concept in rotational dynamics, as it helps in determining how fast an object spins. In our exercise, the angular velocity is denoted as \( \omega_0 = 1.25 \, \text{rad/s} \), which means the spacecraft rotates 1.25 radians per second around the z-axis.
Understanding angular velocity is crucial in scenarios where the rotational speed needs to be maintained constantly, such as in our exercise. When booms extend, the distribution of mass changes, which can affect the angular velocity if not controlled effectively.
The spacecraft's angular velocity needs to remain consistent to avoid destabilization. This is where variable-thrust jets become important as they adjust the forces applied to ensure that the rate of rotation does not fluctuate despite the changes in geometry and mass distribution. Maintaining a constant angular velocity ensures that the spacecraft remains predictable and stable in its movement.
Torque in Dynamics
Torque is a fundamental concept in dynamics and physics, defined as the force that causes an object to rotate around an axis. In the context of our exercise, it is the force provided by the jets that allows us to manage changes in angular momentum as the spacecraft's booms extend.
The torque required to maintain a constant angular velocity is computed from the change in the rotational dynamics of the system. This is articulated in the solution, where torque \( \tau \) is shown as the product of the mass, angular velocity, and the rate of change of the radius squared from the center of rotation (i.e., as the booms extend).
Understanding torque helps us recognize why varying thrust is needed. When there's any alteration in the system's components, such as extending booms, the jets provide the incremental changes in force needed to compute that torque and balance the system's rotation. Thus, calculating this torque is essential in determining the necessary thrust each jet should exert over time, ensuring that the desired angular velocity remains unchanged.

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Most popular questions from this chapter

The semicircular disk of mass \(m\) and radius \(r\) is released from rest at \(\theta=0\) and rotates freely in the vertical plane about its fixed bearing at \(O .\) Derive expressions for the \(n\) - and \(t\) -components of the force \(F\) on the bearing as functions of \(\theta\)

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