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Starting at \(t=0\). a horizontal net externul force \(F=(0.280 \mathrm{~N} / \mathrm{s}) t \hat{\imath}+\left(-0.450 \mathrm{~N} / \mathrm{s}^{2}\right) r^{2} \hat{\jmath}\) is applied to a box that has an initial momentum \(\vec{p}=(-3.00 \mathrm{~kg} \cdot \mathrm{m} / \mathrm{s}) \hat{\imath}+(4.00 \mathrm{~kg} \cdot \mathrm{m} / \mathrm{s}) \hat{\jmath} .\) What is the momentum of the box at \(t=2.00 \mathrm{~s} ?\)

Short Answer

Expert verified
The momentum of the box at \(t=2.00 s\) is \(-2.44 kg*m/s * \hat{\imath} + 2.80 kg*m/s * \hat{\jmath}\).

Step by step solution

01

Find Force Integral for the i-hat Component

The force in the i-hat direction is \(0.280 N/s * t\). Integrate this function with respect to time from 0 to 2 seconds. The integral of t with respect to t is \(0.5*t^2\), so when calculated between 0 and 2 seconds, the integral becomes \(0.5 * 2^2 * 0.280 N/s = 0.560 N * s\).
02

Calculate i-hat Momentum

The i-hat component of momentum is the initial momentum plus the change in momentum caused by the external force. The initial i-hat momentum is -3.00 kg*m/s and the force integral is 0.560 N*s. Adding these together gives the final i-hat momentum of \(-3.00 kg*m/s + 0.560 kg*m/s = -2.44 kg*m/s\).
03

Find Force Integral for the j-hat Component

The force in the j-hat direction is \(-0.450 N/s^2 * t^2\). Integrate this function with respect to time from 0 to 2 seconds. The integral of \(t^2\) with respect to t is \(1/3*t^3\), so when calculated between 0 and 2 seconds, the integral becomes \(-0.450 N/s^2 * 1/3 * 2^3 = -1.20 N * s\).
04

Calculate j-hat Momentum

The j-hat component of momentum is the initial momentum plus the change in momentum caused by the external force. The initial j-hat momentum is 4.00 kg*m/s and the force integral is -1.20 kg*m/s. Adding these together gives the final j-hat momentum of \(4.00 kg*m/s - 1.20 kg*m/s = 2.80 kg*m/s\).
05

Combine Components

Combine the i-hat momentum and the j-hat momentum to find the total momentum at time t=2.00 s. The total momentum is \(-2.44 kg*m/s * \hat{\imath} + 2.80 kg*m/s * \hat{\jmath}\).

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Key Concepts

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

Force Integration
When dealing with varying forces over time, integrating the force function can help find the change in momentum. In simpler terms, force integration involves calculating the area under the force-time curve, which gives us an impulse. Impulse is essentially the total push given to the object.

For a force that changes with time like the one given, you need to determine the integral of the force function over the time interval of interest. For the i-hat direction here, the force increases linearly with time, depicted by the function \(0.280 \; \text{N/s} \, t\). To find the impulse, or the change in momentum, you integrate this function between the specified times (0 to 2 seconds).

The integral of \(t\) with respect to \(t\) is \(0.5 t^2\). Calculating this from 0 to 2 gives:
  • \(0.5 \times (2)^2 \times 0.280 \; \text{N/s} = 0.560 \; \text{N s}\)
This result gives the change in momentum in the i-hat direction due to the external force applied between 0 and 2 seconds.
Change in Momentum
Change in momentum, often referred to as \(\Delta p\), arises when an object is subjected to an external force. The initial momentum is altered by the impulse, the calculated result from force integration.

In our example problem, to find the final momentum, we add the change in momentum due to the external force to the initial momentum. For the i-hat component of momentum, the initial value is \(-3.00 \; \text{kg m/s}\), and the calculated change is \(0.560 \; \text{kg m/s}\). By adding these together:
  • The final i-hat momentum becomes \( -3.00 + 0.560 = -2.44 \; \text{kg m/s}\).
Similarly, for the j-hat component, the change calculated was \(-1.20 \; \text{kg m/s}\), and the initial was \(4.00 \; \text{kg m/s}\). So,
  • Final j-hat momentum is \(4.00 - 1.20 = 2.80 \; \text{kg m/s}\).
By knowing both components, we can find the total momentum at any given time.
External Forces
External forces are influences from outside a system that change its momentum. They play a crucial role in determining how an object's motion evolves over time.

In this problem, a force acting on a box in both horizontal directions (i-hat and j-hat) was applied, modifying its momentum. The net effect of these forces over time is calculated via integration, as we did before.

The concept highlights that without such a force, an object would maintain its state of motion. However, with the presence of an external force like the ones here:
  • A positive force in the i-hat direction increased momentum.
  • A negative force in the j-hat direction decreased momentum.
External forces drive changes by providing energy that alters the object's velocity and, consequently, its momentum. This makes understanding these forces key to predicting and analyzing motion in physical systems.

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Most popular questions from this chapter

In a game of phy sics and skill, a rigid block (A) with mass \(m\) sits at rest at the edge of a frictionless air table, \(1.20 \mathrm{~m}\) above the floor. You slide an identical block \((B)\) with initial speed \(v_{B}\) toward \(A\). The blocks have a head-on elastic collision, and block \(A\) leaves the table with a horizontal velocity. The goal of the game is to have block \(A\) land on a target on the floor. The targct is a horizontal distance of \(2.00 \mathrm{~m}\) from the edge of the table. What is the initial speed \(v_{n}\) that accomplishes this? Neglect air resistance.

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At time \(t=0\) a \(2150 \mathrm{~kg}\) rocket in outer space fires an engine that excrts an increasing force on it in the \(+x\) -direction. This force ohcys the equation \(F_{x}=A t^{2}\), where \(t\) is time, and his a magritude of \(781.25 \mathrm{~N}\) when \(t=1.25 \mathrm{~s}\). (a) Find the \(\mathrm{Sl}\) value of the constant \(\mathrm{A},\) including its units. (b) What impulse does the engine exert on the rocket during the \(1.50 \mathrm{~s}\) intcrval starting \(200 \mathrm{~s}\) after the cngine is firod? (c) By how much docs the rockel's velocity change during this interval? Assume constant mass.

Starting at \(t=0\) a net external force \(F(t)\) in the \(+x\) -direction is applied to an object that has mass \(3.00 \mathrm{~kg}\) and is initially at rest. The force is zero at \(t=0\) and increascs lincarly to \(5.00 \mathrm{~N}\) at \(t=4.00 \mathrm{~s}\) The force then decreases lincarly until it becomes zero at \(t=10.0 \mathrm{~s}\) (a) Draw a graph of \(F\) versus \(t\) from \(t=0\) to \(t=10.0 \mathrm{~s}\). (b) What is the spced of the object at \(t=10.0 \mathrm{~s} ?\)

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