/*! 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 12 Express the vector \(\mathbf{v}=... [FREE SOLUTION] | 91Ó°ÊÓ

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Express the vector \(\mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\) in terms of the unit vectors \(\mathbf{i}\) and \(\mathbf{j}\)

Short Answer

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Question: Express the vector \(\mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\) in terms of the unit vectors \(\mathbf{i}\) and \(\mathbf{j}\). Answer: The vector \(\mathbf{v}\) can be expressed in terms of the unit vectors \(\mathbf{i}\) and \(\mathbf{j}\) as \(\mathbf{v}=v_{1}\mathbf{i}+v_{2}\mathbf{j}\).

Step by step solution

01

Identify the components of the given vector

The given vector \(\mathbf{v}\) is expressed using angle brackets as \(\mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\). In this form, \(v_{1}\) represents the x-component of the vector, and \(v_{2}\) represents the y-component.
02

Express the vector in terms of the unit vectors i and j

Now that we know the x and y components of the vector \(\mathbf{v}\), we can express it in terms of the unit vectors \(\mathbf{i}\) and \(\mathbf{j}\). Recall that in a Cartesian coordinate system, the unit vector \(\mathbf{i}\) has an x-component of 1 and a y-component of 0, while the unit vector \(\mathbf{j}\) has an x-component of 0 and a y-component of 1. Using these unit vectors, we can represent the x and y components of \(\mathbf{v}\) as the scalar multiples of \(\mathbf{i}\) and \(\mathbf{j}\) respectively. So we can write the vector \(\mathbf{v}\) as: $$\mathbf{v}=v_{1}\mathbf{i}+v_{2}\mathbf{j}$$

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Most popular questions from this chapter

Evaluate the following limits. $$\lim _{t \rightarrow 2}\left(\frac{t}{t^{2}+1} \mathbf{i}-4 e^{-t} \sin \pi t \mathbf{j}+\frac{1}{\sqrt{4 t+1}} \mathbf{k}\right)$$

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An object on an inclined plane does not slide provided the component of the object's weight parallel to the plane \(\left|\mathbf{W}_{\text {par }}\right|\) is less than or equal to the magnitude of the opposing frictional force \(\left|\mathbf{F}_{\mathrm{f}}\right|\). The magnitude of the frictional force, in turn, is proportional to the component of the object's weight perpendicular to the plane \(\left|\mathbf{W}_{\text {perp }}\right|\) (see figure). The constant of proportionality is the coefficient of static friction, \(\mu\) a. Suppose a 100 -lb block rests on a plane that is tilted at an angle of \(\theta=20^{\circ}\) to the horizontal. Find \(\left|\mathbf{W}_{\text {parl }}\right|\) and \(\left|\mathbf{W}_{\text {perp }}\right|\) b. The condition for the block not sliding is \(\left|\mathbf{W}_{\mathrm{par}}\right| \leq \mu\left|\mathbf{W}_{\text {perp }}\right| .\) If \(\mu=0.65,\) does the block slide? c. What is the critical angle above which the block slides with \(\mu=0.65 ?\)

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