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\(\mathbb{R}^{2}\) Consider the vectors \(\mathbf{I}=\langle 1 / \sqrt{2}, 1 / \sqrt{2}\rangle\) and \(\mathbf{J}=\langle-1 / \sqrt{2}, 1 / \sqrt{2}\rangle\). Express \(\mathbf{I}\) and \(\mathbf{J}\) in terms of the usual unit coordinate vectors i and j. Then, write i and \(\mathbf{j}\) in terms of \(\mathbf{I}\) and \(\mathbf{J}\).

Short Answer

Expert verified
Question: Express the standard unit coordinate vectors i and j in terms of the given vectors \(\mathbf{I} = \langle 1 / \sqrt{2}, 1 / \sqrt{2}\rangle\) and \(\mathbf{J} = \langle -1 / \sqrt{2}, 1 / \sqrt{2}\rangle\). Answer: \(\mathbf{i} = (1/2)\mathbf{I} + (1/2)\mathbf{J}\) and \(\mathbf{j} = (1/2)\mathbf{I} - (1/2)\mathbf{J}\).

Step by step solution

01

Express \(\mathbf{I}\) and \(\mathbf{J}\) in terms of i and j

We are given \(\mathbf{I} = \langle 1 / \sqrt{2}, 1 / \sqrt{2}\rangle\) and \(\mathbf{J} = \langle -1 / \sqrt{2}, 1 / \sqrt{2}\rangle\). To find the linear combinations of i and j that result in these vectors, we have: \(\mathbf{I} = (1/ \sqrt{2})\mathbf{i} + (1 / \sqrt{2})\mathbf{j}\) \(\mathbf{J} = (-1/ \sqrt{2})\mathbf{i} +(1 / \sqrt{2})\mathbf{j}\)
02

Express i and j in terms of \(\mathbf{I}\) and \(\mathbf{J}\)

Let i and j be linear combinations of \(\mathbf{I}\) and \(\mathbf{J}\) in the following form: \(\mathbf{i} = a\mathbf{I} + b\mathbf{J}\) \(\mathbf{j} = c\mathbf{I} + d\mathbf{J}\) Now, we can use the relationships we found in Step 1 to solve for the coefficients a, b, c, and d. On equating components in the first equation, we get: \(a(1/ \sqrt{2}) + b(-1/ \sqrt{2}) = 1\) \(a(1/ \sqrt{2}) + b(1/ \sqrt{2})= 0\) Similarly, on equating components in the second equation, we get: \(c(1/ \sqrt{2}) + d(-1 / \sqrt{2})= 0\) \(c(1/ \sqrt{2}) + d(1 / \sqrt{2})= 1\) Using the above four equations, we can solve for a, b, c, and d: a = b = 1/2 c = d = 1/2 Finally, we can write i and j in terms of \(\mathbf{I}\) and \(\mathbf{J}\): \(\mathbf{i} = (1/2)\mathbf{I} + (1/2)\mathbf{J}\) \(\mathbf{j} = (1/2)\mathbf{I} - (1/2)\mathbf{J}\)

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Key Concepts

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

Understanding Unit Vectors
Unit vectors are fundamental in vector algebra. They help us understand direction without being affected by magnitude. A unit vector has a length of 1 and is usually represented by a hat symbol, like \( \hat{i} \) and \( \hat{j} \). These vectors form the basis for other vectors in two-dimensional space. For instance, any vector \( \mathbf{v} = \langle x, y \rangle \) can be rewritten as a sum of the unit vectors \( \mathbf{v} = x\hat{i} + y\hat{j} \). This representation allows us to express a vector in terms of its components along the x and y axes.
In our example, we have the vectors \( \mathbf{I} \) and \( \mathbf{J} \), which are expressed in terms of unit vectors \( \mathbf{i} \) and \( \mathbf{j} \). By decomposing these vectors, we get:
  • \( \mathbf{I} = (1/ \sqrt{2})\mathbf{i} + (1 / \sqrt{2})\mathbf{j} \)
  • \( \mathbf{J} = (-1/ \sqrt{2})\mathbf{i} + (1 / \sqrt{2})\mathbf{j} \)
Understanding this expression helps in realizing how unit vectors contribute to forming other vectors.
Demystifying Coordinate Transformation
Coordinate transformation is the process of converting coordinates from one system to another. It allows us to understand and interpret vectors in different orientations or positions. In our exercise, we transform the vector expressions of \( \mathbf{i} \) and \( \mathbf{j} \) in terms of \( \mathbf{I} \) and \( \mathbf{J} \). These transformations require rearranging and solving algebraic equations that define the relationships between different vector systems.
We start with:
  • First, by expressing \( \mathbf{i} \) as a combination of \( \mathbf{I} \) and \( \mathbf{J} \): \( \mathbf{i} = a\mathbf{I} + b\mathbf{J} \).
  • Second, by expressing \( \mathbf{j} \) similarly: \( \mathbf{j} = c\mathbf{I} + d\mathbf{J} \).
Through solving these, we determine the coefficients needed to express these transformations. Here, they turn out to be \( a = b = 1/2 \) and \( c = d = 1/2 \). This means each unit vector is equally composed of vectors \( \mathbf{I} \) and \( \mathbf{J} \). This transformation highlights how vectors can be redefined through orientation changes.
Exploring Linear Combinations
Linear combinations are used to express vectors as sums of other vectors, scaled by coefficients. This is crucial in understanding how different vector components can be added together to form new vectors. In this exercise, we express vectors \( \mathbf{I} \) and \( \mathbf{J} \) as linear combinations of unit vectors \( \mathbf{i} \) and \( \mathbf{j} \), showing the versatility and interchangeability of vector forms.
To achieve this, we use the following combinations:
  • \( \mathbf{I} = (1/ \sqrt{2})\mathbf{i} + (1 / \sqrt{2})\mathbf{j} \)
  • \( \mathbf{J} = (-1/ \sqrt{2})\mathbf{i} + (1 / \sqrt{2})\mathbf{j} \)
Next, we reversed the roles and expressed \( \mathbf{i} \) and \( \mathbf{j} \) in terms of \( \mathbf{I} \) and \( \mathbf{J} \) through linear combinations:
  • \( \mathbf{i} = (1/2)\mathbf{I} + (1/2)\mathbf{J} \)
  • \( \mathbf{j} = (1/2)\mathbf{I} - (1/2)\mathbf{J} \)
This approach allows us to see how different vectors can be constructed from a base set. Linear combinations are powerful tools in vector algebra, making it possible to explore vector relationships and dependencies integrally.

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Most popular questions from this chapter

Consider the curve \(\mathbf{r}(t)=(a \cos t+b \sin t) \mathbf{i}+(c \cos t+d \sin t) \mathbf{j}+(e \cos t+f \sin t) \mathbf{k}\) where \(a, b, c, d, e,\) and fare real numbers. It can be shown that this curve lies in a plane. Graph the following curve and describe it. $$\begin{aligned} \mathbf{r}(t)=&\left(\frac{1}{\sqrt{2}} \cos t+\frac{1}{\sqrt{3}} \sin t\right) \mathbf{i}+\left(-\frac{1}{\sqrt{2}} \cos t+\frac{1}{\sqrt{3}} \sin t\right) \mathbf{j} \\ &+\left(\frac{1}{\sqrt{3}} \sin t\right) \mathbf{k} \end{aligned}$$

Carry out the following steps to determine the (smallest) distance between the point \(P\) and the line \(\ell\) through the origin. a. Find any vector \(\mathbf{v}\) in the direction of \(\ell\) b. Find the position vector u corresponding to \(P\). c. Find \(\operatorname{proj}_{\mathbf{v}} \mathbf{u}\). d. Show that \(\mathbf{w}=\mathbf{u}-\) projy \(\mathbf{u}\) is a vector orthogonal to \(\mathbf{v}\) whose length is the distance between \(P\) and the line \(\ell\) e. Find \(\mathbf{w}\) and \(|\mathbf{w}| .\) Explain why \(|\mathbf{w}|\) is the distance between \(P\) and \(\ell\). \(P(-12,4) ; \ell: y=2 x\)

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 \(\mu=0.65 ?\)

Consider the motion of an object given by the position function $$\mathbf{r}(t)=f(t)\langle a, b, c\rangle+\left(x_{0}, y_{0}, z_{0}\right\rangle, \text { for } t \geq 0$$ where \(a, b, c, x_{0}, y_{0},\) and \(z_{0}\) are constants and \(f\) is a differentiable scalar function, for \(t \geq 0\) a. Explain why this function describes motion along a line. b. Find the velocity function. In general, is the velocity constant in magnitude or direction along the path?

The points \(P, Q, R,\) and \(S,\) joined by the vectors \(\mathbf{u}, \mathbf{v}, \mathbf{w},\) and \(\mathbf{x},\) are the vertices of a quadrilateral in \(\mathrm{R}^{3}\). The four points needn't lie in \(a\) plane (see figure). Use the following steps to prove that the line segments joining the midpoints of the sides of the quadrilateral form a parallelogram. The proof does not use a coordinate system. a. Use vector addition to show that \(\mathbf{u}+\mathbf{v}=\mathbf{w}+\mathbf{x}\) b. Let \(m\) be the vector that joins the midpoints of \(P Q\) and \(Q R\) Show that \(\mathbf{m}=(\mathbf{u}+\mathbf{v}) / 2\) c. Let n be the vector that joins the midpoints of \(P S\) and \(S R\). Show that \(\mathbf{n}=(\mathbf{x}+\mathbf{w}) / 2\) d. Combine parts (a), (b), and (c) to conclude that \(\mathbf{m}=\mathbf{n}\) e. Explain why part (d) implies that the line segments joining the midpoints of the sides of the quadrilateral form a parallelogram.

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