Question 3.SP.5: A cube of side a is acted upon by a force P along the diagon......

A cube of side a is acted upon by a force P along the diagonal of a face, as shown. Determine the moment of P (a) about A, (b) about the edge AB, (c) about the diagonal AG of the cube. (d) Using the result of part c, determine the perpendicular distance between AG and FC.

STRATEGY: Use the equations presented in this section to compute the moments asked for. You can find the distance between AG and FC from the expression for the moment M_{A G}.

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Step 1:
In this problem, we are given a cube with a force P applied at point F. We need to find the moments of this force about points A, AB, and AG, as well as the perpendicular distance between AG and FC.
Step 2:
To find the moment about point A, we first need to resolve the force P and the vector rFA into their rectangular components. We can do this by choosing x, y, and z axes and expressing the vectors in terms of these axes. The vector rFA can be written as rFA = a(i - j), where a is the length of each side of the cube. The force P can be written as P/sqrt(2)(j - k).
Step 3:
The moment of P about A is the vector product of rFA and P. We can calculate this by taking the cross product of the two vectors: MA = rFA x P. This gives us MA = aP/sqrt(2)(i + j + k).
Step 4:
To find the moment about AB, we need to project MA onto the AB direction. Since AB is parallel to the x-axis, the projection of MA onto AB is simply the x-component of MA. Therefore, MAB = MA • i = aP/sqrt(2).
Step 5:
To find the moment about AG, we need to project MA onto the AG direction. We can do this by finding the unit vector along AG, which is given by λ = AG/|AG| = (a(i - j - k))/a√3 = (1/√3)(i - j - k). The moment about AG is then given by MAG = λ • MA. Substituting the values, we get MAG = -aP/√6.
Step 6:
Alternatively, we can also calculate the moment about AG using the determinant form. This involves taking the determinant of a matrix formed by λ and the components of rFA and P. This also gives us MAG = -aP/√6.
Step 7:
Finally, to find the perpendicular distance between AG and FC, we note that P is perpendicular to AG. This can be verified by taking the dot product of P and λ and confirming that it is zero. Since the moment MAG is equal to -Pd, where d is the perpendicular distance between AG and FC, we can equate the two expressions and solve for d. This gives us d = a/√6.
Step 8:
In summary, we have found the moments of the force P about points A, AB, and AG, as well as the perpendicular distance between AG and FC. These calculations involve vector operations and projections, as well as the use of unit vectors and determinants. It is important to visualize the forces and moments in three dimensions to choose the appropriate equations and understand the geometric relationships between them.

Final Answer

MODELING and ANALYSIS:

a. Moment about A. Choosing x, y, and z axes as shown (Fig. 1), resolve into rectangular components the force P and the vector \mathbf{r}_{F / A}=\overrightarrow{A F} drawn from A to the point of application F of P.

\mathbf{r}_{F / A}=a \mathbf{i}-a \mathbf{j}=a(\mathbf{i}-\mathbf{j})

\mathbf{P}=(P / \sqrt{2}) \mathbf{j}-(P / \sqrt{2}) \mathbf{k}=(P / \sqrt{2})(\mathbf{j}-\mathbf{k})

The moment of P about A is the vector product of these two vectors:

\mathbf{M}_A=\mathbf{r}_{F / A} \times \mathbf{P}=a(\mathbf{i}-\mathbf{j}) \times(P / \sqrt{2})(\mathbf{j}-\mathbf{k})

\mathbf{M}_A=(a P / \sqrt{2})(\mathbf{i}+\mathbf{j}+\mathbf{k})

b. Moment about AB. You want the projection of \mathbf{M}_A on AB:

M_{A B}=\mathbf{i} \cdot \mathbf{M}_A=\mathbf{i} \cdot(a P / \sqrt{2})(\mathbf{i}+\mathbf{j}+\mathbf{k})

M_{A B}=a P / \sqrt{2}

You can verify that since AB is parallel to the x axis, M_{A B} is also the x component of the moment M_{A }.

c. Moment about diagonal AG. You obtain the moment of P about AG by projecting M_{A } on AG. If you denote the unit vector along AG by λ (Fig. 2), the calculation looks like this:

\boldsymbol{\lambda}=\frac{\overrightarrow{A G}}{A G}=\frac{a \mathbf{i}-a \mathbf{j}-a \mathbf{k}}{a \sqrt{3}}=(1 / \sqrt{3})(\mathbf{i}-\mathbf{j}-\mathbf{k})

M_{A G}=\boldsymbol{\lambda} \cdot \mathbf{M}_A=(1 / \sqrt{3})(\mathbf{i}-\mathbf{j}-\mathbf{k}) \cdot(a P / \sqrt{2})(\mathbf{i}+\mathbf{j}+\mathbf{k})

M_{A G}=(a P / \sqrt{6})(1-1-1) \quad M_{A G}=-a P / \sqrt{6}

Alternative Method. You can also calculate the moment of P about AG from the determinant form:

M_{A G}=\left|\begin{array}{ccc}\lambda_x & \lambda_y & \lambda_z \\x_{F / A} & y_{F / A} & z_{F / A} \\F_x & F_y & F_z\end{array}\right|=\left|\begin{array}{ccc}1 / \sqrt{3} & -1 / \sqrt{3} & -1 / \sqrt{3} \\a & -a & 0 \\0 & P / \sqrt{2} & -P / \sqrt{2}\end{array}\right|=-a P / \sqrt{6}

d. Perpendicular Distance between AG and FC. First note that P is perpendicular to the diagonal AG. You can check this by forming the scalar product P \cdot \lambda and verifying that it is zero:

\mathbf{P} \cdot \boldsymbol{\lambda}=(P / \sqrt{2})(\mathbf{j}-\mathbf{k}) \cdot(1 / \sqrt{3})(\mathbf{i}-\mathbf{j}-\mathbf{k})=(P \sqrt{6})(0-1+1)=0

You can then express the moment M_{A G} as -Pd, where d is the perpendicular distance from AG to FC (Fig. 3). (The negative sign is needed because the rotation imparted to the cube by P appears as clockwise to an observer at G.) Using the value found for M_{A G} in part c,

M_{A G}=-P d=-a P / \sqrt{6} \qquad d=a / \sqrt{6}

REFLECT and THINK: In a problem like this, it is important to visualize the forces and moments in three dimensions so you can choose the appropriate equations for finding them and also recognize the geometric relationships between them.

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