A tabular analysis of the transactions made by Roberta Mendez & Co., a certified public accounting firm, for the month of August is shown below
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- The company issued shares of stock to stockholders for $25,000 cash.
- The company purchased $7,000 of equipment on account.
- The company received $8,000 of cash in exchange for services performed.
- The company paid $850 for this month’s rent.
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δ=∫0LA(x)E(x)P(x)dx .
Internal Force. The internal axial force varies along the member since it is dependent on the weight W ( y ) of a segment of the member below any section, Fig. 4–8 b . Hence, to calculate the displacement, we must use
\delta =\int_{0}^{L}{\frac{P(x)dx}{A(x)E(x)} }δ=∫0LA(x)E(x)P(x)dx .
At the section located a distance y from its free end, the radius x of the cone as a function of y is determined by proportion; i.e.,
\frac{x}{y}=\frac{r_0}{L}; \quad \quad x=\frac{r_0}{L}yyx=Lr0;x=Lr0y
The volume of a cone having a base of radius x and height y is
V=\frac{1}{3}\pi yx^2=\frac{\pi r^2_0}{3L^2}y^3V=31πyx2=3L2πr02y3
Since W=\gamma VW=γV, the internal force at the section becomes
+\uparrow \sum{F_y}=0;\quad\quad\quad P(y)=\frac{\gamma \pi r^2_0}{3L^2}y^3+↑∑Fy=0;P(y)=3L2γπr02y3
Displacement. The area of the cross section is also a function of position y , Fig. 4–8 b . We have
A(y)=\pi x^2=\frac{\pi r^2_0}{L^2}y^2 A(y)=πx2=L2πr02y2
Applying \delta =\int_{0}^{L}{\frac{P(x)dx}{A(x)E(x)} }δ=∫0LA(x)E(x)P(x)dx between the limits of y = 0y=0 and y = Ly=L yields
\delta =\int_{0}^{L}{\frac{P(y)dy}{A(y)E} }=\int_{0}^{L}{\frac{[(\gamma \pi r^2_0/3L^2)y^3]dy}{[(\pi r^2_0/L^2)y^2]E} }δ=∫0LA(y)EP(y)dy=∫0L[(πr0 need an explanation for this answer? contact us directly to get an explanation for this answer