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26 Pages

### Chap008

Course: ACC 492 acc 492, Spring 2010
School: University of Phoenix
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Word Count: 8707

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08 Chapter - Acquisition and Expenditure Cycle CHAPTER 8 Acquisition and Expenditure Cycle LEARNING OBJECTIVES Review Checkpoints Exercises, Problems, and Simulations 1. Identify significant inherent risks in the acquisition and expenditure cycle. 1 43 2. Describe the acquisition and expenditure cycle, including typical source documents and controls. 2, 3, 4, 5, 6 39 3. Give examples of tests of...

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University of Phoenix - ACC 492 - acc 492
Chapter 09 - Production CycleCHAPTER 9 Production Cycle LEARNING OBJECTIVESReview Checkpoints 1. Describe the production cycle, including typical source documents and controls. Give examples of tests of controls for auditing the controls over conversion
University of Phoenix - ACC 492 - acc 492
Chapter 10 - Finance and Investment CycleCHAPTER 10 Finance and Investment Cycle LEARNING OBJECTIVESReview Checkpoints Exercises, Problems, and Simulations1.Describe the finance and investment cycle, including typical source documents and controls. Gi
University of Phoenix - ACC 492 - acc 492
Chapter 11 - Completing the AuditCHAPTER 11 Completing the Audit LEARNING OBJECTIVESReview Checkpoints 1. Describe the approach used to examine major revenue and expense accounts. Identify procedures performed by auditors to evaluate contingencies, incl
University of Phoenix - ACC 492 - acc 492
University of Phoenix - ACC 492 - acc 492
Module B - Professional EthicsMODULE B Professional Ethics LEARNING OBJECTIVESReview Checkpoints 1. Understand general ethics and a series of steps for making ethical decisions. 2. Reason through an ethical decision problem using the imperative, utilita
University of Phoenix - ACC 492 - acc 492
Module C - Legal LiabilityMODULE C Legal Liability LEARNING OBJECTIVESReview Checkpoints 1. Identify and describe auditors exposure to lawsuits and loss judgments. 2. Specify the characteristics of auditors liability under common law and cite some speci
University of Phoenix - ACC 492 - acc 492
Module E - Overview of SamplingMODULE E Overview of Sampling LEARNING OBJECTIVESReview Checkpoints Exercises, Problems, and Simulations1.Understand the basic principles of sampling, including the differences between statistical and nonstatistical samp
University of Phoenix - ACC 492 - acc 492
Module F - Attribute SamplingMODULE F Attribute Sampling LEARNING OBJECTIVESReview Checkpoints 1. Identify the objectives of attribute sampling, define deviation conditions, and define the population for an attribute sampling application. Understand how
University of Phoenix - ACC 492 - acc 492
Module H - Information Systems AuditingMODULE H Information Systems Auditing LEARNING OBJECTIVESReview Checkpoints 1. 2. 3. List and describe the general and application controls in a computerized information system. Explain the difference between audit
University of Phoenix - ACC 492 - acc 492
Audit StagesFIRST INTERIM AUDIT STAGE 1: Understand the Business Understand the business and industry in which it operates. An example of business risk factors evaluation report is shown in Illustration 1. Other aspects of understanding the business: A g
Virginia Tech - AHRM - 2984
Virginia Tech - AHRM - 2984
Center Front 01 1.5 2chin shoulders bust3waist/elbows hips/wrists4 4.25 5crotch fingertips6knees7calves89ankles10toes
Virginia Tech - AHRM - 2984
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Virginia Tech - AHRM - 2984
International Production and TradeSoak Wai Wong November 13, 20071General Theme The world textile and apparel market after the end of Multi-fiber Agreement (MFA) ~ elimination of quotas Factor of competitiveness that influence sourcing strategies with
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UCLA - PHYS - 1B
Review information for the indicated chapter.
UCLA - PHYS - 1B
Chapter 22Here are sample problems that illustrate how to nd electric elds using Gauss law. First, we show generally how to nd electric elds due to spherically symmetric and then cylindrically symmetric charge distributions. Consider rst a spherically sy
UCLA - PHYS - 1B
Chapter 23As before, the diculty is listed immediately after each problem, ranging from 1 (least dicult) to 10 (most dicult). Problem 1 (Diculty: 5) Consider a collection of N point charges cfw_Q1 , Q2 , ., QN , where each charge Qj is located at a point
UCLA - PHYS - 1B
Chapter 24There are two main types of capacitor congurations: series and parallel. For each of these, heres how the charges and voltages across each capacitor are related, and how to compute the equivalent capacitance.Capacitors in Series: Consider capa
UCLA - PHYS - 1B
Chapter 26There are two main types of resistor congurations: series and parallel. For each of these, heres how the currents and voltages across each resistor are related, and how to compute the equivalent resistance. Resistors in series: Suppose we have
UCLA - PHYS - 1B
Chapter 27Heres an important point to keep in mind regarding magnetic forces. Consider a closed loop of any shape in a uniform magnetic eld, carrying a current I . The magnetic force on the loop is zero. This can be shown mathematically as follows: F=lo
UCLA - PHYS - 1B
Review for Final ExamThe rst section covers reection and transmission in a string, while the second section covers how to derive and explain the Doppler eect, both of which were mentioned to me in conjunction with your nal exam. However, theres much more
UCLA - PHYS - 1C
Physics 1CFirst MidtermFebruary 3, 2009Name:_Solutions_ Student ID:_This is a closed book test. No calculators. Write in pen. You may use your 3X5 inch index card and nothing else (but your brain). Use this booklet and write your name (in print) on ev
UCLA - PHYS - 1C
Physics 1C F irst Week Class notes : Walter Gekelman Winter 2008Physics 1C Winter 2008Class Notes : Walter GekelmanLet us review once again the Force laws as well as those involving electric forces:! ! (1) F = q E + v ! B()Force law with Lorentz te
UCLA - PHYS - 1C
1C second week notes - GekelmanPhysics 1C notes Faradays LawWeek 2Prof. Walter Gekelman(1)!=&quot;! B is the magnetic flux. The first term is the total time derivative of the magnetic flux and the second is the same (the integral is simply the definition
UCLA - PHYS - 1C
Physics 1C Faradays Law ! = &quot;Week 3 notesW. Gekelman#\$ B leads us to the concept of inductance. If one part of a circuit #t p roduces a changing magnetic flux and this in turn goes through a loop in another part of a circuit or in an adjacent circuit i
UCLA - PHYS - 1C
Physics 1C Chapter 31 notesWinter Quarter 2009AC circuits W. GekelmanConsider a capacitor. This is an element of an AC circuit. The charge is related to the voltage by Q = CV . Since dQ dV then I = C . This I= dt dt is the current through the capacitor
UCLA - PHYS - 1C
Midterm 2 study guideThe second 1C midterm will be on Friday February 27th in class. Just like the first exam it will be in a self contained booklet provided to you. There will be trig identities if you need them . You may bring a 3X5 inch index card wit
UCLA - PHYS - 1C
Physics 1CWinter Quarter 2009W. Gekelman Notes-5Let us write down Maxwells equations in both integral and differential form. Differential Form !&quot; !E = #0 ! !B = 0 ! ! \$B !&quot;E= # \$t ! ! ! \$E ! &quot; B = 0 j + 0# 0 \$t Integral Form ! q E i ndA = &quot; ! 0 ! ! Bin
UCLA - PHYS - 1C
Physics 1C W. GekelmanClass Notes Sixth WeekWinter 2009 chapter 33Consider the energy density of an electromagnetic wave. To get it let us add the energy density (energy/volume) of electric fields and of magnetic fields.u=1 12 E !0E 2 + B but = c = 2
UCLA - PHYS - 1C
Physics 1C Week 7 Interference of Light:Winter 2009Class Notes Walter GekelmanIf two vectors of equal magnitude and opposite direction are added their sum is zero. This is the basic principle of the interference of light. E = E0 cos( kz ! &quot; t ) ! E0 co
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 10-05-09HOMEWORK # 1 Reading Assignment: Review Special Relativity energy-momentum relations: SMM, Ch. 2, Summary p. 59. SMM: Ch. 3: Sections 3.1 - 3.6.Problems: 1. Consider the black body radiation curves (Figure 3
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 10-12-09HOMEWORK # 2 Reading Assignment: SMM Ch. 4: section 4.2, subsection Rutherfords Model of the Atom (the rest of 4.2 is optional background material); sections 4.3 - 4.5.Problems: 1. SMM Ch. 4: Problem #15 2.
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 10-16-09HOMEWORK # 3 Reading Assignment: SMM Ch. 5. (Subsection The Electron Microscope in section 5.2 is optional material. You may also nd it useful to review the basics of wave motion, interference and diraction i
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 10-23-09HOMEWORK # 4 Reading Assignment: SMM Ch. 6, Sections 6.1-6.5. Subsection Charge-Coupled Devices in 6.4 is optional.Problems: 1. SMM Ch. 6: #1 2. SMM Ch. 6: #2 3. SMM Ch. 6: #5 4. The Schrdinger equation for
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 11-2-09HOMEWORK # 5 MIDTERM: Our Midterm exam is on Friday, October 30. (The midterm date was changed by majority vote.) REVIEW: Thursday, October 29, 3-4:20 pm, MS 5147 Reading Assignment: SMM Ch. 6, Sections 6.1 -
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 11-13-09HOMEWORK # 6 Reading Assignment: Reif, Ch. 2. Omit Section 2.3 (The Binomial Distribution), p. 67-74. After you study Ch. 2, you may go back and read through Ch. 1, Sections 1.1 - 1.4, as useful qualitative b
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 11-23-09HOMEWORK # 7 Reading Assignment: Reif, Ch. 3.Problems: 1. Three particles are placed in a cubic box of edge length L. The system is isolated with total energy 2 h2 . E = 12 2m L2 Focus attention on any one o
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 11-30-09HOMEWORK # 8 Reading Assignment: Reif, Ch. 4.Problems: 1. = 1/kT expressed in energy units of eV at room temperature is about 40 (eV)1 . Consider then a macroscopic system at room temperature. Suppose the sy
UCLA - PHYS - 17
Physics 17 Fall 2009 T. TomboulisDue 12-4-09HOMEWORK # 9 Final: Monday, December 7 Reading Assignment: Reif, Ch. 5 (section 5.2 optional)Problems: 1. R Ch. 5: #5.3 2. R Ch. 5: #5.4 3. R Ch. 5: #5.5 4. R Ch. 5: #5.14 5. R Ch. 5: #5.151
UCLA - PHYS - 17
UCLA - PHYS - 17
6 (a) Energy conservation: Ei = Ef + hf + where p is the momentum of the recoiling atom. Momentum conservation: 0 = p p where p is the momentum of the emitted photon . But p = Hence, (1) - (2) give: Ei = Ef + hf + i.e. the exact formula for f is: f2 + 2M
UCLA - PHYS - 17
UCLA - PHYS - 17
UCLA - PHYS - 17
UCLA - PHYS - 17
UCLA - PHYS - 17
UCLA - PHYS - 17
UCLA - PHYS - 17
UCLA - PHYS - 17
Physics 17 Fall 2009 October 30, 2009 T. TomboulisMIDTERM SOLUTIONS 1. [10 points ] The electron in a hydrogen atom is initially in the second excited state state (n = 3). 1. What is the longest wavelength of light it could absorb? 2. Suppose the electro
University of Texas - MKT - 320F
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