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City College of San Francisco - FINANCE - Excel
A 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32B Quiz1 92 73 93 75 83C Quiz2 78 92 87 79 92D Quiz3 90 69 75 85 97E Average 87 78 85 80 91F Grade C D C D B Grading Criteria 94100 8893 8187 7580 074 A B C D FG
City College of San Francisco - FINANCE - Excel
Klassy Kow Salary Projections Based on Performance RatingsLast Name Kraus Stewart Ladewig McDonald Sante Sumara Steele Eassa Steinbeck Artagnan Calcivechia Alverez Nguyen First Name Heinrich Kathleen Glenn Robin Juan Keiko Marietta Nassar Sarah Ted Maria
City College of San Francisco - FINANCE - Excel
Klassy Kow Human Resources 2003 Vacation DaysLast NameKraus Stewart Ladewig McDonald Sante Sumara Steele Eassa Steinbeck Artagnan Calcivechia Alverez Nguyen Kraus Johnson Simara Remus Gorz Artagnan Sante Steinbeck Alverez Johnson Nguyen McDonald McDonal
City College of San Francisco - FINANCE - Excel
Klassy Kow Human Resources 2003 Vacation DaysLast NameAlverez Artagnan Calcivechia Eassa Kraus Kraus Ladewig McDonald Nguyen Sante Steele Steinbeck Stewart SumaraFirst NameToni Ted Maria Nassar Heinrich Heinrich Glenn Robin Luni Juan Conrad Sarah Kath
City College of San Francisco - FINANCE - Excel
Klassy Kow Human Resources 2003 Vacation DaysLast NameAlverez Artagnan Calcivechia Gorz Johnson Johnson McDonald McDonald Nguyen Remus Sante Simara Steinbeck StewartFirst NameToni Ted Maria Ronald Ted Ted Robin Robin Luni Rita Juan Melody Sarah Kathle
City College of San Francisco - FINANCE - Excel
Klassy Kow Ice Cream, Inc. Human Resources Department 401K Matching Contributions for 2005California January February March April May June July August September October November December Total $10,750 $10,535 $10,750 $10,643 $11,825 $12,040 $11,288 $12,9
City College of San Francisco - FINANCE - Excel
Klassy Kow Ice Cream Shops Inc. Kowabunga SalesChocolate Eugene Ashland Klamath Falls Roseburg Medford Vanilla Total
City College of San Francisco - FINANCE - Excel
City College of San Francisco - FINANCE - Excel
Klassy Kow Ice Cream, Salinas ShopHoliday Staff Payroll Week Ending 7/06/2002 Last Name Adams Bronfman Castleman Daly Johns Franks Meth O'Reilly Petersen Wagner Total First Name Julia Harvey Leonard Maureen Lisa Waldo Zena Megan Irene Charlotte Hours Wor
City College of San Francisco - FINANCE - Excel
Wilfredo De Leona9be64dff2b61c902ec184185ee97d303e3b4427.xls Sheet110/30/2010Klassy Kow Ice Cream Sales Representatives Expense Report Month of AprilWeek of April 3 Budgeted amount Actual expense Difference Week of April 10 Budgeted amount Actual expe
City College of San Francisco - FINANCE - Excel
City College of San Francisco - FINANCE - Excel
Klassy Kow Ice Cream Soda, Malted, and Shake SalesJune Ice Cream Soda, small Ice Cream Soda, medium Ice Cream Soda, large Malted, small Malted, medium Malted, large Shake, small Shake, medium Shake, large 10,000 11,000 10,000 9,000 9,000 5,000 12,000 16,
City College of San Francisco - FINANCE - Excel
Scenario SummaryCurrent Values: Current Prices Reduced Prices Increased PricesThis scenario shows This scenario shows This scenario shows sales at current sales at reuced sales at higher prices prices prices Modified by Wilfredo De Leon on 5/13/2007Cha
City College of San Francisco - FINANCE - Excel
Scenario SummaryCurrent Values: Modest SalesAssumes modest salesBest SalesAssumes high salesWorst SalesAssumes low salesChanging Cells: Oct 12,000 12,000 18,000 9,000 Nov 13,000 13,000 20,000 10,000 Dec 12,500 12,500 19,000 9,500 Result Cells: $B$5
City College of San Francisco - FINANCE - Excel
Scenario SummaryCurrent Values: Modest SalesAssumes average sales.Best SalesAssumes high sales.Worst SalesAssumes low sales.Changing Cells: Oct 23,000 10,500 23,000 Nov 24,000 10,000 24,000 Dec 25,000 9,000 25,000 Result Cells: $B$5 $50,370.00 $22,
City College of San Francisco - FINANCE - Excel
Klassy Kow Ice Cream, Inc. Employee Credit Union Christmas SpecialsCar Loan Number of payback years Total number of payments Loan amount Interest rate for loan Savings Plan 4 Number of savings years 48 Total number of deposits $(15,406) Deposit amount 4.
City College of San Francisco - FINANCE - Excel
Scenario SummaryCurrent Values: GrowthRateChanging Cells: $G$4 7.92% 1.50% Result Cells: $G$16 $4,000,000 $3,408,341 Notes: Current Values column represents values of changing cells at time Scenario Summary Report was created. Changing cells for each sc
City College of San Francisco - FINANCE - Excel
Scenario SummaryCurrent Values: 1%Multiplier 3%Ultiplier 2%MultiplierChanging Cells: ExtraCakes 25 50 17 Result Cells: $D$13 $720.38 $678.00 $715.67 Notes: Current Values column represents values of changing cells at time Scenario Summary Report was cre
City College of San Francisco - FINANCE - Excel
Soda Price AnalysisSelling Prices 0 0 0 $1.19 $238.00 $267.75 $357.00 $1.29 $258.00 $290.25 $387.00 $1.39 $278.00 $312.75 $417.00 $1.49 $298.00 $335.25 $447.00 $1.59 $318.00 $357.75 $477.00 $1.69 Number Sold $338.00 200 $380.25 225 $507.00 300Prices and
City College of San Francisco - FINANCE - Excel
Soda Count Flavor Size Chocolate Date Large Medium 11-Apr 1 1 10-Apr 2 9-Apr 8-Apr 1 6-Apr 5-Apr 4-Apr 1 2-Apr 1 1-Apr Grand Total 4 3Small 1 1 1Strawberry LargeVanilla Medium Small Large 1 1 1 1 1 1 Medium 1 1 SmallGrand Total 3 4 2 3 2 1 2 4 1 221
City College of San Francisco - FINANCE - Excel
Sales Rep Commission Comparison0 5.0% $1,000 5.50% $1,100 6.0% $1,200 6.50% $1,300 7.0% $1,400 7.50% Dollar Sales $1,500 $20,000Sales Versus Commission 0 5.0% 5.50% $20,000 $1,000 $1,100 $25,000 $1,250 $1,375 $30,000 $1,500 $1,650 $35,000 $1,750 $1,925
Capilano - PHYS - 214
4. (a) VB VA = U/q = W/(e) = (3.94 1019 J)/(1.60 1019 C) = 2.46 V. (b) VC VA = VB VA = 2.46 V. (c) VC VB = 0 (Since C and B are on the same equipotential line).
SFT - BUSINESS A - 45
One Member Limited Liability CompanyContributio n capital Assignment Profit distribution Membersh ip L iabilityWhen to contribute Proof of contributionFlowchartOrganizati onlegal representati ve D irector Who can be? Membershi p requiremen tBoard of
UWO - PHILOSOP - 2074
Syllabus:BusinessEthics(Philosophy2074)Whatisthenatureofmoralreasoning? 1.AmartyaSen,DoesBusinessEthicsMakeEconomicSense? HeatherSalazar,KantianBusinessEthics DavidMeeler,Utilitarianism Docorporationshavesocialresponsibilities? 2.MiltonFriedman,TheSocial
Universitas Padjadjaran - PHYSICS - 1820392838
III. Conclusion Through the use of Atwoods machine, we were able to test Newtons second law. By measuring the acceleration of the masses tested with Atwoods machine, we were able to calculate a value for the acceleration of gravity. While our data is not
Copiah-Lincoln - PHY - 225
6. (a) E = F e = ( 3.9 1015 N ) (1.60 1019 C ) = 2.4 104 N C = 2.4 104 V/m.(b) V = Es = 2.4 104 N C 012 m = 2.9 103 V. .chbg
Cogswell Poly - PHYS - 221
7. (a) The work done by the electric field isW = q0 E ds =i fq0 2 0d0dz =q0d (1.60 1019 C)(5.80 1012 C/m 2 )(0.0356 m) = 2 0 2(8.85 1012 C2 /N m 2 )= 1.87 1021 J. (b) Since V V0 = W/q0 = z/20, with V0 set to be zero on the sheet, the electric pote
Capitol College - PHY - 415
9. We connect A to the origin with a line along the y axis, along which there is no change of potential (Eq. 24-18: E ds = 0 ). Then, we connect the origin to B with a line along the x axis, along which the change in potential isV = zzx=40E ds = 4.0
Franklin IN - PHY - 520
10. In the inside region between the plates, the individual fields (given by Eq. 24-13) are in the same direction ( i ): 50 109 C/m 2 25 109 C/m 2 + Ein = i = (4.2 103 N/C)i . 12 2 2 12 2 2 2(8.85 10 C /N m ) 2(8.85 10 C /N m ) In the outside region whe
Mississippi Delta Community College - ASXX - 254
11. (a) The potential as a function of r is V ( r ) = V ( 0 ) E ( r )dr = 0 r r00qr 2 dr = 4 0 R 3 8 0 R 3 qr=(8.99 109 N m 2 C 2 )(3.50 1015 C)(0.0145 m) 2 = 2.68 104 V. 3 2(0.0231 m)(b) Since V = V(0) V(R) = q/80R, we have V ( R) = q 8 0 R = (8.9
Piedmont - CHEM - 125
12. (a) The potential difference is VA VB = q 4 0 rA 1 1 = (1.0 106 C ) ( 8.99 109 N m 2 C2 ) 4 0 rB 2.0 m 1.0 m q= 4.5 103 V. (b) Since V(r) depends only on the magnitude of r , the result is unchanged.
ITT Tech Pittsburgh - PHYS - 198
13. (a) The charge on the sphere isq = 4 0 VR =(200 V)(0.15 m) = 3.3 109 C. 9 2 2 8.99 10 N m C(b) The (uniform) surface charge density (charge divided by the area of the sphere) is=q 3.3 10 9 C = = 12 10 8 C / m 2 . . 2 2 4 R 4 015 m .bg
ITT Tech Pittsburgh - PHY - 248
14. The charge isq = 4 0 RV =(10m) (1.0V) 8.99 10 N m92/C2= 1.1109 C.
Hudson VCC - PHYS - 282
15. A charge 5q is a distance 2d from P, a charge 5q is a distance d from P, and two charges +5q are each a distance d from P, so the electric potential at P isq (8.99 109 N m 2 C2 )(5.00 1015 C) 1 1 1 1 V= + = = 4 0 2d d d d 8 0 d 2(4.00 102 m) q= 5.62
Hudson VCC - PHYS - 219
17. First, we observe that V (x) cannot be equal to zero for x > d. In fact V (x) is always negative for x > d. Now we consider the two remaining regions on the x axis: x < 0 and 0 < x < d. (a) For 0 < x < d we have d1 = x and d2 = d x. LetV ( x) = kFG
Duquesne - PHYS - 264
16. Since according to the problem statement there is a point in between the two charges on the x axis where the net electric field is zero, the fields at that point due to q1 and q2 must be directed opposite to each other. This means that q1 and q2 must
East MS CC - PHYS - 361
18. In applying Eq. 24-27, we are assuming V 0 as r . All corner particles are equidistant from the center, and since their total charge is 2q1 3q1+ 2 q1 q1 = 0, then their contribution to Eq. 24-27 vanishes. The net potential is due, then, to the two +4q
Cogswell Poly - PHY - 287
19. (a) The electric potential V at the surface of the drop, the charge q on the drop, and the radius R of the drop are related by V = q/40R. Thus8.99 10 9 N m 2 / C 2 30 10 12 C q R= = = 5.4 10 4 m. 4 0V 500 V (b) After the drops combine the total volum
Mississippi Gulf Coast Community College - PHY - 262
20. When the charge q2 is infinitely far away, the potential at the origin is due only to the charge q1 : q1 = 5.76 107 V. V1 = 4 0 d Thus, q1/d = 6.41 1017 C/m. Next, we note that when q2 is located at x = 0.080 m, the net potential vanishes (V1 + V2 = 0
Caldwell College - PHYS - 232
21. We use Eq. 24-20: V=9 2 2 30 p ( 8.99 10 N m C ) (1.47 3.34 10 C m ) = = 1.63 105 V. 2 2 9 4 0 r ( 52.0 10 m )1
Ludwig Maximilians Universität - PH - 282
22. From Eq. 24-30 and Eq. 24-14, we have (for i = 0) p cos p cos i Wa = qV = e 2 4 0 r 2 4 0 r ep cos cos 1) = 2( 4 0 rwith r = 20 109 m. For = 180 the graph indicates Wa = 4.0 1030 J, from which we can determine p. The magnitude of the dipole moment i
Daniel Webster - CHEM - 212
23. (a) All the charge is the same distance R from C, so the electric potential at C is 5Q1 1 Q1 6Q1 5(8.99 109 N m 2 C2 )(4.20 1012 C) = = 2.30 V, V= = 4 0 R R 4 0 R 8.20 102 m where the zero was taken to be at infinity. (b) All the charge is the same di
Carson-Newman - PHY - 315
24. The potential is VP = 1 4 0 dq 1 Q (8.99 109 N m 2 C2 )(25.6 1012 C) = dq = = rod R 4 0 R rod 4 0 R 3.71102 m= 6.20 V. We note that the result is exactly what one would expect for a point-charge Q at a distance R. This coincidence is due, in part, to
American Dubai - PHYS - 122
25. (a) From Eq. 24-35, we find the potential to be V =2 L / 2 + ( L2 / 4) + d 2 ln 4 0 d (0.06 m / 2) + (0.06 m) 2 / 4 + (0.08 m) 2 = 2(8.99 109 N m 2 C2 )(3.68 1012 C/m) ln 0.08 m = 2.43102 V. (b) The potential at P is V = 0 due to superposition.
The Petroleum Institute - PHYS - 241
26. Using Gauss law, q = = +495.8 nC. Consequently, q (8.99 109 N m 2 C2 )(4.958 107 C) V= = = 3.71104 V. 4 0 r 0.120 m
Claflin - PHY - 321
28. The dipole potential is given by Eq. 24-30 (with = 90 in this case) V= p cos p cos 90 = =0 4 0 r 2 4 0 r 2since cos(90) = 0 . The potential due to the short arc is q1 / 4 0 r1 and that caused by the long arc is q2 / 4 0 r2 . Since q1 = +2 C, r1 = 4.0
Andrew Jackson - PHY - 253
27. Since the charge distribution on the arc is equidistant from the point where V is evaluated, its contribution is identical to that of a point charge at that distance. We assume V 0 as r and apply Eq. 24-27:V= 1 +Q1 1 +4Q1 1 2Q1 1 Q1 + + = 4 0 R 4 2 R
Claflin - PHYS - 201
29. The disk is uniformly charged. This means that when the full disk is present each quadrant contributes equally to the electric potential at P, so the potential at P due to a single quadrant is one-fourth the potential due to the entire disk. First fin
Copiah-Lincoln - PHYS - 202
10. In the inside region between the plates, the individual fields (given by Eq. 24-13) are in the same direction ( i ): 50 109 C/m 2 25 109 C/m 2 + Ein = i = (4.2 103 N/C)i . 12 2 2 12 2 2 2(8.85 10 C /N m ) 2(8.85 10 C /N m ) In the outside region whe
Universitas Padjadjaran - PHYSICS - 1820392838
(Newton's Second Law and the Conservation of Energy)OBJECTIVE: To study the relation of masses and accelerations. METHOD: Consider the Atwood machine shown in Fig. 1. A pulley is mounted on a support a certain distance above the floor. A string with loop
Universitas Padjadjaran - PHYSICS - 1820392838
CalorimetryHeat Capacity of the CalorimeterConceptsIn calorimetry it is often desirable to know the heat capacity of the calorimeter itself rather than the heat capacity of the entire calorimeter system (calorimeter and water). The heat (q) released by
Sacred Heart - ACCT - 1001
Introduction and the IAS FrameworkWiecek and YoungIFRS PrimerChapter 1Chapter Overview Introductionand the Framework The U.S. experience to date Looking ahead Measurement model End-of-chapter practice2Introduction and the IAS FrameworkAcommon se
Sacred Heart - ACCT - 1001
Financial Statements IAS 1Wiecek and YoungIFRS PrimerChapter 2Related Standards FAS130 Reporting Comprehensive Income2Related Standards IFRS5 Non-current Assets Held for Sale and Discontinued Operations IFRS 7 Financial Instruments: Disclosures
Sacred Heart - ACCT - 1001
Statement of Cash Flows IAS 7Wiecek and YoungIFRS PrimerChapter 3Statement of Cash Flows Related IASstandards7 Current GAAP comparisons Looking ahead End-of-chapter practice2Related Standards FAS95 Statement of cash flows FAS 102 Statement of c
Sacred Heart - ACCT - 1001
Non-current Assets Held for Sale and Discontinued Operations: IFRS 5Wiecek and YoungIFRS PrimerChapter 4Non-current Assets Held for Sale and Discontinued Operations Related IFRSstandards5 Current GAAP comparisons IFRS financial statement disclosure
Sacred Heart - ACCT - 1001
Provisions, Contingent Liabilities and Contingent Assets: IAS 37Wiecek and YoungIFRS PrimerChapter 5Provisions, Contingent Liabilities and Contingent Assets Related IASstandards37 Current GAAP comparisons Looking ahead End-of-chapter practice2Rel
Sacred Heart - ACCT - 1001
Revenue: IAS 18Wiecek and YoungIFRS PrimerChapter 6Revenue Related IASstandards18 Current GAAP comparisons IFRS financial statement disclosures Looking ahead End-of-chapter practice2Related Standards SAB 104 Revenue Recognition SOP 81-1 Acc
Sacred Heart - ACCT - 1001
Inventories: IAS 2Wiecek and YoungIFRS PrimerChapter 7Inventories Related IASstandards2 Current GAAP comparisons IFRS financial statement disclosures Looking ahead End-of-chapter practice2Related Standards FAS151 Inventory costsan amendment of
Sacred Heart - ACCT - 1001
Construction Contracts: IAS 11Wiecek and YoungIFRS PrimerChapter 8Construction Contracts Related IASstandards11 Current GAAP comparisons IFRS financial statement disclosures Looking ahead End-of-chapter practice2Related Standards SAB104 Revenue
Sacred Heart - ACCT - 1001
Sacred Heart - ACCT - 1001
Property, Plant and Equipment: IAS 16Wiecek and YoungIFRS PrimerChapter 10Property, Plant and Equipment Related IASstandards16 Current GAAP comparisons IFRS financial statement examples Looking ahead End-of-chapter practice2Related StandardsFAS