Full Beam Design Example

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Full Beam Design Example"

Transcript

1 Full Beam Design Example CEE 3150 Reinforced Concrete Design Fall 003 Design the flexural (including cutoffs) and shear reinforcement for a typical interior span of a six span continuous beam with center-to-center spacing of 0 ft. Assume the supports are 1 inches wide. Check that deflection (excessive deflections will cause problems) and crack-width serviceability requirements are met. Given: SDL.15 kip/ft LL.65 kip/ft f c 4 kip/in f y 60 kip/in γ c 150 lb/ft 3 FLEXURAL DESIGN (A) Choose the beam depth, h. Because we are concerned about deflection, use a fairly deep beam (architect said it was O.K.): h l/10 0 ft/10 (1 in/foot) 4 in. (B) Assume two rows of steel both top and bottom: d pos d neg h 3.5 in 0.5 in. (C) Use a narrow beam for better efficiency. Assuming r b/d pos 0.4, b 0.4d pos 0.4(0.5 in) 8. in, use b 9 in. (D) Compute M u and M n at the midspan (maximum positive moment) and support (maximum negative moment). With our estimated beam height and width, we can calculate the selfweight, SW, and determine the total dead load, DL. SW bhw c (9 in)(4 in)(150 lb/ft 3 )(1 foot /144 in )(1 kip/1000 lb) 0.5 kip/ft DL SDL + SW (.15 kip/ft kip/ft).375 kip/ft w u 1.DL + 1.6LL 1.(.375 kip/ft) + 1.6(.65 kip/ft) 7.09 kip/ft Using the ACI design coefficients {ACI 8.3.3}: M u,pos w u l n/16 (7.09 kip/ft)(19 ft) / kip ft M n,pos M u,pos /φ (160 kip ft)/ kip ft M u,neg w u l n/11 (7.09 kip/ft)(19 ft) /11 33 kip ft M n,neg M u,neg /φ ( 33 kip ft)/ kip ft (E) Compute R Mn bd. R pos M n,pos bd pos R neg M n,neg bd neg 178 kip ft (1 in/foot)(1000 lb/1 kip) 564 psi (1) (9 in)(0.5 in) 59 kip ft (1 in/foot)(1000 lb/1 kip) 80 psi () (9 in)(0.5 in) 1

2 5 #7s #7s #5s 6 #5s M φ n Support 51 kip ft φ Mn Midspan 16 kip ft Figure 1: Reinforcing layout at the support and at midspan. Reading from the chart gives: (F) Compute A s,pos and A s,neg. ρ pos (3) ρ neg (4) A s,pos ρ pos bd pos (9 in)(0.5 in) 1.90 in (5) A s,neg ρ neg bd neg (9 in)(0.5 in).95 in (6) (G) Choose bars, make sure they fit. Positive: Use 6 #5, A s,pos 1.86 in. Negative: Use 5 #7, A s,neg 3.00 in. We are using slightly less steel for the positive reinforcement because #5 bars are small, resulting in a larger d pos than originally estimated. The positive reinforcement will be two rows of three bars, the negative reinforcement will have a top row of three and a bottom row of two bars (see Figure 1) and it is assumed that two bars from both positive and negative reinforcing will be continuous. A generic formula for the minimum width of a beam is given by: n b min cover + d bs + d bf,i + (n 1)c s,min (7) i1 where d bs is the diameter of the stirrup, d bf,i is the diameter of the i th flexural reinforcing bar, and c s,min is the minimum clear spacing between bars. We will use 1.5 inches clear cover and assume a #3 stirrup. The minimum beam width, b min, is controlled by the 3 #7 (d b in) bars: c s,min max(d b, 1 in) max(0.875 in, 1 in) 1 in (8) b min (1.5 in) + (0.375 in) + 3(0.875 in) + (1 in) 8.38 in (9) The bars will fit. Calculate the actual values for d pos and d neg. Because the positive steel is in two equal rows, the centroid is located at the center of the two rows. d pos 4 in 1.5 in in 0.65 in 0.5 in 1.0 in (10)

3 The negative steel has two unequal rows so the centroid is found by: d neg,1 4 in 1.5 in in (0.875 in)/ 1.7 in (11) d neg, d neg, in 1 in 19.8 in (1) d neg 3d neg,1 + d neg, 3(1.7 in) + (19.8 in) 0.9 in (13) 5 5 (H) Analyze the section, check φm n M u. Because some of the positive steel will continue into the negative moment region, and vice-versa, sections will be analyzed as doubly reinforced. It is assumed that two bars on top and bottom will continue throughout the beam. The spreadsheet doubly.xls in the course directory is used to analyze the sections and perform code checks. From the spreadsheet: φm n,pos 16.4 kip ft > M u,pos 160 kip ft (14) φm n,neg 50.8 kip ft > M u,neg 33 kip ft (15) The initial flexural design is done. Next, we design the shear reinforcement. SHEAR DESIGN (1) Find the shear envelope. The ACI coefficients give shear at the face of interior supports as w u l n /. Thus, for the present case: V u,sup w ul n (7.09 kip/ft)(19 ft) 67.4 kip (16) Assume that the maximum shear at midspan is as derived for a simple beam: V u,mid 1.6(LL)l n 8 1.6(.65 kip/ft)(19 ft) kip (17) The equation which defines the shear envelope is then given by: [ ] Vu,sup V u,mid V u (x) V u,sup x (18) l n / [ ] 67.4 kip 10.1 kip 67.4 kip x (19) 19 ft/ 67.4 kip (6.03 kip/ft)x (0) () Check that V u,max φ(v c + 8 f cbd). Recall that V u,max is the shear at the critical section distance d from the face of the support. Assume that d d pos 1.0 in(1 foot/1 in) 1.75 ft so that: V u,max V u (d pos ) V u (1.75 ft) (1) 67.4 kip (6.03 kip/ft)(1.75 ft) 56.8 kip () V c f cbd pos (3) 4, 000 lb/in (9 in)(1.0 in)(1 kip/1000 lb) (4) 3.9 kip (5) φ(v c + 8 f cbd pos ) φ(5v c ) 0.75(5)(3.9 kip) 89.7 kip. (6) Thus, V u,max 56.8 kip < φ(v c + 8 f cbd pos ) 89.7 kip indicating that the section is large enough. The shear envelope is plotted in Figure. 3

4 V u,sup V u (x) (kip) 0 10 V u,max V u,mid 1 3 x (feet) Figure : The shear envelope. (3) Pick bars and set spacing. Assume #3 stirrups will be used. The spacing near the support, dependent on V u,max, is (again, using d pos for d): s A vf y d pos V u,max φ 0. in (60 kip/in )(1.0 in) 56.8 kip V c 3.9 kip in (7) Use s 5.0 in and compute the capacity of the stirrups: V s A vf y d pos s 0. in (60 kip/in )(1.0 in) 5.0 in 55.4 kip (8) To find the maximum spacing, compare V s to 4 f cbd pos : 4 f cbd pos 4 4, 000 lb/in (9 in)(1.0 in)(1 kip/1000 lb) 47.8 kip (9) Thus, because V s > 4 f cbd pos the maximum spacing is given by d pos /4 1.0 in/4 5.5 in. The chosen spacing, s 5.0 in < 5.5 in, meets the maximum spacing. The total capacity of the beam, φv n, for s 5.0 in is then: φv n φ(v c + V s ) 0.75(3.9 kip kip) 59.5 kip > V u,max 56.8 kip (30) As the shear drops, the maximum spacing will increase to d pos / (1.0 in)/ 10.5 in. So, we will use s 10.0 in near the midspan. The shear capacity of the stirrups and total capacity at that spacing is V s A vf y d pos 0. in (60 kip/in )(1.0 in) 7.7 kip (31) s 10.0 in φ(v c + V s ) 0.75(3.9 kip kip) 38.7 kip (3) Solving Equation 0 for V u (x) 38.7 kip gives x 4.76 ft 4 ft 9 in. Note that at s 10.0 in, V s < 4 f cbd pos so that the maximum stirrup spacing is indeed d/. Check that 4

5 5" 7" 10" " 4" x (feet) Figure 3: Initial shear design. this meets the minimum steel requirements: ( b A v,min max 0.75 f c w s, 50b ) ws f y f y ( (9 in)10.0 in max , 000 lb/in 60, 000 lb/in, 50 ) lb/in (9 in)10.0 in 60, 000 lb/in (33) (34) max ( in, in ) in (35) Using a #3 stirrup, A v (0.11 in ) 0. in > A v,min, so we meet the minimum area requirement of the code. Choose one more spacing interval, s 7 in, resulting in: V s A vf y d pos 0. in (60 kip/in )(1.0 in) 39.6 kip (36) s 7 in φ(v c + V s ) 0.75(3.9 kip kip) 47.6 kip (37) Because V s < 4 f cbd pos for s 7 in (compare Equation 36 to Equation 9), d/ spacing controls. Solving Equation 0 for V u (x) 47.6 kip gives x 3.8 ft 3 ft 3 in. Zone A starts when V u drops below φv c /: φv c / 0.75(3.9 kip)/ 8.96 kip < V u,mid 10.1 kip (38) Thus, there is no Zone A stirrups must be used throughout the beam. Using the calculations above, the stirrups are designed as shown in Figure 3 with the first stirrup at inches from the face of the support, then 8 additional stirrups at 5 inch spacing, 4 at 7 inch spacing, and 4 at 10 inch spacing. This results in a shear capacity as shown in Figure 4. FLEXURAL STEEL CUTOFFS Negative Reinforcement Cutoffs At the support there are five #7 bars as tension reinforcement (at the top of the beam since the moment is negative). It is assumed that two #5 compressive bars continue from the positive moment reinforcement. The nominal moment capacity for this arrangement is 51 kip ft as calculated above. The steel configuration at the support is shown in Figure 5 along with configurations used after cutting off steel as explained below. 5

6 V (x) and φ u V n (x) (kip) φv n(x) V u(x) x (feet) Figure 4: The shear envelope. Support Cutoff #1 Cutoff # φ Mn 51 kip ft φ Mn 163 kip ft φ Mn 111 kip ft Figure 5: Negative reinforcing layouts and section moment resistance. 6

7 c v c c 1 h Figure 6: Dimensions c 1, c h, and c v. Cutoff #1 We first wish to cut off the two #7s in the bottom row of the tension steel. This results in a moment capacity of 163 kip ft. Determine the development length using the general formula: l d 3 f y αβγλ 40 f c+k tr d b (39) c d b Note that α 1.3 because there are more than 1 inches of concrete below the reinforcing. Recall that c min(c 1, c ) where c 1 is the distance from the center of the bar to the nearest concrete surface and c is one-half the center-to-center spacing of the bars being developed in the horizontal or vertical direction. Designating c h as the horizontal dimension and c v as the vertical dimension (see Figure 6): c in in + (0.875 in)/.31 in (40) c h (b/ c 1 ) (9 in/.31 in).19 in (41) c v (d b + 1 in) / (0.875 in + 1 in) / in (4) c min(c 1, c h, c v ) in (43) Conservatively estimating that K tr 0, gives: c + K tr d b in in 1.07 (44) However, because we have stirrups and more than d b clear spacing in both the horizontal and vertical direction, the expression from the table in {ACI 1..} can be used for a #7 bar: l d f yαβλ 0 d b 60, 000 lb/in (1.3)(1.0)(1.0) f c in 4, 000 lb/in (45) 54.0 in 4.50 ft 0.37l n (46) Cutoff # Next, we will cut the center tension bar of the remaining three #7s. As there is only one row left, we do not need to worry about vertical spacing (c c h ). Again, we will use the general 7

8 Midspan Cutoff #1 Cutoff # φ Mn 16 kip ft φ Mn 138 kip ft φ Mn 88 kip ft Figure 7: Positive reinforcing layouts and section moment resistance. formula and compute c first: c in in + (0.875 in)/.31 in (47) c (b/ c 1 )/ ((9 in)/.31 in)/ 1.10 in (48) c min(c 1, c ) 1.10 in (49) c + K tr 1.10 in (50) d b in The expression c+ktr d b is less than 1.5, so it is more advantageous to use the equations in {ACI 1..} which gives the same development length as before: l d 0.37l n. At the cutoff locations, it is required that a buffer of length max(d, 1d b ) be provided (Rule #1). max(d, 1d b ) max(d neg, 1d b ) max(0.9 in, 1(0.875 in)) 0.9 in (51) Using a buffer of d neg 0.9 in 1.74 ft 0.09l n, the cutoff locations are determined as sketched on the attached plot. Positive Reinforcement Cutoffs At the midspan there are six #5 bars as tension reinforcement. It is assumed that two #7 compressive bars continue from the negative moment reinforcement. The steel configuration is shown in Figure 7 along with configurations used after cutting off steel as explained below. Cutoff #1 We first wish to cut off the middle #5 in the top row of the tension steel. This results in a moment capacity of 138 kip ft. c in in + (0.65 in)/.19 in (5) c h (b/ c 1 )/ ((9 in)/.19 in)/ 1.16 in (53) c v (d b + 1 in)/ (0.65 in + 1 in)/ 0.81 in (54) c min(c 1, c h, c v ) min(.19 in, 1.16 in, 0.81 in) 0.81 in (55) c + K tr 0.81 in (56) d b 0.65 in 8

9 We have more than d b clear spacing both horizontally and vertically and we are using stirrups, so again we will use the table in {ACI 1..} for #5 reinforcing steel: l d f yαβλ 5 d b 60, 000 lb/in (1.0)(1.0)(1.0) f c in 4, 000 lb/in (57) 3.7 in 1.98 ft 0.104l n (58) Cutoff # Next, we will cut the remaining #5s in the top row. The remaining three bars in the bottom row will continue into the supports. When cutting these two #5s, the vertical spacing is the same as before and will control the development length so that l d 0.104l n again. In this case our buffer is d pos 1.0 in 1.75 ft 0.09l n, and the cutoff locations are determined as sketched on the attached plot. Checking the Rules Negative Cutoff #1 Rule #1 Bars must extend the longer of d or 1d b past flexural cutoff points except at supports of simple spans or ends of cantilevers. {ACI } The buffer of max(d, 1d b ) is shown on the attached moment plot and the cutoff was determined so that this rule was satisfied. Rule # Bars must extend at least l d from the point of maximum bar stresses or from the point at which adjacent bars which are cut or bent are no longer required to resist flexure. {ACI 1.10., , 1.1.} Cutting these bars l d from the support results in a cutoff location 4.5 ft from face of the support. Rule #3 Bars cannot be cutoff in tension regions unless conditions in {ACI } are met. The #7s being cut are in tension so we must satisfy {ACI } which stipulates we must meet one of the conditions given in {ACI , , or }. {ACI }: To satisfy this condition, we need V u φv n /3 or V u /φv n /3. Looking at the shear design at x 4.50 ft (the location of cutoff #1) we are using s 7 in as spacing so that φv n 47.6 kip, and V u V u (4.50 ft) 67.4 kip (6.03 kip/ft)(4.50 ft) 40.3 kip. V u φv n 40.3 kip 47.6 kip 0.85 > 3 Thus, we do not satisfy this section. {ACI }: To satisfy this, we may need to add extra stirrups over the last 0.75d neg of the bar being cut. The required spacing of the additional bars, s + is: ( A v f y s + min (60 lb/in )b, d ) neg 8β b where β b is the ratio of the area of bars being cut to the total area. In this case, β b /5 since two #7s out of five are being cut. 0.75d neg s + (59) (60) ( 0. in (60, 000 lb/in ) ) 0.9 in s + min, 6.53 in (61) 60 lb/in (9 in) 8(/5) 0.75(0.9 in) 6.53 in/stirrup At the point of the cut we are using s 7 in spacing, so.40 stirrups (6) 0.75d neg s 0.75(0.9 in) 7 in 15.7 in 7 in.4 (63) 9

10 That is, we have.4 stirrups from the initial design and we need to add.40 additional stirrups for a total of 4.64 stirrups over 15.7 inches at the end of the cut bars. This works out to a spacing of 15.7 inches/4.64 stirrups3.4 inch/stirrup. So, we could reduce our stirrup spacing to 3 inches near the end of the cut bars. This is less than the ideal minimum of 4 inch spacing, but we are only doing it for a short distance because of concerns about the cutoff. {ACI }: In order to meet this criterion, we must have V u /φv n 3/4. Considering Equation 59, this is not met. Thus, to meet rule #3 we must add stirrups near the end of the bars being cut since we are cutting in tension. However, the point of inflection (P.I.) occurs at 4 ft 7 in from the face of the support so that by extending the two #7s by an inch we would no longer be cutting in tension and rule #3 would not apply. This is what we will do. Rule #6 Negative moment reinforcement must be anchored into or through supporting columns of members. {ACI 1.1.1} We plan to continue the negative reinforcement into the next span, through the support this rule is satisfied. Rule #7 We are considering an interior beam, so the applicable rule is: At least one-third of the negative moment reinforcement must be extended by the maximum of d, 1d b, or l/16 past the negative moment P.I. {ACI 1.1.3} The two #7s that continue throughout the beam represent /5 of the negative moment reinforcement which is greater than 1/3. This rule is satisfied. We have satisfied the cutoff rules for negative cutoff #1. The only change we needed to make was to add an extra inch to the cutoff location so that we are not cutting these bars in tension. Negative Cutoff # Rule #1 Bars must extend the longer of d or 1d b past flexural cutoff points except at supports of simple spans or ends of cantilevers. {ACI } The buffer is plotted on the chart and by inspection, this rule is met. Rule # Bars must extend at least l d from the point of maximum bar stresses or from the point at which adjacent bars which are cut or bent are no longer required to resist flexure. {ACI 1.10., , 1.1.} The adjacent bars were cut at cutoff #1. Consulting the attached plot, it is seen that the continuing bars continue more than l d from the point at which the bars from cutoff #1 are no longer needed. Rule #3 Bars cannot be cutoff in tension regions unless conditions in {ACI } are met. The # cutoff occurs in a region of positive moment, thus the bars are not being cut in tension. We do not need to consult {ACI }. Rule #6 Negative moment reinforcement must be anchored into or through supporting columns of members. {ACI 1.1.1} As above, we plan to continue the negative reinforcement into the next span, through the support, satisfying this rule. Rule #7 The same reasoning from cutoff #1 applies and this rule is satisfied. The cutoff rules are satisfied for negative cutoff #. Rule checking was made considerably easier because we are not cutting this bar in tension. Positive Cutoff #1 Rule #1 The buffer is plotted this rule is met. Rule # Bars must extend at least l d from the point of maximum bar stresses or from the point at which adjacent bars which are cut or bent are no longer required to resist flexure. {ACI 1.10., , 1.1.} The bar at cutoff #1 develops its full strength before maximum moment at midspan. This rule is satisfied. Rule #3 Bars cannot be cutoff in tension regions unless conditions in {ACI } are met. The #5 being cut is in tension so we must satisfy one of the conditions given in {ACI , , or }. {ACI }: Looking at the shear design at x 5.00 ft (the location of positive cutoff #1) 10

11 we are using s 7 in spacing so that φv n 47.6 kip, and V u V u (5.00 ft) 67.4 kip (6.03 kip/ft)(5.00 ft) 37.3 kip. V u φv n 37.3 kip 47.6 kip 0.78 > 3 (64) We do not satisfy this section. {ACI }: The required spacing over the last 0.75d of the bar being cut of the additional stirrups, s + is: 0.75d pos s + ( A v f y s + min (60 lb/in )b, d ) pos (65) 8β b ( 0. in (60, 000 lb/in ) ) 1.0 in min, in (66) 60 lb/in (9 in) 8(1/6) 0.75(1.0 in) in/stirrup 1.00 stirrup (67) where β b 1/6 since one #5 out of six are being cut. At the point of the cut we are using s 7 in spacing, so 0.75d pos s 0.75(1.0 in) 7 in in 7 in/stirrup.5 stirrups (68) That is, we have.5 stirrups from the initial design and we need to add an additional 1.00 stirrup for a total of 3.5 stirrups over in at the end of the cut bars. This works out to a spacing of in/3.5 stirrups 4.85 inch/stirrup. So, we will reduce our spacing to 4 inches near the end of the cut bar. {ACI }: In order to meet this criterion, we must meet three conditions: 1. No. 11 bars or smaller. We are cutting a #5, so we meet this.. Continuing reinforcement provides double the area required for flexure at the cutoff point. That is, φm n /M u at the cutoff point, where φm n is the moment capacity of the continuing bars. After positive cutoff #1 the moment capacity is φm n 138 kip ft, and reading from the graph, the moment demand, M u, is 96 kip-ft. φm n M u 138 kip ft 96 kip ft 1.53 < (69) Thus, this criterion is not met. 3. Factored shear does not exceed three fourths the design shear strength, φv n. That is, V u /φv n 3/4. Based on the results from Equation 64, this criterion is not met either. Overall, the stipulations of {ACI } are not met based on the moment capacity. The end result is that we will be adding extra stirrups near the end of the first cut bar as required by {ACI }. Rules #4 and #5 are based on conditions near the supports and will be checked for Positive Cutoff #. 11

12 Positive Cutoff # Rule #1 Satisfied by inspection. Rule # Bars must extend at least l d from the point of maximum bar stresses or from the point at which adjacent bars which are cut or bent are no longer required to resist flexure. {ACI 1.10., , 1.1.} The bar at cutoff #1 was adjacent to the bars being checked now. The bars from cutoff # reach their full strength before bars from cutoff #1 are needed, so this rule is satisfied. Rule #3 Bars cannot be cutoff in tension regions unless conditions in {ACI } are met. The edge of the buffer occurs at x 3.14 ft. If we cut here, it will be in a region of positive moment, thus we must meet one of the conditions of {ACI }. At the cutoff location, x 3.14 ft, we are using s 5 in spacing so that φv n 56.8 kip, and V u V u (3.14 ft) 67.4 kip (6.03 kip/ft)(3.14 ft) 48.5 kip. V u φv n 48.5 kip 56.8 kip 0.85 (70) The ratio in Equation 70 is greater than /3 and 3/4, so we cannot meet the provisions of {ACI } or {ACI }. We could add extra stirrups near the cutoff location as stipulated in {ACI }. However, we are cutting the bars near the positive P.I. so that by extending the cutoff a few inches (4.33 inches to be exact) towards the support we will not be cutting in tension. We elect to extend the bars and the rule is satisfied since we will no longer be cutting in tension. Rule #4 (a) Simple supports At least one-third of the positive moment reinforcement must extend six inches into the support. {ACI } (b) Continuous interior beams with closed stirrups At least one-fourth of the positive moment reinforcement must extend six inches into the support. {ACI , } (c) Continuous interior beams without closed stirrups At least one-fourth of the positive moment reinforcement must be continuous. {ACI , } (d) Continuous perimeter beams At least one-fourth of the positive moment reinforcement must be continuous around the perimeter of the building and enclosed within closed stirrups or stirrups with 135-degree hooks. {ACI } We are considering a continuous interior beam. One-half of the positive reinforcing (three of six bars) will be continuing through the support. Thus, whether the stirrups are closed or not, we meet this rule. Rule #5 At the positive moment point of inflection (P.I.), and at simple supports, the positive moment reinforcement must satisfy: l d qm n V u + l a (71) where V u is the factored shear at the P.I. or the support, for a P.I. l a is the larger of d or 1d b and is less than the actual embedment past the P.I, for a simple support l a is the end anchorage past the center of the support, and q is 1.3 if the ends of reinforcement are confined by compressive reaction (generally true for simple supports) and 1.0 otherwise. {ACI } The positive moment P.I. occurs at 0.146l n 0.146(19 ft).77 ft. Calculating the needed quantities at the P.I.: φm n 88 kip ft 88 kip ft 88 kip ft M n 97.8 kip ft φ 0.9 (7) V u 67.4 kip (6.03 kip/ft)(.77 ft) 50.7 kip (73) l a max(d pos, 1d b ) max(1.0 in, 1(0.65 in)) 1.0 in (74) 1

13 Because this is a P.I. (and not a support), q 1.0. The development length from cutoff #1 is l d 3.7 in so that qm n V u + l a (1.0)97.8 kip ft (1 in/foot) in 44.1 in > l d 3.7 in (75) 50.7 kip Rule #5 is satisfied and we are done with the flexural steel cutoff design. FINAL DESIGN As required by ACI : 7" 4" 10" Stirrup at Center 8" " Positive Cutoff ft 9in Negative Cutoff 4ft 7in Positive Cutoff 5ft 0in Negative Cutoff 6ft 0in CL x (feet) Figure 8: The final design. 13

14 SERVICEABILITY DEFLECTION (1) Would large deflections cause a problem? Yes they would (given). () Calculate I g, M cr, and I cr. I g bh3 1 9 in(4 in)3 1 10, 368 in 4 (76) M cr 1 6 f rbh , 000 lb/in (9 in)(4 in) (77) 409, 831 lb in 34. kip ft n E s 9, 000, 000 lb/in E c 57, (78) 4, 000 lb/in Note that Equation 77 is valid because this is a rectangular section. 1 Calculate I cr at the midspan (I cr,mid ) and support (I cr,sup ). At midspan, there are 6 #5 for the tensile steel (A s 1.86 in ) and #7 for the compressive steel (A s 1.0 in ). The distance from the top to the neutral axis, c, is found by solving the quadratic formula: bc + [na s + (n 1)A s] c na s d pos (n 1)A sd pos (79) (9 in)c + [ 8.04(1.86 in ) (1.0 in ) ] c 8.04(1.86 in )(1.0 in) 7.04(1.0 in )(.3 in) (80) 4.5c + 3.4c (81) Solving gives c 6.39 in. We can then solve for the cracked moment of inertia, I cr,mid. I cr,mid bc3 3 + (n 1)A s(c d pos) + na s (d pos c) (8) (9 in)(6.39 in) (1.0 in )(6.39 in.3 in) 3 (83) +8.04(1.86 in )(1.0 in 6.39 in) (84) 4116 in 4 At the support, there are five #7 bars for tensile steel at the top since moments are negative (A s 3.0 in ), the bottom has 3 #5 (A s 0.93 in ) and is in compression so that c neg is the distance from the bottom to the neutral axis. The distances to the steel, d neg and d neg are also measured from the bottom of the section. bc neg + [na s + (n 1)A s] c neg na s d neg (n 1)A sd neg (85) (9 in)c neg + [ 8.04(3.0 in ) (0.93 in ) ] c neg 8.04(3.0 in )(0.9 in) 7.04(0.93 in )(. in) (86) 4.5c neg c neg (87) Solving gives c neg 7.85 in which leads to I cr,sup bc3 neg 3 + (n 1)A s(c neg d neg) + na s (d neg c neg ) (88) (9 in)(7.85 in) (0.93 in )(7.85 in. in) 3 (89) +8.04(3.0 in )(0.9 in 7.85 in) (90) 5768 in 4 (3) Find I,D, I,D+L, I,L, I,SUST. 1 For other sections use the definition: M cr frig y t. 14

15 Deflection under Service Dead Loads Using the coefficients from {ACI 8.3.3} with service loads (w D DL): M D,mid w D l n/16 (.375 kip/ft)(19 ft) / kip ft (91) M D,sup w D l n/11 (.375 kip/ft)(19 ft) / kip ft (9) Both exceed the uncracked moment of inertia, M cr 34. kip ft, so that I e,mid I cr,mid + (I g I cr,mid ) ( Mcr M D,mid ) 3 (93) ( ) kip ft 4116 in 4 + (10, 368 in in 4 ) 5740 in 4 (94) 53.6 kip ft ( ) 3 Mcr I e,sup I cr,sup + (I g I cr,sup ) (95) M D,sup ( ) kip ft 5768 in 4 + (10, 368 in in 4 ) 6157 in kip ft (96) I e 0.70I e,mid I e,sup (97) 0.70(5740 in 4 ) (6157 in 4 ) 5865 in 4 An approximate formula for the deflection of a continuous beam is: 5wl4 n M A,supl n M B,supl n (98) 384E c I e 16E c I e 16E c I e where M A,sup and M B,sup are the moments at the supports at side A and B respectively, and E c is the modulus of elasticity for concrete: E c 57, 000 f c 57, 000 4, 000 lb/in (1 kip/1000 lb) 3605 kip/in (99) Thus, with M A,sup M B,sup M D,sup the immediate deflections from dead loads are: I,D 5w Dl 4 n 384E c I e M D,supl n 8E c I e (100) 5(.375 kip/ft)(19 ft)4 (1 in/foot) 3 384(3605 kip/in )(5865 in 4 ) (101) 77.9 kip ft(19 ft) (1 in/foot) 3 8(3605 kip/in )(5865 in 4 ) (10) I,D 0.04 in (103) Deflection under Service Dead + Live Loads The service distributed load is w D+L DL+LL.375 kip/ft+.65 kip/ft 5.05 kip/ft. M D+L,mid w D+L l n/16 (5.05 kip/ft)(19 ft) / kip ft (104) M D+L,sup w D+L l n/11 (5.05 kip/ft)(19 ft) / kip ft (105) 15

16 I e,mid I cr,mid + (I g I cr,mid ) ( Mcr M D+L,mid ) 3 (106) ( ) kip ft 4116 in 4 + (10, 368 in in 4 ) 489 in 4 (107) 113 kip ft ( ) 3 Mcr I e,sup I cr,sup + (I g I cr,sup ) (108) M D+L,sup ( ) kip ft 5768 in 4 + (10, 368 in in 4 ) 5809 in kip ft (109) I e 0.70I e,mid I e,sup (110) 0.70(489 in 4 ) (5809 in 4 ) 4745 in 4 We can then calculate the deflections due to dead + live and live only: I,D+L 5w D+Ll 4 n 384E c I e M D+L,supl n 8E c I e (111) 5(5.05 kip/ft)(19 ft)4 (1 in/foot) 3 384(3605 kip/in )(4745 in 4 ) (11) 165 kip ft(19 ft) (1 in/foot) 3 8(3605 kip/in )(4745 in 4 ) (113) in (114) I,L I,D+L I,D in 0.04 in in (115) Deflection under Sustained Loads Assume that 50% of the live load is sustained: M L,mid M D+L,mid M D,mid 113 kip ft 53.6 kip ft 59.4 kip ft (116) M SUST,mid M D,mid + 0.5M L,mid 53.6 kip ft + 0.5(59.4 kip ft) 83.3 kip ft (117) M L,sup M D+L,sup M D,sup 165 kip ft 77.9 kip ft 87.1 (118) M SUST,sup M D,sup + 0.5M L,sup 77.9 kip ft + 0.5(87.1 kip ft) 11 kip ft (119) Solving for the effective moments of inertia: I e,mid I cr,mid + (I g I cr,mid ) ( M cr M SUST,mid ) 3 (10) ( ) kip ft 4116 in 4 + (10, 368 in in 4 ) 4549 in 4 (11) 83.3 kip ft ( ) 3 M cr I e,sup I cr,sup + (I g I cr,sup ) (1) M SUST,sup ( ) kip ft 5768 in 4 + (10, 368 in in 4 ) 587 in 4 11 kip ft (13) I e 0.70I e,mid I e,sup (14) Solving for the deflection: 0.70(4549 in 4 ) (587 in 4 ) 4946 in 4 w SUST DL + 0.5LL.375 kip/ft + 0.5(.65 kip/ft) 3.70 kip/ft (15) 16

17 I,SUST 5w SUST l 4 n M SUST,supl n 384E c I e 8E c I e (16) 5(3.70 kip/ft)(19 ft)4 (1 in/foot) 3 384(3605 kip/in )(4946 in 4 ) (17) 11 kip ft(19 ft) (1 in/foot) 3 8(3605 kip/in )(4946 in 4 ) (18) I,SUST in (19) (4) Find long-term creep and shrinkage deflection, CS. As defined in the code, CS λ I,SUST Using a 5-year timespan (ξ.0) and ρ at the midspan: Substituting all values: CS ρ A s (0.60 in ) bd pos (9 in)(1.0 in) ξ ρ I,SUST (130) (131).0 (0.079 in) 0.10 in (13) ( ) (5) Check code requirements. The serviceability deflection, S, is given by S CS + I,L 0.10 in in in (133) Because large deflections could cause problems: S in l n 19 ft (1 in/foot) in (134) We meet the deflection requirement, the beam is adequately designed. SERVICEABILITY CRACK WIDTH To meet the requirements for crack width, the center-to-center spacing of the tension steel, s c c, must satisfy 540 kip/in s c c.5c c (135) f s At the midspan, we have 3 #5 bars and a #3 stirrup so that s c c is: 9 in (1.5 in) (0.375 in) 0.65 in s c c.31 in (136) With 1.5 inch clear cover, c c 1.5 in in in, and use f s 0.6f y 0.6(60 ksi) 36 ksi so that the equations to check are 540 kip/in s c c.31 in.5(1.875 in) 10.3 in (137) 36 kip/in ( ) ( ) 36 ksi 36 ksi s c c.31 in 1 in 1 in 1 in (138) 36 ksi This requirement is satisfied at the midspan. At supports there are three #7s in the tension zone so that f s 9 in (1.5 in) (0.375 in) in s c c.19 in (139) The quantities c c and f s are the same as at the midspan, and since s c c is actually smaller at the support, we know that the section at the support meets crack-width requirements. THE END 17

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

Problem Set 3: Solutions

Problem Set 3: Solutions CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C

Διαβάστε περισσότερα

Section 8.3 Trigonometric Equations

Section 8.3 Trigonometric Equations 99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.

Διαβάστε περισσότερα

Approximation of distance between locations on earth given by latitude and longitude

Approximation of distance between locations on earth given by latitude and longitude Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth

Διαβάστε περισσότερα

2 Composition. Invertible Mappings

2 Composition. Invertible Mappings Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,

Διαβάστε περισσότερα

Section 7.6 Double and Half Angle Formulas

Section 7.6 Double and Half Angle Formulas 09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)

Διαβάστε περισσότερα

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr 9.9 #. Area inside the oval limaçon r = + cos. To graph, start with = so r =. Compute d = sin. Interesting points are where d vanishes, or at =,,, etc. For these values of we compute r:,,, and the values

Διαβάστε περισσότερα

Math 6 SL Probability Distributions Practice Test Mark Scheme

Math 6 SL Probability Distributions Practice Test Mark Scheme Math 6 SL Probability Distributions Practice Test Mark Scheme. (a) Note: Award A for vertical line to right of mean, A for shading to right of their vertical line. AA N (b) evidence of recognizing symmetry

Διαβάστε περισσότερα

Homework 3 Solutions

Homework 3 Solutions Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For

Διαβάστε περισσότερα

Strain gauge and rosettes

Strain gauge and rosettes Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified

Διαβάστε περισσότερα

EE512: Error Control Coding

EE512: Error Control Coding EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3

Διαβάστε περισσότερα

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β 3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle

Διαβάστε περισσότερα

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required) Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts

Διαβάστε περισσότερα

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch: HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying

Διαβάστε περισσότερα

Finite Field Problems: Solutions

Finite Field Problems: Solutions Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The

Διαβάστε περισσότερα

Example Sheet 3 Solutions

Example Sheet 3 Solutions Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο

Διαβάστε περισσότερα

Section 9.2 Polar Equations and Graphs

Section 9.2 Polar Equations and Graphs 180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify

Διαβάστε περισσότερα

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3

Διαβάστε περισσότερα

derivation of the Laplacian from rectangular to spherical coordinates

derivation of the Laplacian from rectangular to spherical coordinates derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used

Διαβάστε περισσότερα

Solutions to Exercise Sheet 5

Solutions to Exercise Sheet 5 Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X

Διαβάστε περισσότερα

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1. Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given

Διαβάστε περισσότερα

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =? Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least

Διαβάστε περισσότερα

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- ----------------- Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin

Διαβάστε περισσότερα

Instruction Execution Times

Instruction Execution Times 1 C Execution Times InThisAppendix... Introduction DL330 Execution Times DL330P Execution Times DL340 Execution Times C-2 Execution Times Introduction Data Registers This appendix contains several tables

Διαβάστε περισσότερα

MECHANICAL PROPERTIES OF MATERIALS

MECHANICAL PROPERTIES OF MATERIALS MECHANICAL PROPERTIES OF MATERIALS! Simple Tension Test! The Stress-Strain Diagram! Stress-Strain Behavior of Ductile and Brittle Materials! Hooke s Law! Strain Energy! Poisson s Ratio! The Shear Stress-Strain

Διαβάστε περισσότερα

Math221: HW# 1 solutions

Math221: HW# 1 solutions Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin

Διαβάστε περισσότερα

The Simply Typed Lambda Calculus

The Simply Typed Lambda Calculus Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and

Διαβάστε περισσότερα

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ. Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action

Διαβάστε περισσότερα

Concrete Mathematics Exercises from 30 September 2016

Concrete Mathematics Exercises from 30 September 2016 Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)

Διαβάστε περισσότερα

PARTIAL NOTES for 6.1 Trigonometric Identities

PARTIAL NOTES for 6.1 Trigonometric Identities PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot

Διαβάστε περισσότερα

Homework 8 Model Solution Section

Homework 8 Model Solution Section MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx

Διαβάστε περισσότερα

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013 Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering

Διαβάστε περισσότερα

( y) Partial Differential Equations

( y) Partial Differential Equations Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate

Διαβάστε περισσότερα

Solution to Review Problems for Midterm III

Solution to Review Problems for Midterm III Solution to Review Problems for Mierm III Mierm III: Friday, November 19 in class Topics:.8-.11, 4.1,4. 1. Find the derivative of the following functions and simplify your answers. (a) x(ln(4x)) +ln(5

Διαβάστε περισσότερα

( ) 2 and compare to M.

( ) 2 and compare to M. Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8

Διαβάστε περισσότερα

C.S. 430 Assignment 6, Sample Solutions

C.S. 430 Assignment 6, Sample Solutions C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order

Διαβάστε περισσότερα

5.0 DESIGN CALCULATIONS

5.0 DESIGN CALCULATIONS 5.0 DESIGN CALCULATIONS Load Data Reference Drawing No. 2-87-010-80926 Foundation loading for steel chimney 1-00-281-53214 Boiler foundation plan sketch : Figure 1 Quantity Unit Dia of Stack, d 6.00 m

Διαβάστε περισσότερα

CHAPTER 12: PERIMETER, AREA, CIRCUMFERENCE, AND 12.1 INTRODUCTION TO GEOMETRIC 12.2 PERIMETER: SQUARES, RECTANGLES,

CHAPTER 12: PERIMETER, AREA, CIRCUMFERENCE, AND 12.1 INTRODUCTION TO GEOMETRIC 12.2 PERIMETER: SQUARES, RECTANGLES, CHAPTER : PERIMETER, AREA, CIRCUMFERENCE, AND SIGNED FRACTIONS. INTRODUCTION TO GEOMETRIC MEASUREMENTS p. -3. PERIMETER: SQUARES, RECTANGLES, TRIANGLES p. 4-5.3 AREA: SQUARES, RECTANGLES, TRIANGLES p.

Διαβάστε περισσότερα

Other Test Constructions: Likelihood Ratio & Bayes Tests

Other Test Constructions: Likelihood Ratio & Bayes Tests Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :

Διαβάστε περισσότερα

6.3 Forecasting ARMA processes

6.3 Forecasting ARMA processes 122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear

Διαβάστε περισσότερα

1 String with massive end-points

1 String with massive end-points 1 String with massive end-points Πρόβλημα 5.11:Θεωρείστε μια χορδή μήκους, τάσης T, με δύο σημειακά σωματίδια στα άκρα της, το ένα μάζας m, και το άλλο μάζας m. α) Μελετώντας την κίνηση των άκρων βρείτε

Διαβάστε περισσότερα

Matrices and Determinants

Matrices and Determinants Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z

Διαβάστε περισσότερα

10.7 Performance of Second-Order System (Unit Step Response)

10.7 Performance of Second-Order System (Unit Step Response) Lecture Notes on Control Systems/D. Ghose/0 57 0.7 Performance of Second-Order System (Unit Step Response) Consider the second order system a ÿ + a ẏ + a 0 y = b 0 r So, Y (s) R(s) = b 0 a s + a s + a

Διαβάστε περισσότερα

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds! MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.

Διαβάστε περισσότερα

Second Order RLC Filters

Second Order RLC Filters ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor

Διαβάστε περισσότερα

Chapter 7 Transformations of Stress and Strain

Chapter 7 Transformations of Stress and Strain Chapter 7 Transformations of Stress and Strain INTRODUCTION Transformation of Plane Stress Mohr s Circle for Plane Stress Application of Mohr s Circle to 3D Analsis 90 60 60 0 0 50 90 Introduction 7-1

Διαβάστε περισσότερα

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0. DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec

Διαβάστε περισσότερα

Srednicki Chapter 55

Srednicki Chapter 55 Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third

Διαβάστε περισσότερα

Μηχανική Μάθηση Hypothesis Testing

Μηχανική Μάθηση Hypothesis Testing ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Μηχανική Μάθηση Hypothesis Testing Γιώργος Μπορμπουδάκης Τμήμα Επιστήμης Υπολογιστών Procedure 1. Form the null (H 0 ) and alternative (H 1 ) hypothesis 2. Consider

Διαβάστε περισσότερα

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits. EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα είναι μικρότεροι το 1000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Διάρκεια: 3,5 ώρες Καλή

Διαβάστε περισσότερα

4.6 Autoregressive Moving Average Model ARMA(1,1)

4.6 Autoregressive Moving Average Model ARMA(1,1) 84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this

Διαβάστε περισσότερα

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is Pg. 9. The perimeter is P = The area of a triangle is A = bh where b is the base, h is the height 0 h= btan 60 = b = b In our case b =, then the area is A = = 0. By Pythagorean theorem a + a = d a a =

Διαβάστε περισσότερα

Second Order Partial Differential Equations

Second Order Partial Differential Equations Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y

Διαβάστε περισσότερα

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that

Διαβάστε περισσότερα

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R + Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b

Διαβάστε περισσότερα

Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Review Test MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Find the exact value of the expression. 1) sin - 11π 1 1) + - + - - ) sin 11π 1 ) ( -

Διαβάστε περισσότερα

Surface Mount Multilayer Chip Capacitors for Commodity Solutions

Surface Mount Multilayer Chip Capacitors for Commodity Solutions Surface Mount Multilayer Chip Capacitors for Commodity Solutions Below tables are test procedures and requirements unless specified in detail datasheet. 1) Visual and mechanical 2) Capacitance 3) Q/DF

Διαβάστε περισσότερα

CRASH COURSE IN PRECALCULUS

CRASH COURSE IN PRECALCULUS CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter

Διαβάστε περισσότερα

Αναερόβια Φυσική Κατάσταση

Αναερόβια Φυσική Κατάσταση Αναερόβια Φυσική Κατάσταση Γιάννης Κουτεντάκης, BSc, MA. PhD Αναπληρωτής Καθηγητής ΤΕΦΑΑ, Πανεπιστήµιο Θεσσαλίας Περιεχόµενο Μαθήµατος Ορισµός της αναερόβιας φυσικής κατάστασης Σχέσης µε µηχανισµούς παραγωγής

Διαβάστε περισσότερα

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1 Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the

Διαβάστε περισσότερα

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8  questions or comments to Dan Fetter 1 Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test

Διαβάστε περισσότερα

D Alembert s Solution to the Wave Equation

D Alembert s Solution to the Wave Equation D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique

Διαβάστε περισσότερα

the total number of electrons passing through the lamp.

the total number of electrons passing through the lamp. 1. A 12 V 36 W lamp is lit to normal brightness using a 12 V car battery of negligible internal resistance. The lamp is switched on for one hour (3600 s). For the time of 1 hour, calculate (i) the energy

Διαβάστε περισσότερα

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD CHAPTER FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD EXERCISE 36 Page 66. Determine the Fourier series for the periodic function: f(x), when x +, when x which is periodic outside this rge of period.

Διαβάστε περισσότερα

1) Formulation of the Problem as a Linear Programming Model

1) Formulation of the Problem as a Linear Programming Model 1) Formulation of the Problem as a Linear Programming Model Let xi = the amount of money invested in each of the potential investments in, where (i=1,2, ) x1 = the amount of money invested in Savings Account

Διαβάστε περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)

Διαβάστε περισσότερα

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

6.1. Dirac Equation. Hamiltonian. Dirac Eq. 6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2

Διαβάστε περισσότερα

Figure A.2: MPC and MPCP Age Profiles (estimating ρ, ρ = 2, φ = 0.03)..

Figure A.2: MPC and MPCP Age Profiles (estimating ρ, ρ = 2, φ = 0.03).. Supplemental Material (not for publication) Persistent vs. Permanent Income Shocks in the Buffer-Stock Model Jeppe Druedahl Thomas H. Jørgensen May, A Additional Figures and Tables Figure A.: Wealth and

Διαβάστε περισσότερα

[1] P Q. Fig. 3.1

[1] P Q. Fig. 3.1 1 (a) Define resistance....... [1] (b) The smallest conductor within a computer processing chip can be represented as a rectangular block that is one atom high, four atoms wide and twenty atoms long. One

Διαβάστε περισσότερα

Every set of first-order formulas is equivalent to an independent set

Every set of first-order formulas is equivalent to an independent set Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent

Διαβάστε περισσότερα

Συστήματα Διαχείρισης Βάσεων Δεδομένων

Συστήματα Διαχείρισης Βάσεων Δεδομένων ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Συστήματα Διαχείρισης Βάσεων Δεδομένων Φροντιστήριο 9: Transactions - part 1 Δημήτρης Πλεξουσάκης Τμήμα Επιστήμης Υπολογιστών Tutorial on Undo, Redo and Undo/Redo

Διαβάστε περισσότερα

Potential Dividers. 46 minutes. 46 marks. Page 1 of 11

Potential Dividers. 46 minutes. 46 marks. Page 1 of 11 Potential Dividers 46 minutes 46 marks Page 1 of 11 Q1. In the circuit shown in the figure below, the battery, of negligible internal resistance, has an emf of 30 V. The pd across the lamp is 6.0 V and

Διαβάστε περισσότερα

ST5224: Advanced Statistical Theory II

ST5224: Advanced Statistical Theory II ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known

Διαβάστε περισσότερα

Partial Differential Equations in Biology The boundary element method. March 26, 2013

Partial Differential Equations in Biology The boundary element method. March 26, 2013 The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet

Διαβάστε περισσότερα

5.4 The Poisson Distribution.

5.4 The Poisson Distribution. The worst thing you can do about a situation is nothing. Sr. O Shea Jackson 5.4 The Poisson Distribution. Description of the Poisson Distribution Discrete probability distribution. The random variable

Διαβάστε περισσότερα

Right Rear Door. Let's now finish the door hinge saga with the right rear door

Right Rear Door. Let's now finish the door hinge saga with the right rear door Right Rear Door Let's now finish the door hinge saga with the right rear door You may have been already guessed my steps, so there is not much to describe in detail. Old upper one file:///c /Documents

Διαβάστε περισσότερα

Macromechanics of a Laminate. Textbook: Mechanics of Composite Materials Author: Autar Kaw

Macromechanics of a Laminate. Textbook: Mechanics of Composite Materials Author: Autar Kaw Macromechanics of a Laminate Tetboo: Mechanics of Composite Materials Author: Autar Kaw Figure 4.1 Fiber Direction θ z CHAPTER OJECTIVES Understand the code for laminate stacing sequence Develop relationships

Διαβάστε περισσότερα

Cross sectional area, square inches or square millimeters

Cross sectional area, square inches or square millimeters Symbols A E Cross sectional area, square inches or square millimeters of Elasticity, 29,000 kips per square inch or 200 000 Newtons per square millimeter (N/mm 2 ) I Moment of inertia (X & Y axis), inches

Διαβάστε περισσότερα

TMA4115 Matematikk 3

TMA4115 Matematikk 3 TMA4115 Matematikk 3 Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet Trondheim Spring 2010 Lecture 12: Mathematics Marvellous Matrices Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet

Διαβάστε περισσότερα

Dr. D. Dinev, Department of Structural Mechanics, UACEG

Dr. D. Dinev, Department of Structural Mechanics, UACEG Lecture 4 Material behavior: Constitutive equations Field of the game Print version Lecture on Theory of lasticity and Plasticity of Dr. D. Dinev, Department of Structural Mechanics, UACG 4.1 Contents

Διαβάστε περισσότερα

Jackson 2.25 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Jackson 2.25 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell Jackson 2.25 Hoework Proble Solution Dr. Christopher S. Baird University of Massachusetts Lowell PROBLEM: Two conducting planes at zero potential eet along the z axis, aking an angle β between the, as

Διαβάστε περισσότερα

The challenges of non-stable predicates

The challenges of non-stable predicates The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates

Διαβάστε περισσότερα

Tridiagonal matrices. Gérard MEURANT. October, 2008

Tridiagonal matrices. Gérard MEURANT. October, 2008 Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,

Διαβάστε περισσότερα

ΕΛΕΓΧΟΣ ΤΩΝ ΠΑΡΑΜΟΡΦΩΣΕΩΝ ΧΑΛΥΒ ΙΝΩΝ ΦΟΡΕΩΝ ΜΕΓΑΛΟΥ ΑΝΟΙΓΜΑΤΟΣ ΤΥΠΟΥ MBSN ΜΕ ΤΗ ΧΡΗΣΗ ΚΑΛΩ ΙΩΝ: ΠΡΟΤΑΣΗ ΕΦΑΡΜΟΓΗΣ ΣΕ ΑΝΟΙΚΤΟ ΣΤΕΓΑΣΤΡΟ

ΕΛΕΓΧΟΣ ΤΩΝ ΠΑΡΑΜΟΡΦΩΣΕΩΝ ΧΑΛΥΒ ΙΝΩΝ ΦΟΡΕΩΝ ΜΕΓΑΛΟΥ ΑΝΟΙΓΜΑΤΟΣ ΤΥΠΟΥ MBSN ΜΕ ΤΗ ΧΡΗΣΗ ΚΑΛΩ ΙΩΝ: ΠΡΟΤΑΣΗ ΕΦΑΡΜΟΓΗΣ ΣΕ ΑΝΟΙΚΤΟ ΣΤΕΓΑΣΤΡΟ ΕΛΕΓΧΟΣ ΤΩΝ ΠΑΡΑΜΟΡΦΩΣΕΩΝ ΧΑΛΥΒ ΙΝΩΝ ΦΟΡΕΩΝ ΜΕΓΑΛΟΥ ΑΝΟΙΓΜΑΤΟΣ ΤΥΠΟΥ MBSN ΜΕ ΤΗ ΧΡΗΣΗ ΚΑΛΩ ΙΩΝ: ΠΡΟΤΑΣΗ ΕΦΑΡΜΟΓΗΣ ΣΕ ΑΝΟΙΚΤΟ ΣΤΕΓΑΣΤΡΟ Νικόλαος Αντωνίου Πολιτικός Μηχανικός Τµήµα Πολιτικών Μηχανικών, Α.Π.Θ.,

Διαβάστε περισσότερα

Fractional Colorings and Zykov Products of graphs

Fractional Colorings and Zykov Products of graphs Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is

Διαβάστε περισσότερα

STRUCTURAL CALCULATIONS FOR SUSPENDED BUS SYSTEM SEISMIC SUPPORTS SEISMIC SUPPORT GUIDELINES

STRUCTURAL CALCULATIONS FOR SUSPENDED BUS SYSTEM SEISMIC SUPPORTS SEISMIC SUPPORT GUIDELINES Customer: PDI, 4200 Oakleys Court, Richmond, VA 23223 Date: 5/31/2017 A. PALMA e n g i n e e r i n g Tag: Seismic Restraint Suspended Bus System Supports Building Code: 2012 IBC/2013 CBC&ASCE7-10 STRUCTURAL

Διαβάστε περισσότερα

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset

Διαβάστε περισσότερα

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We

Διαβάστε περισσότερα

Numerical Analysis FMN011

Numerical Analysis FMN011 Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =

Διαβάστε περισσότερα

Reminders: linear functions

Reminders: linear functions Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U

Διαβάστε περισσότερα

Structural Design of Raft Foundation

Structural Design of Raft Foundation QATAR UNIVERSITY COLLAGE OF ENGINEERING COURSE: DESIGN OF REINFORCED CONCRETE STRUCTURES Structural Design of Raft Foundation Submitted to: Dr. Mohammed Al-ansari Prepared by: Haytham Adnan Sadeq Mohammed

Διαβάστε περισσότερα

Volume of a Cuboid. Volume = length x breadth x height. V = l x b x h. The formula for the volume of a cuboid is

Volume of a Cuboid. Volume = length x breadth x height. V = l x b x h. The formula for the volume of a cuboid is Volume of a Cuboid The formula for the volume of a cuboid is Volume = length x breadth x height V = l x b x h Example Work out the volume of this cuboid 10 cm 15 cm V = l x b x h V = 15 x 6 x 10 V = 900cm³

Διαβάστε περισσότερα

D28 1-1/4" PIPE x 42-1/2" HIGH RAIL WITHOUT BOTTOM RAIL

D28 1-1/4 PIPE x 42-1/2 HIGH RAIL WITHOUT BOTTOM RAIL Ultra-tec Cable Railing Systems G-D28 D28 1-1/4" PIPE x 42-1/2" HIGH RAIL WITHOUT BOTTOM RAIL Building Code: Material: 2006 International Building Code 2007 California Building Code AISC Steel Construction

Διαβάστε περισσότερα

Stresses in a Plane. Mohr s Circle. Cross Section thru Body. MET 210W Mohr s Circle 1. Some parts experience normal stresses in

Stresses in a Plane. Mohr s Circle. Cross Section thru Body. MET 210W Mohr s Circle 1. Some parts experience normal stresses in ME 10W E. Evans Stresses in a Plane Some parts eperience normal stresses in two directions. hese tpes of problems are called Plane Stress or Biaial Stress Cross Section thru Bod z angent and normal to

Διαβάστε περισσότερα

department listing department name αχχουντσ ϕανε βαλικτ δδσϕηασδδη σδηφγ ασκϕηλκ τεχηνιχαλ αλαν ϕουν διξ τεχηνιχαλ ϕοην µαριανι

department listing department name αχχουντσ ϕανε βαλικτ δδσϕηασδδη σδηφγ ασκϕηλκ τεχηνιχαλ αλαν ϕουν διξ τεχηνιχαλ ϕοην µαριανι She selects the option. Jenny starts with the al listing. This has employees listed within She drills down through the employee. The inferred ER sttricture relates this to the redcords in the databasee

Διαβάστε περισσότερα

Code Breaker. TEACHER s NOTES

Code Breaker. TEACHER s NOTES TEACHER s NOTES Time: 50 minutes Learning Outcomes: To relate the genetic code to the assembly of proteins To summarize factors that lead to different types of mutations To distinguish among positive,

Διαβάστε περισσότερα