Approximate analysis of the frame and wall type structures
    On the basis of the method of §6.4.3, perform the approximate analysis of both the frame and the wall type structures of the two previous paragraphs.
    Frame type structure    (§6.4.1)
    The building height is H=6 × 3.0=18.0 m.
    The structure is classified as frame system in both directions, therefore Ct,x=Ct,y=Ct=0.075 The structure is    also regular in both plan and elevation, thus q=3.60. (The accurate value is 3.90, but for the comparability of the results we use the    same value as in §6.4.1).
    T1,x= T1,y=    Τ    1    =Ct     ×     H3/4=0.075     ×     18.03/4=0.7 sec
    Since 0.50=TC≤0.70=T1<2.0=TD (see §6.1.6),
    Sd(T1)=max[    γ    I    ·     agR     ·     S     ·     (    2.5/q)     ·     (    Tc/T1),     β     ·     γ    I     ·             agR]=        
        =max(1.0         × 0.15 × 1.2 × (2.5/3.6) × (0.50/0.70), 0.2 × 1.0 × 0.15)     ·             g=0.089g.        
    Since T1=0.70≤1.0=2TC  →  λ=0.85, thus aCM=    λ · Sd(T1)=0.85 × 0.089g=0.076g
The mass of each floor is M=177.4 t except from the mass of the last floor which is M6=166.9 t, therefore Σ    (Mi)=166.9+5 × 177.4=1053.9 t.
    The elevation of the centre of mass is    
    ZCM=    Σ    (Mj     ·     Z    j    )/    Σ    (Mj)= =(177.4 ×     3.0+    177.4 ×     6.0+    177.4 ×     9.0+    177.4 ×     12.0+    177.4 ×     15.0+    166.9 ×     18.0)/1053.9 =10987.2/1053.9      →  ZCM=10.4 m
    The triangular distribution gives the accelerations by means of the expression
    aj=(Zj/ZCM)     ·     aCM    =(0.076g/10.4)     ·     Zj     →  aj=0.0073g × Zj
    a1=0.0073g     × 3.0=    0.022g, a2=0.044g, a3=0.066g, a4=0.088g, a5=0.110g, a6=0.131g
    H1=a1     ·     M1=    0.023     ·     10m/sec2     ·     177.4     ·     103kg=39 kN, H2=78, H3=117, H4=156, H5=195     και     H6=0.131     ·     10m/sec2     ·     166.9     ·     103kg =219 kN    .
    According to the application of the modal response spectrum analysis carried-out in §6.4.2, the average fundamental natural period of the structure,    in the various cases, is equal to T1x=T1y=1.0 sec taking into account a stiffness reduction factor equal to 0.50 due to cracking of    structural elements, while T1x=T1y=0.65 sec taking into account full stiffnesses. It therefore follows that the value range of the    fundamental natural period of the structure is quite wide depending on its type, e.g. cross-sectional dimensions, foundation type, etc., as well as on the    assumption of the stiffnesses reduction due to cracking.
		    Wall type structure    (§6.4.2)
    The building height is H=6 × 3.0=18.0 m.
    The structure is classified as wall system in both directions, thus Ct,x=Ct,y=Ct=0.050. The structure is also    regular in both plan and elevation, thus q=3.60.
    T1,x= T1,y=    Τ    1    =Ct     ·     H3/4=0.050     ×     18.03/4=0.44 sec
    Since 0.15=TB≤0.44=T1<0.50=TC (see §6.1.6)    
    Sd(T1)=    γ    I     ·     agR     ·     S     ·     (    2.5/q)=1.0     × 0.15 × 1.2 × 2.5/3.6= 0.125g.
Since T1=0.44≤1.00=2TC  →  λ=0.85, thus aCM=    λ × Sd(T1)=0.85 × 0.125g=0.10625g
The mass of each floor is M=186.3 t, except from the mass of the last floor which is M6=165.0 t, therefore Σ    (Mi)=165.0+5 × 186.3=1096.5 t.
    The elevation of the centre of mass is
    ZCM    =Σ(    Mj     ·     Z    j    )/Σ(    Mj    )= =(186.3 ·     3.0+    186.3 ·     6.0+    186.3 ·     9.0+    186.3 ·     12.0+    186.3 ·     15.0+    165.0 ·     18.0)/1096.5=11353.5/1096.5      →  ZCM=10.4 m
    The triangular distribution gives the accelerations by means of the expression
    aj=(Zj/ZCM)     ·     aCM    =(0.10625g/10.4)     ·     Zj     →  aj=0.0102g · Zj
    which yields a1=0.031g, a2=0.061g, a3=0.092g, a4=0.122g, a5=0.153g, a6=0.184g and seismic forces H1=a1 · M1=0.031 · 10m/sec2 · 186.3 · 103kg=58 kN, H2=114, H3=171, H4=227, H5=285 andH6=0.184     · 10m/sec2 · 165 · 103kg =304 kN.
    According to the application of the modal response spectrum analysis carried-out in §6.4.2, the average fundamental natural period of the structure,    in the various cases, is equal to T1x=T1y=0.7 sec taking into account a stiffness reduction factor equal to 0.50 due to cracking of    structural elements, while T1x=T1y=0.5 sec taking into account full stiffnesses. It therefore follows that the value range of the    fundamental natural period of the structure is quite wide depending on its type, e.g. cross-sectional dimensions, foundation type, etc., as well as on the    assumption of the stiffnesses reduction due to cracking.
    a)     The value of the approximate calculation of the     fundamental    natural            period and the design seismic acceleration lies in checking the correctness of the corresponding quantities derived from the algorithms of the modal        response spectrum analysis.    
    In the related software, the fundamental natural period is obtained from the modal response spectrum analysis and is shown as a red arrow in the seismic    acceleration graph at the elevation of the centre of mass.
    b)             The value of the approximate method for the triangular distribution of seismic accelerations consists in the evaluation of the accelerations obtained        by the algorithms of the modal response spectrum analysis, which should follow the triangular distribution to some extent.    
    In the related software, the triangular distribution is shown using a red dashed line.