Understanding the concepts on Degrees of Freedom
1)A five storey structure with 5 translational DOF is shown here. Each storey has mass ‘m’. The eigenvalue problem has been solved and the 5 periods of vibration Tn and their corresponding mode shapes, φn has been derived.

The fundamental period of vibration (T1 = 2 seconds) and its associated mode shape:

The second mode of vibration (T2 = 0.6852 seconds) and its associated mode shape:

The third mode of vibration (T3 = 0.4346 seconds) and its associated mode shape:

The fourth mode of vibration (T4 = 0.3383 seconds) and its associated mode shape:

The fifth mode of vibration (T4 = 0.2966 seconds) and its associated mode shape:

- Ln , Mn and Γn for each of the five modes are to be computed from Equations below.
- Also, calculate the effective modal mass Mn* and the modal mass participating ratio for the 5 modes. The mass matrix will be required to evaluate these parameters.

- Finally, obtain the base shear for each of the 5 modes of vibration and the combined base shear as per SRSS rule. The pseudo acceleration design spectrum to obtain the base shear for each mode is provided below.

- How many modes are to be considered such that a modal mass participating ratio of 90% is obtained?

AIM:
To compute Ln , Mn and Γn for each of the five modes from the given equations.
To calculate the effective modal mass Mn* and the modal mass participating ratio for the 5 modes.
To obtain the base shear for each of the 5 modes of vibration and the combined base shear as per SRSS rule.
SOLUTION:
Mass matrix(m)=`[[m,0,0,0,0],[0,m,0,0,0],[0,0,m,0,0],[0,0,0,m,0],[0,0,0,0,m]]`
Modified mass matrix(M)=``phi_(n)^T.m.phi_n`
`[0.334,0.641,0.895,1.078,1.173]``[[m,0,0,0,0],[0,m,0,0,0],[0,0,m,0,0],[0,0,0,m,0],[0,0,0,0,m]]`` `[[0.334],[0.641],[0.895],[1.078],[1.173]]`
`M_1`=3.861
Model property(L)=``phi_(n)^T.m.L
Where L =influence vector (Assuming 100% utilization of seismic force)=`[[1],[1],[1],[1],[1]]`
For the first mode (n=1)=`[0.334,0.641,0.895,1.078,1.173]``[[m,0,0,0,0],[0,m,0,0,0],[0,0,m,0,0],[0,0,0,m,0],[0,0,0,0,m]]``[[1],[1],[1],[1],[1]]`
`L_1=`4.121m
Modal participation factor(`(Gamma)=L/M`
For the first mode ,`Gamma=L_1/M_1`
`nbsp; `Gamma_1=4.121/3.381m`
`Gamma_1=1.067`
Similarly,`Gamma_2=0,335`
`nbsp; `Gamma_3=0.177`
`Gamma_4=-0.098`
`Gamma_5=0.045`
Effective modal mass(`(M^(*))=L_n^2/M_n`
`nbsp; For the first mode,`M_1^*=L_1^2/M_1`
(n=1)
`M_1^*=4.398`
Similarly,`M_2^*=0.436m`
`M_3^*=0.121m`
`M_4^*=0.038m`
`M_5^*=0.08m`
Modal mass participation ratio=`M_n^*/m_j`
Where ,`M_j=`Total mass of the building
=m+m+m+m+m
=5m
Modal masss participation of first mode(n=1)=4.398m/5m=0.88
Similarly,second mode (n=2)=0.09
Third mode (n=3)=0.02
Fourth mode (n=4)=0.01
Fifth mode(n=5)=0.002
Adding first two mode mass participation ratios
We get 0.88+0.09=0.97
To achieve minimum 90% of modal mass participation ratio,first two modes are enough
Base shear `(V_B)=M_n^*.A_n`
For the first mode,`V_B1=4.398m*0.27g`
(n=1)
`V_B1=1.187mg`
Similarly , `V_B2=0.327mg`
`V_B3=0.126mg`
`V_B4=0.039mg`
`V_B5=0.008mg`
Average Base shear is calculated by the method of square root of sum of square
`sqrt(V_b1^2)+(V_b2^2)+(V_b3^2)+(V_b4^2)+(V_b5^2)`
`V_B=1.15mg`
RESULT:
Adding first two mode mass participation ratios
We get 0.88+0.09=0.97
Base shear
`V_B=1.15mg`