RSPEC

Bulk Data Entry Specifies directional combination method, modal combination method, excitation direction(s), response spectra and scale factors for Response Spectrum Analysis.

Format

(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
RSPEC RID DCOMB MCOMB CLOSE MMASS RIGRESP
DTISPEC1 SCALE1 X11 X12 X13 ZPA1 FA1 FB1
DTISPEC2 SCALE2 X21 X22 X23 ZPA2 FA2 FB2
DTISPEC3 SCALE3 X31 X32 X33 ZPA3 FA2 FB2

Example 1

(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
RSPEC 35 ALG SRSS 1.0
7 1.3 0.5 0.5 -1.

Example 2

(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
RSPEC 35 SRSS CQC 0.0
7 1.3 0.5 0.5 -1.
4 2.0 -2 -0.0 -1.
2 17. 0.5 -2.5 -1.

Definitions

Field Contents SI Unit Example
RID RSPEC identification number. Must be unique.

No default (Integer > 0)

DCOMB Directional combination method.
ALG (Default)
Algebraic.
SRSS
Square root of sum of squares.
MCOMB Modal combination method.
ABS (Default)
Absolute sum.
SRSS
Square root of sum of squares. 2
CQC
Complete quadratic combination.
NRL
Navy Research Laboratory's SRSS.
CLOSE Modal frequency closeness parameter. 2

Default = 1.0 (Real ≥ 1.0)

MMASS Keyword indicating missing mass response is used.

Default = blank

RIGRESP Keyword specifying which rigid response method is applied.
GUPTA
Gupta rigid response method is applied.
LINDLEY
Lindley-Yow rigid response method is applied.

Default = blank

DTISPECi Response spectrum reference. Identification number of the DTI,SPECSEL entry.

No default (Integer > 0)

SCALEi Scale factor for excitation.

No default (Real <> 0.0)

Xij Components of a vector representing ground excitation i, j = 1..3
ZPAi Zero Period Acceleration value. 4

No default (Real ≥ 0.0)

FAi, FBi Frequency limits indicating a pure periodic response or a pure rigid response. 4

No default (Real ≥ 0.0, FBiFAi)

Comments

  1. DTISPEC2/SCALE2/X21/X22/X23 and DTISPEC3/SCALE3/X31/X32/X33 are optional ground excitations for multi-directional excitation. The directions of excitation have to be orthogonal to each other and will be reported as error otherwise.
  2. When MCOMB = SRSS or NRL, natural frequencies that are close will be summed by the ABS method. The close frequencies are determined using the inequality.
    F ( i + 1 ) < C L O S E * F ( i ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOraiaacI cacaWGPbGaey4kaSIaaGymaiaacMcacqGH8aapcaWGdbGaamitaiaa d+eacaWGtbGaamyraiaacQcacaWGgbGaaiikaiaadMgacaGGPaaaaa@4378@

    Where, F ( i ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOraiaacI cacaWGPbGaaiykaaaa@3908@ and F ( i + 1 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOraiaacI cacaWGPbGaey4kaSIaaGymaiaacMcaaaa@3AA5@ are successive natural frequencies.

    Then, they are combined with other modal contributions in accordance with the specified MCOMB option. Since natural frequencies are in ascending order, CLOSE values should be greater than or equal to 1.0.

  3. Response spectra values are defined as a table of frequencies in the X axis and the response spectra in the Y axis in a TABLED1 entry referenced by the DTI,SPECSEL entry. For any modes extracted during the response spectrum analysis that lie within or outside the range of the frequencies defined by the TABLED1 entry, linear interpolation or extrapolation is carried out to determine the corresponding spectral values associated with such modes.
  4. ZPAi must be defined for missing mass response or rigid response with Lindley-Yow Method. Missing mass response can be used together with both rigid response methods.

    When RIGRESP option is active, the response is divided into periodic part and rigid part in modal combinations. A variable α is introduced as the ratio of the rigid part to the modal response of mode i, hence providing an estimate of the proportion of rigid part of the response.

    Rigid part:

    R r i = α i R i MathType@MTEF@5@5@+= feaahGart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape GaamOua8aadaWgaaWcbaWdbiaadkhacaWGPbaapaqabaGcpeGaeyyp a0JaeqySde2damaaBaaaleaapeGaamyAaaWdaeqaaOWdbiaadkfapa WaaSbaaSqaa8qacaWGPbaapaqabaaaaa@3F63@

    Periodic part:

    R p i = 1 α i 2 R i MathType@MTEF@5@5@+= feaahGart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape GaamOua8aadaWgaaWcbaWdbiaadchacaWGPbaapaqabaGcpeGaeyyp a0ZaaOaaa8aabaWdbiaaigdacqGHsislcqaHXoqypaWaa0baaSqaa8 qacaWGPbaapaqaa8qacaaIYaaaaaqabaGccaWGsbWdamaaBaaaleaa peGaamyAaaWdaeqaaaaa@41F5@

    Gupta method calculates α based on the frequency. When the frequency is less than FA, it is pure periodic response, so α = 0; When the frequency is greater than FB, it is pure rigid response, so α = 1; When the frequency is between FA and FB, a value [0,1] is adopted for α in the transition range.

    Lindley-Yow method calculates α based on the acceleration response spectrum value. When the spectrum value is equal to ZPA, it is pure rigid response, so α = 1; When the spectrum value is less than ZPA it is pure periodic response, so α = 0; When the spectrum value is greater than ZPA, a value [0,1] is adopted for α in the transition range. It is optional to define FA in Lindley-Yow method, and α is 0 as long as the frequency is less than FA.
    ZPA FA FB
    MMASS Required
    GUPTA Required Required
    LINDLEY Required Optional
  5. Refer to Response Spectrum Analysis in the User Guide for more details.