As we know One Pa·s is equal to 1 daP (1 Pa·s = 1 daP).
To convert Pascal Second to Dekapoise, multiply your Pa·s figure by 1.
Example : convert 25 Pa·s to daP:
25 Pa·s = 25 × 1 daP = daP
To convert Dekapoise to Pascal Second, divide your daP figure by 1.
Example : convert 25 daP to Pa·s:
25 daP = 25 ÷ 1 Pa·s = Pa·s
As we know One daP is equal to 1 Pa·s (1 daP = 1 Pa·s).
To convert Dekapoise to Pascal Second, multiply your daP figure by 1.
Example : convert 45 daP to Pa·s:
45 daP = 45 × 1 Pa·s = Pa·s
To convert Pascal Second to Dekapoise, divide your Pa·s figure by 1.
Example : convert 45 Pa·s to daP:
45 Pa·s = 45 ÷ 1 daP = daP
Pa·s to kgf·s/m² | 1 Pa·s = 0.1019716213 kgf·s/m² |
Pa·s to N·s/m² | 1 Pa·s = 1 N·s/m² |
Pa·s to mN·s/m² | 1 Pa·s = 1000 mN·s/m² |
Pa·s to dyn·s/cm² | 1 Pa·s = 10 dyn·s/cm² |
Pa·s to P | 1 Pa·s = 10 P |
Pa·s to EP | 1 Pa·s = 1.E-17 EP |
Pa·s to PP | 1 Pa·s = 1.E-14 PP |
Pa·s to TP | 1 Pa·s = 1.E-11 TP |
Pa·s to GP | 1 Pa·s = 1.E-8 GP |
Pa·s to MP | 1 Pa·s = 0.00001 MP |
Pa·s to kP | 1 Pa·s = 0.01 kP |
Pa·s to hP | 1 Pa·s = 0.1 hP |
Pa·s to daP | 1 Pa·s = 1 daP |
Pa·s to dP | 1 Pa·s = 100 dP |
Pa·s to cP | 1 Pa·s = 1000 cP |
Pa·s to mP | 1 Pa·s = 10000 mP |
Pa·s to µP | 1 Pa·s = 10000000 µP |
Pa·s to nP | 1 Pa·s = 10000000000 nP |
Pa·s to pP | 1 Pa·s = 10000000000000 pP |
Pa·s to fP | 1 Pa·s = 10000000000000000 fP |
Pa·s to aP | 1 Pa·s = 10000000000000000000 aP |
Pa·s to lbf·s/in² | 1 Pa·s = 0.0001450377 lbf·s/in² |
Pa·s to lbf·s/ft² | 1 Pa·s = 0.0208854342 lbf·s/ft² |
Pa·s to pdl·s/ft² | 1 Pa·s = 0.6719689751 pdl·s/ft² |
Pa·s to g/(cm·s) | 1 Pa·s = 10 g/(cm·s) |
Pa·s to slug/(ft·s) | 1 Pa·s = 0.0208854342 slug/(ft·s) |
Pa·s to lb/(ft·s) | 1 Pa·s = 0.6719689751 lb/(ft·s) |
Pa·s to lb/(ft·h) | 1 Pa·s = 2419.0883105 lb/(ft·h) |
Created @ o.vg | Free Unit Converters |
daP. Since one Pa·s equals 1 daP, 9 Pa·s in daP will be daP.
There are 1 daP in one Pa·s. In turn, one daP is equal to 1 Pa·s.
1 daP is approximately equal to 1 Pa·s.
The Pascal Second value of 8 daP is Pa·s. (i.e.,) 8 x 1 = Pa·s.
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