Table 1.
+Ca2+ (activating solution, pCa 4.73) | −Ca2+ (relaxing solution) | |||
---|---|---|---|---|
Velocity μm/s | Force pN/μm | Velocity μm/s | Force pN/μm | |
−Tm | 4.68±0.09 (15)** | 1.07±0.06 (38)** | ||
Δ2Tm | 5.71±0.09 (29)** | 0.48±0.04 (58)** | 0.26±0.05 (4) | 0 |
Δ3Tm | 4.90±0.29 (9)** | 0.37±0.03 (74)** | 0.36±0.03 (10) | 0 |
Δ6Tm | 6.26±0.13 (22)** | 1.52±0.16 (48) | 6.47±0.12 (9)** | 0.66±0.05 (47)** |
wtTm | 7.70±0.07 (16) | 1.63±0.06 (101) | 0.33±0.02 (10) | 0 |
P2sTm | 6.73±0.19 (10)** | 1.46±0.08 (55)(*) | 0.32±0.02 (10) | 0 |
P3sTm | 6.92±0.14 (12)** | 1.53±0.09 (56) | 0.39±0.02 (10) | 0 |
P2P3sTm | 9.27±0.18 (11)** | 2.11±0.12 (85)** | 0.33±0.02 (10) | 0 |
P1P5Tm | 6.92±0.23 (18)** | 2.06±0.12 (66)** | 5.41±0.22 (8)** | 0.28±0.03 (32)** |
For velocity measurements, velocity distribution such as shown in Fig. 1 was deduced from a video record consisting of 3 sec, and then the distribution was fitted to Eq. 1 to find Vc. Vc was then averaged for many records, and shown with ±SEM in this Table. For force measurements, the filament-attached beads are trapped by optical tweezers, the thin filaments and HMM interaction was performed, then force was measured (Fig. 2), histogram (Fig. 3) was created, and averaged. 0: force was not detectable. Experiments were performed in the presence of 2 mM MgATP at 24°C. In comparison, the velocity measured in the rigor solution (no ATP, no Ca) was 0.40±0.01 (N=6) for wtTm, and 0.45±0.04 (N=4) in the absence of Tm and Tn; Force was not detectable.
P≤0.01,
0.01<P≤0.05, and
0.05<P≤0.1 compared to wtTm (based on paired T-tests).